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1994 Part 3 |
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Front Cover (1994 - Part
3) No author information
available
Summary: Not
available |
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Table of Contents (1994 - Part
3) No author information
available
Summary: Not
available |
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Superconducting
cueing receiver for space
experiment T.C.L.G. Sollner, W.G.
Lyons, D.R. Arsenault, A.C. Anderson, M.M. Seaver, R.R.
Boisvert and R.L. Slattery
Summary:
Exploiting the high-temperature superconductor YBa/sub
2/Cu/sub 3/O/sub 7-x/ (YBCO), we have extended chirp-transform
processing to instantaneously analyze the spectrum of an
incoming signal over greater bandwidth than any competing
technology. A compact receiver has been developed that can
analyze a 3 GHz bandwidth in 120 ns with 110 MHz resolution.
The cryogenic YBCO chirp filter and ambient-temperature
semiconductor electronics have been space qualified for flight
on the US Navy's High-Temperature Superconductivity Space
Experiment, a package to be launched on the US Air Force ARGOS
scientific satellite. |
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Design
and performance of low-noise hybrid
superconductor/semiconductor 7.4 GHz receiver
downconverter J.B. Barner, J.J.
Bautista, J.G. Bowen, W. Chew, M.C. Foote, B.H. Fujiwara, A.J.
Guern, B.J. Hunt, H.H.S. Javadi, G.G. Ortiz, D.L. Rascoe, R.P.
Vasquez, P.D. Wamhof, K.B. Bhasin, R.F. Leonard, R.R.
Romanofsky and C.M. Chorey
Summary: Low noise
receivers play critical role in space applications. Thin film
high-critical-temperature-superconducting (HTS) passive
circuits were combined with GaAs microwave devices to achieve
ultra low noise and small size receiver downconverter at 77 K.
HTS pre-select filter, a cryogenic mixer, and a hybrid
oscillator with an HTS resonator were designed, fabricated and
interconnected to produce a low-noise hybrid
superconductor/semiconductor 7.4 GHz microwave receiver. When
cooled to 77 K, the downconverter plus cables inside a
cryogenic refrigerator had a noise figure of approximately 0.7
dB with conversion gain of 18 dB. In addition to reduce noise
figure, advantages of small size and low power consumption are
observed due to the use of HTS circuits in the
downconverter. |
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High-temperature
superconducting four-channel
filterbanks S.H. Talisa, M.A.
Janocko, D.L. Meier, C. Moskowitz, R.L. Grassel, J.
Talvacchio, P. LePage, G. Hira, D.C. Buck, S.J. Pieseski, J.C.
Brown and G.R. Wagner
Summary: A
high-temperature superconducting four-channel filterbank was
fabricated and tested. The device was made in microstrip
configuration with an architecture that included two
branch-line hybrids and two identical parallel-coupled line
filters per channel. The filterbank was fully integrated, with
microstrip interconnections between channels and thin-film
load terminations in the out-of-phase port of the output
hybrid. |
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YBCO/ferrite
low-loss microwave phase
shifter G.F. Dionne, D.E. Oates
and D.H. Temme
Summary: Microstrip-geometry
phase shifters have limited use at microwave frequencies
because of high insertion losses resulting from resistance in
the metal conductors. We report a phase shifter fabricated
from a YBa/sub 2/Cu/sub 3/O/sub 7-x/ microstrip line on
LaAlO/sub 3/ coupled to a ferrite toroid. The magnetic flux
required for gyromagnetic interaction with the microwave
signal is contained within the closed magnetic path of the
ferrite toroid so that the superconductor encounters a very
low external magnetic field. Initial measurements at 77 K
using a meanderline structure to provide nonreciprocal
operation have demonstrated greater than 700 deg of
differential phase shift at 10 GHz in a compact structure 2.5
cm long by 0.5 cm wide. The insertion loss is smaller than 0.7
dB which yields a figure of merit considerably greater than
1000 deg/dB. The best conventional phase shifters have an
estimated figure of merit of 300 deg/dB at 77 K. Potential
radar system applications and improvements in the figure of
merit are discussed. |
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YBCO
step edge junctions on various
substrates C.L. Pettiette-Hall,
J.A. Luine, J. Murduck, J.F. Burch, R. Hu, M. Sergant and D.
St. John
Summary: We have fabricated YBCO
90/spl deg/ grain boundary junctions on step edges in
NdGaO/sub 3/ and in deposited dielectric (CeO/sub 2/ on YSZ
and SrTiO/sub 3/ on MgO) in order to compare junction
performance to our standard, LaAlO/sub 3/. Average I/sub
c/R/sub n/ values at 77 K in the 300-400 /spl mu/V range were
measured for 2 /spl mu/m step edge junctions on NdGaO/sub 3/,
LaAlO/sub 3/, and SrTiO/sub 3//MgO. Junction I/sub c/ is
greatly reduced with the CeO/sub 2//YSZ system. I/sub c/R/sub
n/ values in the 300-400 /spl mu/V range were measured at 65 K
for 4 /spl mu/m junctions. |
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Proximity
effect in edge type junctions with PrBa/sub 2/Cu/sub 3/O/sub
7/ barriers prepared by Br-ethanol
etching M.I. Faley, U. Poppe,
C.L. Jia, K. Urban and Y. Xu
Summary:
Multilayer Josephson edge type junctions were prepared
on the edges of c-axis oriented YBa/sub 2/Cu/sub 3/O/sub 7/
thin films structured by chemical etching in a Br-ethanol
solution. Resistive PrBa/sub 2/Cu/sub 3-x/Ga/sub x/O/sub 7/
(x=0, 0.15, and 0.3) films were deposited by the high oxygen
pressure dc-sputtering technique and used for barrier and
insulation layers. Basic properties of the junctions such as
I/sub c/(T), I/sub c/(d), R/sub n/(T), and basic
characteristics of the proximity effect such as /spl xi//sub
n/, /spl gamma/ and /spl gamma//sub B/ were obtained and
discussed. |
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Ramp
type HTS Josephson junctions with PrBaCuGaO
barriers M.A.J. Verhoeven, G.J.
Gerritsma, H. Rogalla and A.A. Golubov
Summary:
Ramp type Josephson junctions have been fabricated
using DyBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// as electrode
material and PrBa/sub 2/Cu/sub 3-x/Ga/sub x/O/sub 7-/spl
delta// with x=0, 0.10 and 0.40 as junction barriers. Barrier
thickness lie between 6-30 nm. Several junctions without
barrier were made in order to find ways to minimize the damage
of the ramp interface. In total about 40 chips were fabricated
each containing several junctions and their I-V
characteristics measured for various temperatures down to 4.2
K. Only those junctions showing clear RSJ-like curves were
selected to be analyzed. In some cases we also measured I/sub
c/ as a function of a small applied field and obtained a clear
Fraunhofer pattern, but there is a tendency to flux trapping
as evidenced by LTSEM. It was found at 4.2 K that the critical
current density J/sub c/ scales with the specific resistance
R/sub n/A as J/sub c/=C/sub bar/(R/sub n/A)/sup -m/ (m=1.8/spl
plusmn/0.5). The barrier material dependent constant C/sub
bar/ increases with x, whereas, for a given d, J/sub c/ is
constant and R/sub n/A increases. |
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Transport
properties of YBCO/PBCO/YBCO
junctions Y. Sawada, H. Terai, A.
Fujimaki, Y. Takai and H. Hayakawa
Summary:
We studied on the transport properties of edge-type
YBCO/PBCO/YBCO junctions. They showed clear Josephson
characteristics with I/sub c/R/sub n/ products of a few mV.
The experimental results revealed that normal-state
characteristics were dominated by the tunneling via localized
states. Besides, taking account of constant I/sub c/R/sub n/
products, we could consider the transport mechanism of
supercurrent as the resonant tunneling. |
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Fabrication
and characterization of high temperature superconductor
Josephson junctions with a novel device
design Q.X. Jia, X.D. Wu, S.R.
Foltyn, D. Reagor, M. Hawley, K.N. Springer, P. Tiwari, C.
Mombourquette, R.J. Houlton, I.H. Campbell, H. Kung, T.E.
Mitchell and D.E. Peterson
Summary: A unique
normal-metal (N) layer construction was used to fabricate high
temperature superconducting (S) YBa/sub 2/Cu/sub 3/O/sub
7-/spl delta// SNS Josephson junctions. The normal-metal
included a gradient Pr-doped Y/sub 1-x/Pr/sub x/Ba/sub
2/Cu/sub 3/O/sub 7-/spl delta// layer which was composed of a
light doping (x=0.1) next to both YBa/sub 2/Cu/sub 3/O/sub
7-/spl delta// electrodes, a slightly higher doping (x=0.3)
towards the center, and a doping concentration of x=0.5 in the
middle of the N-layer. A gradient of the doping profile of the
N-layer instead of an abrupt one provides good thermal,
structural, and chemical compatibility between adjacent
regions. The multilayer configuration of the gradient Pr-doped
N-layers on YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// showed
good growth structure as confirmed by X-ray diffraction and
Rutherford backscattering channeling tests. The SNS junctions
fabricated in such a way showed resistively shunted junction
current vs voltage characteristics above 77 K. Microwave
induced Shapiro steps above 77 K and voltage modulation of dc
SQUIDs at 77 K were both demonstrated with this
technology. |
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Properties
of YBaCuO thin film single-level dc SQUIDs fabricated using
step-edge junctions J.Z. Sun,
L.S. Yu-Jahnes, V. Foglietti, R.H. Koch and W.J.
Gallagher
Summary: A quantitative comparison
study of single-level step-edge junction-based SQUIDs and
bicrystal-substrate-based SQUIDs is given. Similar SQUID
performance was found in terms of white flux noise level and
junction-critical-current-related 1/f noise. Excess current
was found in most step-edge devices. Issues related to systems
applications, such as magnetic field-induced noise, junction
cyclability upon repeated use, and environmental stability of
oxide-metal contacts are also discussed. |
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The
PTB 83-SQUID system for biomagnetic applications in a
clinic D.
Drung
Summary: The PTB 83-SQUID
(superconducting quantum interference device) system is
described which is operated in a clinical environment.
Integrated dc SQUID magnetometers with additional positive
feedback (APF) are used in order to realize electronic first-
or second-order gradiometer configurations. The dewar for the
system has a flat bottom. It allows the detection of vertical
(B/sub z/) and horizontal (B/sub x,y/) field components: 49
sensors (plus 14 reference magnetometers) are sensitive for
B/sub z/ and 14 sensors (plus 6 reference magnetometers) for
B/sub x,y/. The system is installed inside a standard shielded
room (Vakuumschmelze type AK3b) in the Klinikum Benjamin
Franklin, Steglitz, Berlin. A typical white noise level of 2.5
fT//spl radic/(Hz) has been measured in the first-order
gradiometer mode. Due to the very low system noise level it
became possible for the first time to detect the extremely
weak neuromagnetic fields (5-10 fT peak amplitude) generated
by the nerve roots deep in the lower back which are evoked by
electrical nerve stimulation at the foot (200 Hz system
bandwidth, 8000 responses averaged). |
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Noise
cancellation by a whole-cortex SQUID MEG
system J. Vrba, B. Taylor, T.
Cheung, A.A. Fife, G. Haid, P.R. Kubik, S. Lee, J. McCubbin
and M.B. Burbank
Summary: We report on the
noise cancellation performance of several whole-cortex MEG
systems operated under diverse noise conditions, ranging from
unshielded environments to moderately shielded rooms. The
noise cancellation is performed by means of spatial filtering
using high order gradiometers (2nd or 3rd), which can be
formed optionally either by SQUID electronics firmware or by
software. The spatial dependence of the gradiometer responses
was measured in an unshielded environment and compared with
simulations to yield an estimate of the system common mode
magnitudes relative to field, 1st, and 2nd gradients. High
order gradiometers were also formed when the system was
operated in moderately shielded rooms. The combination of the
spatial filtering and room shielding resulted in very high
combined noise rejections approaching that of high quality
shielded rooms. Examples of noise cancellation under various
conditions are shown. |
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Superconducting
magnetic sensors operating from a moving
platform T.R.
Clem
Summary: Sensors incorporating
Superconducting Quantum Interference Devices (SQUIDs) provide
the greatest sensitivity for magnetic anomaly detection
available with current technology, The Coastal Systems Station
(CSS) has pioneered the use of superconducting magnetic
sensors in the field operating onboard airborne and undersea
moving platforms, where environmental and instrument noises
present operational problems which are not encountered under
laboratory conditions. Basic conceptual approaches for
utilizing these sensors onboard moving platforms, including
field deployable sensor configurations, are described.
Environmental and instrumental technical issues are also
addressed. A historical sketch of sensor development, current
sensor capabilities, recent technology advances, and future
trends is included. Naval applications and dual use
opportunities for this technology are given based on
experience developed at CSS. |
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An
experimental digital SQUID with large dynamic range and low
noise Perng-Fei Yuh and S.V.
Rylov
Summary: A digital SQUID chip designed
for large dynamic range and intrinsic sensitivity as good as
an analog SQUID was fabricated and tested. It consists of a
pickup coil, a SQUID amplifier, edge-triggered latching
comparators, and a feedback loop using an integrating
single-flux-quantum D/A converter. Proper operation of the
chip was demonstrated, with the output one-bit data stream
averaged and integrated to reconstruct the input signal. A
sampling rate up to 500 MHz was achieved. |
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Design
and performance aspects of pickup loop structures for
miniature SQUID magnetometry M.B.
Ketchen and J.R. Kirtley
Summary: As
miniature SQUID susceptometers and scanning SQUID microscopes
come into wider use, it is important to understand in detail
the magnetic coupling of objects of interest to small
superconducting pickup loops as well as our ability to scale
such pickup loop structures to sub-/spl mu/m dimensions. In
this paper we address important aspects of both of these
issues. First, assuming a perfect circular pickup loop, we
examine the coupling to three-dimensional objects and arrive
at a number of simple practical results for measurements on
small samples with various geometries and positions. Second,
we examine the nature of small superconducting pickup loop
structures and the impact on scaling of factors such as
connecting leads, local groundplanes and the superconducting
penetration depth. We conclude that highly localized pickup
areas of well under 1 /spl mu/m/sup 2/ are possible with
existing technology. |
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High-frequency
magnetic microscopy using a high-T/sub c/
SQUID R.C. Black, F.C. Wellstood,
E. Dantsker, A.H. Miklich, D. Koelle, F. Ludwig and J.
Clarke
Summary: We have used a
liquid-nitrogen-cooled scanning SQUID microscope to obtain
magnetic images at frequencies ranging from zero to 200 GHz,
that is, from audio frequencies through the radio frequency
band and into the millimeter microwave band. We present images
of thin film and bulk metallic samples, with a spatial
resolution of about 30 /spl mu/m, taken using various readout
schemes we have developed. |
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An
integrated digital SQUID magnetometer with high sensitivity
input M. Radparvar and S.
Rylov
Summary: A single chip SQUID
magnetometer is described that integrates a SQUID-based
pre-amplifier with a high sensitivity comparator gate and
feedback circuitries on the same chip. The comparator gate is
an asymmetric SQUID gate driving two SQUID quantizers in
series with the feedback coil. The chip's sensitivity and
noise level are primarily determined by the pre-amplifier
SQUID. The pick up coil is in series with the feedback
transformer. Since the current in the feedback coil is
maintained close to zero, the dynamic range of the chip can be
extremely wide and is independent of the SQUID pre-amplifier
or comparator architectures. The chip's slew rate is
determined by the bipolar clock biasing the comparator gate.
Clocks running in the tens of MHz result in a magnetometer
system with slew rate exceeding 10/sup 5/ /spl Phi//sub 0//s
(/spl Phi//sub 0/=2.07/spl times/10/sup -7/ Gauss-cm/sup 2/).
This chip simplifies room temperature electronics and, due to
its digital output, can be easily multiplexed on-chip. A
system based on this chip can be operated in a relatively high
magnetic field environment without extensive magnetic
shielding. The details of the chip as well as preliminary
measurement results for the pre-amplifier as well as the
digital circuit will be presented. |
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DC-SQUID
electronics based on the noise cancellation
scheme M. Kiviranta and H.
Seppa
Summary: We have constructed a compact
dc SQUID electronics unit, in which the noise of the
room-temperature amplifier is measured by the SQUID and
cancelled out. This makes it unnecessary to use a transformer
and a modulation scheme to achieve noise matching between the
SQUID and the amplifier. The electronics unit contains a
PI/sup 3/2/-controller and it has demonstrated a bandwidth of
100 kHz, a 1.2 /spl mu//spl Phi//sub 0///spl radic/(Hz) white
noise level and a 1/f noise corner of 0.3 Hz in a flux-locked
loop mode. The design criteria for the noise-cancelled
electronics are discussed, including the problem of excess
noise. |
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Portable
DC SQUID based magnetic susceptibility
meter V.V. Khanin, J.N.
Sotnikova, V.Y. Slobodchikov and A.N.
Matlashov
Summary: The device is designed as
a top-loading system for operation in a storage helium dewar
with a 1 1/4" dia neck. Sample temperature is regulated in the
range of 4.2-300 K using gaseous helium fed from a helium
bath. The sample diameter is up to 4.0 mm, the maximum
magnetizing field 0.18 T, the magnetic moment resolution 5/spl
times/10/sup -12/ A/spl times/m/sup 2/. The high sensitivity
of the instrument makes it possible to investigate the
magnetic susceptibility of 1 mm/spl times/1 mm HTc thin films
as a function of temperature in a transverse magnetic field of
about 10/sup -3/ T. The provisions for measuring the
magnetizing field with the help of a Hall sensor enable
samples to be cooled down in the fields below 10/sup -5/ T to
measure the Meisner effect. |
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Application
of high performance DC SQUIDs in precision measurement
technique W. Vodel, H. Koch, P.
Seidel, K. Bluthner and P. Weber
Summary: In
this review the performance of a DC SQUID system with
Nb-NbO/sub x/-Pb/In/Au window-type Josephson junctions is
described. The SQUIDs and the SQUID control units were
developed for universal applications in precision measurement
technique. Under optimum conditions a flux noise level of
2/spl times/10/sup -6/ /spl Phi//sub 0///spl radic/Hz was
achieved corresponding to an energy resolution of 3/spl
times/10/sup -31/ J/Hz. The contribution gives the design of
the DC SQUID device and summarizes recent results of its
application in precision measurement technique. The
applications include a cryogenic current comparator for
non-destructive measurement of the beam intensity produced in
a particle accelerator, a high-sensitive SQUID voltmeter for
investigations of the low-field Hall coefficient of high
purity metals, the upgrade of a multichannel RF SQUID
neuromagnetometer for biomagnetic research, and a planned
high-precision experiment in fundamental
physics. |
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3-channel
double relaxation oscillation SQUID magnetometer system with
simple readout electronics Y.H.
Lee, J.M. Kim, H.C. Kwon, Y.K. Park, J.C. Park, M.J. van
Duuren, D.J. Adelerhof, J. Flokstra and H.
Rogalla
Summary: Recently several approaches
have been made to simplify the readout scheme of the standard
dc SQUID. A double relaxation oscillation SQUID(DROS)
consisting of a hysteretic dc SQUID and a reference junction
in series shunted by an inductor and a resistor can provide a
very large flux-to-voltage transfer coefficient. Thus, a DROS
with direct readout with room temperature dc amplifier can be
a good candidate for the next-generation SQUID magnetometer.
We report on the development of a 3-channel magnetometer
system based on DROS. The DROS is based on Nb/AlO/sub X//Nb
Josephson junctions and the main feature of the system is its
simple readout electronics. |
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High
sensitivity magnetic flux sensors with direct voltage readout:
double relaxation oscillation
SQUIDs D.J. Adelerhof, M.J. van
Duuren, J. Flokstra, H. Rogalla, J. Kawai and H.
Kado
Summary: The experimental sensitivity of
double relaxation oscillation SQUIDs (DROSs) has been compared
with theory and with the results obtained by numerical
simulations. The experimental sensitivity ranges from 60 to
13h, where h is Planck's constant, for relaxation frequencies
from 0.4 up to 10 GHz. For low frequencies the DROS
characteristics can be explained by thermal noise on the
critical currents. For high frequencies, the voltage-flux
characteristics and the sensitivity are limited by the plasma
frequency. The cross-over frequency is at 2 GHz, which is
about 2% of the plasma frequency of the DROSs. |
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Theoretical
analysis of a relaxation oscillation
SQUID M. Morisue, M. Yamadaya, A.
Kanasugi and G. Uehara
Summary: Describes the
theoretical analysis of oscillation modes produced in a
relaxation oscillation SQUID (ROS). It is made clear what kind
of oscillation modes are produced in ROS in relation to
circuit parameters of the SQUID from the viewpoint of
relaxation oscillation. Emphasis is placed on mapping of
oscillation modes to design the ROS. Furthermore, the effect
of mutual inductance between the load impedance and SQUID to
the oscillation frequency is analyzed. |
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Washer
designs for SQUIDs with several junctions in a parallel
array M.E. Huber, A.T. Champion
and M.W. Gleason
Summary: We report on washer
designs for superconducting quantum interference devices
(SQUIDs) which include more than two Josephson junctions in a
parallel array, and on calculations of the operating
characteristics of such devices in the resistively-shunted
junction model. Coupling of the operating current to the
multi-junction device suppresses the voltage biased at
constant current. The coupling decreases as the ratio of the
mutual inductance between adjacent loops to the self
inductance of a single loop approaches 0.5. In various washer
designs, however, the practical limit for the ratio is no
greater than about 0.4. At this value, the simulations
indicate that significant reductions in voltage modulation
occur for even a small number of junctions. Also, the flux
responsivity increases with the number of junctions only
slightly more rapidly than does the total loop area, so the
sensitivity to a current in a coupling coil is nearly the same
as that of a single-loop device. This trend may ultimately
limit the usefulness of these devices. |
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Optimization
of a dc SQUID magnetometer to minimize the field
resolution K. Suzuki and Y.
Okabe
Summary: The circuit parameters of a dc
SQUID magnetometer have been optimized by computer
simulations. Our principle of optimization is to minimize the
field resolution. We have optimized the circuit parameters of
a dc SQUID magnetometer, such as a Ketchen type, Drung type,
directly-coupled type, etc. The only noise source was thermal
noise from the shunt resistors. For a Ketchen type SQUID, our
results show that the inductance of the input coil should be
larger than that reported previously. It is also the case for
a Drung type SQUID that the inductance of the SQUID washer
coil should be slightly increased. By this design method, the
optimum field resolution of a Ketchen type SQUID magnetometer
is improved by a factor of 2/3. Furthermore, we compared the
resolution of 3 types of dc SQUIDs and concluded that the
optimum type of SQUID depends on the value of the critical
current and the radius of the pick-up coil. Finally, we have
proposed a new design method that can optimize the field
resolution of dc SQUIDs under constraints on the critical
current and the spatial resolution. |
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Investigation
of YBa/sub 2/Cu/sub 3/O/sub 7/ Josephson junctions on MgO
bicrystal substrates L.
Vonderbeck, C.A. Copetti, A.M. Klushin, G. Kunkel, M. Siegel,
E. Sodtke, J. Schubert and W. Zander
Summary:
We report on the characterization of the dynamic (ac)
properties of YBa/sub 2/Cu/sub 3/O/sub 7/ Josephson junctions
on MgO bicrystal substrates with 24/spl deg/ angle. Shapiro
steps have been measured in the frequency range 80-95 GHz.
Measured current-voltage characteristics, as well as the
dependence of Shapiro step height on microwave power, were
compared to numerical simulations within the RSJ model
including thermal noise. At 77 K, the junctions showed ideal
RSJ behavior. The occurrence of half-integer Shapiro steps at
lower temperatures could be explained by an inhomogeneous
critical current density of the junctions yielding a dc
SQUID-like behavior. A nonsinusoidal current-phase relation
could be ruled out because of the periodicity of the
half-integer steps. |
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Fabrication
of biepitaxial YBCO Josephson junctions on different
substrates K. Petersen, C.
Stolzel, M. Schmitt, C. Krimmer, W. Wilkens, J. Sollner, H.W.
Grueninger and H. Adrian
Summary: Biepitaxial
Josephson junctions were fabricated on MgO and SrTiO/sub 3/
(STO) substrates. Electrical characteristics such as the
critical current densities J/sub c/, contact resistivities
/spl rho//sub n/ and I/sub c/R/sub n/-products on both
substrates are investigated. Junctions on MgO substrates are
stable against thermal cycling in contrast to many junctions
on STO substrates. The obtained current-voltage
characteristics and Shapiro step oscillations are in agreement
with the RSJ-model. The resistive transitions are strongly
broadened. DC-SQUIDs patterned on both substrates show
modulations dV/d/spl Phi/ at 77 K. At 55 K the energy
resolution /spl epsi/ in the range of white noise lies within
a factor of two of the theoretical limit. |
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Critical
current density distribution and magnetic flux states in
YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// bicrystal grain
boundary Josephson junctions G.M.
Fischer, B. Mayer, H. Schulze and R. Gross
Summary:
We have studied the spatial homogeneity of the critical
current density J/sub c/ and static magnetic flux states in
YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// bicrystal grain
boundary Josephson junctions (GBJs) using Low Temperature
Scanning Electron Microscopy (LTSEM). By LTSEM the J/sub c/
distribution and the static magnetic flux states in the GBJs
could be imaged with a resolution of less than 1 /spl mu/m.
Varying the applied magnetic field B the different magnetic
flux states with up to more than 15 vortices in the GBJ could
be observed. The spatial variation of the measured LTSEM
voltage signal agrees well with the theoretically expected
signal according to the sinusoidal modulation of the maximum
Josephson current density by an external magnetic field. The
LTSEM analysis clearly demonstrates that the spatial variation
of J/sub c/ along the grain boundary is less than about 30% on
the length scale of the spatial resolution of the LTSEM
technique. |
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Supercurrent
density correlation function of YBa/sub 2/Cu/sub 3/O/sub
7-/spl delta// grain boundary Josephson
junctions O.M. Froehlich, H.
Schulze, A. Beck, R. Gerdemann, B. Mayer, R. Gross and R.P.
Huebener
Summary: We have measured the
thermal noise induced slope R/sub p/(B) of the current-voltage
characteristics of YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
Grain Boundary Josephson Junctions (GBJs) for I/spl rarr/0 in
magnetic fields up to B=12 T. From the measured R/sub p/(B)
dependences the magnetic field dependence of the critical
current I/sub c/(B) was derived in the large magnetic field
range between 0 and 12 T. Finally, the supercurrent density
correlation function was obtained from the I/sub c/(B)
dependence using the Wiener-Khinchine relation. By introducing
the concept of the bright (BGCF) and dark ground correlation
function (DGCF) a spatial filtering of the information on the
supercurrent density distribution was obtained. The
investigation of the BGCFs and the comparison to DGCFs gives
clear evidence that supercurrent density has strong
inhomogeneities on small length scales in the nanometer
regime. |
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Fabrication
and superconducting transport properties of bicrystal grain
boundary Josephson junctions on different
substrates A. Beck, A. Stenzel,
O.M. Froehlich, R. Gerber, R. Gerdemann, L. Alff, B. Mayer, R.
Gross, A. Marx, J.C. Villegier and H.
Moriceau
Summary: We have reproducibly
fabricated YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// (YBCO)
grain boundary Josephson junctions (GBJs) on SrTiO/sub 3/ and
MgO bicrystals as well as by introducing buffer layers between
the c-axis oriented YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
film and the SrTiO/sub 3/ bicrystal substrate. For the
additional layers non-superconducting Nd/sub 1.85/Ce/sub
0.15/CuO/sub x/ (NCCO) and NdGaO/sub 3/ were used. The effect
of the layer structure on the superconducting transport
properties of the GBJs was analyzed by measuring the
current-voltage characteristics (IVCs), their derivatives, the
resistive transition R(T), and the magnetic field dependence
of the critical current I/sub c/(B). YBCO-GBJs fabricated on
MgO and SrTiO/sub 3/ bicrystal substrates were found to have
very similar low frequency characteristics. Fiske resonances
were investigated to obtain information on the high-frequency
properties. The Swihart velocity was found to be considerably
smaller for GBJs fabricated on SrTiO/sub 3/ as compared to MgO
due to the large relative dielectric constant of SrTiO/sub 3/
and the related stray capacitance. |
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Microwave-enhanced
superconductivity and transport properties of Y-Ba-Cu-O
bicrystal weak-links C.M. Fu,
J.Y. Juang, M.F. Chen, K.H. Wu, T.M. Uen and Y.S.
Gou
Summary: The effects of the tilt angle on
microwave-enhanced transition temperatures and critical
currents of YBCO bicrystal weak-links have been investigated.
It was found that, with smaller grain boundary tilt angles
(e.g. 24/spl deg/), the enhancement was small, displaying
essentially the same behavior as that manifested in
intragranular regions. By contrast, when the tilt angle was
increased from 36.8/spl deg/ to 45/spl deg/, noticeable Tc
enhancement was found to occur even at low input microwave
powers. The results were compared to the temperature dependent
critical current, in order to delineate possible correlations
between the two physical parameters. |
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Parallel
plate resonators in YBa/sub 2/Cu/sub 3/O/sub 7/ bicrystal
grain boundaries Y.M. Zhang, D.
Winkler, G. Brorsson and T. Claeson
Summary:
Intrinsic properties, such as the London penetration
depth /spl lambda//sub L/, and the surface resistance R/sub
s/, can be estimated in high-T/sub c/ films by studying
self-induced electromagnetic resonances (Fiske modes) in
bicrystal grain boundaries. Grain boundaries, 4-30 /spl mu/m
long and 0.2 /spl mu/m thick in YBa/sub 2/Cu/sub 3/O/sub 7/
made on yttria-stabilized zirconia 0-32/spl deg/ [001]-tilt
bicrystals were investigated. Typical values obtained for /spl
lambda//sub L/ and R/sub s/ (at approximately 200-400 GHz) are
110-170 nm, and 20-710 m /spl Omega/,
respectively. |
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Effect
of the misorientation angle on the magnetic properties of YBCO
grain boundary Josephson
junctions T. Ogawa and T.
Yamashita
Summary: We have studied magnetic
properties of YBa/sub 2/Cu/sub 3/O/sub x/ grain boundary
Josephson junctions (GBJJs) fabricated on SrTiO/sub 3/
bicrystal substrates to investigate whether the Josephson
characteristics change or not owing to the variation of the
misorientation angle. When the misorientation angle was
36.8/spl deg/, the total current was periodically suppressed
by the applied field; the current component was almost
Josephson current. On the contrary, for the GBJJs (/spl
theta/=24/spl deg/), the n-th minima (n/spl ges/2) in the
Ic(B) patterns did not occur at zero; a constant non-Josephson
current (bulky supercurrent) contribution to the patterns was
present. The results were also identified from the existence
of an excess current in the I-V curves (/spl theta/=24/spl
deg/) and a residual supercurrent in the strong magnetic field
dependence of Ic for the GBJJs with /spl theta/=24/spl deg/
(the field was applied up to 14 T). Next, the junction
homogeneity was investigated from the differences between
measured Ic(B) patterns and that of an ideal Josephson
junction. Contrary to expectation, the deviations of the GBJJs
with /spl theta/=24/spl deg/ or /spl theta/=36.8/spl deg/ from
an ideal Ic(B) pattern corresponded; the first minima did not
occur at zero, then the first maxima occurred at higher values
than normalized ideal case (I/sub 1-th minima//Ic/sub MAX//spl
ap/0.22). As a result, the current density distribution is
considered as an asymmetrical current density profile peaked
at the junction edges. Last, we have tried to control Jc on
the same tilt angle by changing the laser power in the pulsed
laser deposition process. The results showed Jc varied at the
range of about two order. |
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Ba/sub
1-X/K/sub X/BiO/sub 3/ grain boundary junctions prepared on
SrTiO/sub 3/ bicrystal
substrates S. Imaeda, M. Inoue,
A. Fujimaki and H. Hayakawa
Summary: We
succeeded in the fabrication of Ba/sub 1-X/K/sub X/BiO/sub 3/
artificial grain boundary junctions prepared on SrTiO/sub 3/
bicrystal substrates. These junctions showed the Josephson
current and the energy gap structure in the I-V
characteristics. In a magnetic field, the critical current was
modulated and the I/sub c/-B curve showed a clear Fraunhofer
pattern. Fiske steps were also observed in the I-V
characteristics. In the radiation of 10.5 GHz microwaves,
Shapiro steps were observed. |
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Excess
low-frequency noise in YBCO thin-film
devices J.C. Macfarlane, Ling
Hao, C.M. Pegrum and G.B. Donaldson
Summary:
Excess low-frequency noise degrades the performance of
many of the high T/sub c/ superconducting devices that have
been proposed or demonstrated. We report measurements of noise
in grain-boundary junctions and flux-flow amplifier devices
that have been fabricated in several different laboratories.
The system is calibrated in terms of absolute noise
temperature, and its voltage noise sensitivity is below 0.1
nVHz/sup -1/2/. Device characteristics and noise have been
measured as a function of junction area, critical current,
temperature, bias current and magnetic field. Noise levels in
a fixed frequency band of 40-60 kHz are reported, as well as
the frequency dependence between 0.1 Hz and 60 kHz. Noise
temperatures exceeding the device physical temperature at
certain levels of bias current are attributed to fluctuations
in critical current and normal tunnelling resistance. Noise
due to magnetic flux motion is also seen. We compare results
with available theory and other relevant data in the
literature, and assess the practical effects of noise on the
performance of high T/sub c/ devices such as SQUIDs, flux flow
amplifiers and bolometers. |
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Niobium
SIS mixers at 490 GHz, 690 GHz and 810
GHz C.E. Honingh, K. Jacobs, S.
Haas, D. Hottgenroth and J. Stutzki
Summary:
Low noise mixers are developed for a dual channel
heterodyne receiver for astronomical applications which will
operate alternatingly in two of three the frequency bands
460-490 GHz, 660-690 GHz, and 800-850 GHz. As mixing elements
Nb-Al/sub 2/O/sub 3/-Nb (SIS) tunnel junctions are used,
fabricated at the University of Cologne with integrated RF and
IF circuitry, also made of niobium. The frequency dependent
RF-properties of the circuitry are calculated for all bands
using Mattis-Bardeen theory in the extreme anomalous limit.
The circuits are optimized for a large instantaneous receiver
bandwidth to facilitate the use of waveguide type mixer mounts
without mechanical tuners. Results on receiver noise,
stability and design accuracy will be presented. |
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Fabrication
and mixer performance of Nb/Al double-barrier
junctions T. Lehnert, Sheng-Cai
Shi and T. Noguchi
Summary: Specific
difficulties of the fabrication of Nb/Al double-barrier
junctions with high current density (10 kA/cm/sup 2/) and
small area (1-3 /spl mu/m/sup 2/) are discussed and possible
solutions are presented. The problem of nonuniform areas of
the two superposed junctions was circumvented by introducing a
loading effect in the etching process. Strong backbending of
the I/V-curve was reduced by increasing the thickness of the
Nb layer between the two superposed junctions. In a mixer
experiment in the 100 GHz frequency band a broad-band response
of the double-barrier device was obtained with a minimum
receiver noise temperature of 45 K at 115 GHz. |
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Modulation
of self-resonant modes in NbCN/MgO/NbCN junctions by
quasiparticle injection S.
Kohjiro, S. Kiryu, A. Shoji, S. Kodaira and S.
Takada
Summary: In the submillimeter wave
region, we have studied the modulation of self-resonant modes
in NbCN/MgO/NbCN Josephson junctions (detectors). The tuning
mechanism is based on the quasiparticle injection via an
overlaid tunnel junction (injector). From the current-voltage
characteristics of detectors, the maximum shift of resonant
frequencies /spl Delta/f and Q factors due to electrode loss
at the injected state Q/sub inj/ have been estimated to be
/spl Delta/f/f(0)=0.11 and Q/sub inj/=100 at 470 GHz, where
f(0) is the resonant frequency without quasiparticle
injection. It is found Q/sub inj/ decreases with increase of
the injector bias voltage. |
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An
SIS mixer using two junctions connected in
parallel T. Noguchi, Sheng-Cai
Shi and J. Inatani
Summary: We have
fabricated a superconductor-insulator-superconductor (SIS)
mixer using a couple of junctions connected in parallel
through a stripline inductor. The junctions have significantly
larger area, i.e. larger capacitance, and smaller normal
resistance than conventional ones. In order to obtain a good
impedance matching between the source and the junctions, an
impedance transformer made of a superconducting stripline was
integrated with the junctions. The capacitance of the
junctions was tuned out by the inductor to obtain a broadband
operation without mechanical tuning elements. It was shown
that the double sideband noise temperature of the receiver
employing this type of mixer device was less than 40 K over
the bandwidth of 90-115 GHz. The lowest receiver noise
temperature of /spl sim/20 K, which is only 4 times as large
as the quantum limited photon noise of hv/k/sub B/, was
obtained around 105 GHz. |
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Hot
electron quasioptical NbN superconducting
mixer B.S. Karasik, G.N.
Gol'tsman, B.M. Voronov, S.I. Svechnikov, E.M. Gershenzon, H.
Ekstrom, S. Jacobsson, E. Kollberg and K.S.
Yngvesson
Summary: Hot electron
superconductor mixer devices made of thin NbN films on SiO/sub
2/-Si/sub 3/N/sub 4/-Si membrane have been fabricated for
300-350 GHz operation. The device consists of 5-10 parallel
strips each 5 /spl mu/m long by 1 /spl mu/m wide which are
coupled to a tapered slot-line antenna. The I-V
characteristics and position of optimum bias point were
studied in the temperature range 4.5-8 K. The performance of
the mixer at higher temperatures is closer to that predicted
by theory for uniform electron heating. The intermediate
frequency bandwidth versus bias has also been investigated. At
the operating temperature 4.2 K a bandwidth as wide as 0.8 GHz
has been measured for a mixer made of 6 nm thick film. The
bandwidth tends to increase with operating temperature. The
performance of the NbN mixer is expected to be better for
higher frequencies where the absorption of radiation should be
more uniform. |
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A
heterodyne receiver at 533 GHz using a diffusion-cooled
superconducting hot electron bolometer
mixer A. Skalare, W.R. McGrath,
B. Bumble, H.G. LeDuc, P.J. Burke, A.A. Verheijen and D.E.
Prober
Summary: This paper describes
heterodyne measurements at 533 GHz using a novel
superconducting hot electron bolometer in a waveguide mixer
block. The bolometer is a thin (10 nm) and narrow (0.1 /spl
mu/m) strip of niobium with a length of less than half a
micron and a critical temperature of approximately 5.5 K. The
short length ensures that diffusion dominates over
electron-phonon interaction as a cooling mechanism for the hot
electrons, thus allowing heterodyne detection with
intermediate frequencies of several GHz. A Y-factor response
of 1.15 dB has been obtained at an intermediate frequency of
1.4 GHz with hot/cold load temperatures of approximately
295/77 K, indicating a receiver noise temperature around 650 K
DSB. The IF response extends up to at least 2 GHz and possibly
higher. |
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Signal
resolution of RSFQ
comparators T.V. Filippov, Y.A.
Polyakov, V.K. Semenov and K.K. Likharev
Summary:
We have designed and tested a Rapid Single-Flux-Quantum
(RSFQ) circuit for experimental measurement of the
fluctuation-induced threshold uncertainty of switching of SFQ
comparators, which are essential components of RSFQ logic
devices, analog-to-digital converters, and digital SQUIDs.
Statistical density of the switching events in comparators
using externally-overdamped Nb-trilayer Josephson junctions
has been found to be in agreement with the distribution which
follows from a simple theory based on a time-dependent
harmonic-oscillator model of the device. Width of the
distribution (i.e, the single-shot current resolution of the
comparator) measured as a function of temperature in the range
1.7-4.2 K corresponds to fundamental (thermal/quantum)
fluctuations, with no evidence of excess noise
sources. |
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Design
and testing of QOS comparators for an RSFQ based analog to
digital converter D.K. Brock,
S.S. Martinet, M.F. Bocko and J.X. Przybysz
Summary:
Successful utilization of the quasi one-junction SQUID
(QOS) as a signal comparator for analog-to-digital conversion
(ADC) has been demonstrated by several groups, This idea is
extended to show how similar comparators can be integrated
into an all rapid single flux quantum (RSFQ) digital
architecture. Comparators are interrogated by SFQ sampling
pulses and in turn give output according to the RSFQ
convention. One- and two-bit ADC's have been simulated,
fabricated and tested at low speed. Total performance of these
devices is estimated within the framework of a multiple bit
parallel flash ADC architecture. |
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Two-loop
modulator for sigma-delta analog to digital
converter J.X. Przybysz, D.L.
Miller and E.H. Naviasky
Summary: A two-loop
modulator has been designed for a superconductive sigma-delta
analog to digital converter. In contrast to semiconductor
modulators, which use high-gain amplifiers in the signal feed
forward path, the superconductive modulator used digital gain
in the signal feedback path. The use of superconductive
electronics to precisely feed back a single flux quantum into
the second integrator loop and multiple flux quanta into the
first integrator loop is a key to this circuit. In simulations
of a 40 GHz sampling rate, the modulator obtained a 98 dB
signal to noise ratio on the dc-60 MHz band. The modulator
tolerated thermal noise well, obtaining 98 dB SNR on the dc-4
MHz band, while sampling at a rate of 4 GHz. The modulator
tolerated clock timing jitter better than Nyquist-rate A/D
converters, obtaining equivalent performance with 3 times as
much rms jitter. Compared to single-loop sigma-delta and
oversampled lobe-counting A/D converters, the two-loop
modulator can achieve equivalent performance at a
significantly reduced sampling and digital filter
rate. |
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Design
of SFQ-counting analog-to-digital
converter J.C. Lin, V.K. Semenov
and K.K. Likharev
Summary: We describe the
design of an oversampling single-flux-counting
analog-to-digital converter with the estimated bandwidth of a
few tens of MHz, based on Rapid Single-Flux-Quantum (RSFQ)
devices. It consists of an input analog circuit, high-speed
quantizer with an original analog/digital negative feedback
loop, decimation (comb) filter, and supporting subsystems
including clock distribution circuits, quantization signal
conditioner, and output drivers. We have applied a new
approach, the 'symmetrizing' negative feedback, to free the
quantizer from the intrinsic hysteresis without dynamic range
sacrifice. The 16-bit version of the system comprises about
1,500 Josephson junctions and consumes 1.2 mW of DC power,
when implemented using Nb-trilayer technology with 1 kA/cm/sup
2/, 3.5 /spl mu/m Josephson junctions. All subsystems of the
converter have been successfully tested and testing of the
system as a whole is in progress. |
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Superconducting
high-resolution A/D converter based on phase modulation and
multichannel timing
arbitration S.V. Rylov and R.P.
Robertazzi
Summary: We have developed a
flux-quantizing A/D converter (ADC) based on RSFQ elements,
employing a novel front end capable of generating
high-linearity multibit differential code within a wide
dynamic range (up to 16 bits). The front end operates as a
phase modulator/demodulator and uses fractional-flux-quantum
least significant bit (LSB). It runs at multi-GHz speed,
enabling ADCs with large oversampling ratio and effective
resolution in excess of 20 bits (after decimation filtering).
We have designed, fabricated and tested several versions of a
complete ADC using this new architecture and demonstrated its
operation with dynamic range of 14 bits. We have also
confirmed continuous phase modulation of the flux quantizer
with a carrier frequency of 10 GHz. |
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Design
and high-speed testing of a superconducting delta-sigma
oversampled converter P.H. Xiao,
D. Hebert, S.R. Whiteley and T. Van Duzer
Summary:
A delta-sigma modulator with a lowpass filter can
achieve the same signal-to-noise ratio (SNR) and dynamic range
as a delta-sigma modulator with an integrator by adjusting the
cut-off frequency of its lowpass filter. A lowpass filter
modulator in superconducting niobium technology was designed
and tested up to a 1 GHz sampling rate and was shown to be
operating correctly. The bits of a pseudo-random bit stream
digital output are acquired individually by a high-speed logic
analyzer. The acquired data show 6 bits of modulator dynamic
range, which is limited below the simulated value of 11 bits,
at least in part, by errors in the test
equipment. |
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Operation
of Josephson comparator under Josephson noise from
SQUID E. Takeda, T. Nishino and
K. Takagi
Summary: Operation of a Josephson
comparator for analog-to-digital conversion of signal from a
SQUID is studied. In the study, a test circuit consisting of
the SQUID and the comparator is used. The measured result
shows that the comparator responds to AC noise due to the AC
Josephson effect. Numerical simulation shows amplitude, which
is determined from the response of the comparator, is smaller
than the original AC noise amplitude. The difference comes
from low-pass characteristics of the Josephson junction in the
comparator due to the turn-on delay. The delay is effective in
reducing the AC noise, and provides a means for the accurate
conversion. |
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Microwave
properties of voltage-tunable YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta///SrTiO/sub 3/ coplanar waveguide transmission
lines D.C. DeGroot, J.A. Beall,
R.B. Marks and D.A. Rudman
Summary: To
explore the electrical characteristics of monolithic microwave
circuits with integrated high-temperature superconductor and
ferroelectric materials, we fabricated a series of coplanar
waveguide transmission lines in laser-deposited YBa/sub
2/Cu/sub 3/O/sub 7-/spl delta// and SrTiO/sub 3/ thin films.
We characterized the voltage-tunable two-port microwave
response of the transmission lines at cryogenic temperatures
using a calibrated network analyzer system. Total phase shifts
and phase tuning in these devices increased for increasing
ferroelectric film thickness with only moderate increases in
transmission loss. |
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Optical
switching of HTS band reject
resonators E.R. Soares, K.F.
Raihn, N.O. Fenzi and G.L. Matthaei
Summary:
A method for optically switching HTS (High Temperature
Superconducting) band reject resonators is presented. Fast low
loss switching of HTS filter elements enable digital selecting
of arbitrary pass bands and stopbands. Each switch element
must preserve the high Q of the HTS filter element in one
switch state, and remove the HTS filter element without adding
loss in the other state. Patterned pieces of GaAs are used as
the switch. Fiber optic cabling is used to bring the optical
energy to the cryogenic package. This minimizes the thermal
loading of the filter package. Cryogenic switching of a single
resonator is discussed, as well as integration of the
switching method to entire filters and banks of fibers.
Measured and modeled data are compared. |
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A
4 bit instantaneous frequency meter at 10 GHz with coplanar
YBCO delay lines M. Biehl, A.
Vogt, R. Herwig, M. Neuhaus, E. Crocoll, R. Lochschmied, T.
Scherer, W. Jutzi, H. Kratz, P. Berberich and H.
Kinder
Summary: A device on a single
2"-LaAlO/sub 3/ wafer for a four bit instantaneous frequency
measurement between 9.5 GHz and 10.5 GHz has been developed
with coplanar YB/sub 2/Cu/sub 3/O/sub 7-/spl delta// delay
lines and power dividers. Compared to known triplate strip
lines, coplanar delay lines are easier to fabricate
monolithically and allow for a greater flexibility in the
circuit design. Simulated and measured results are in good
agreement. |
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An
integrated 11 GHz cryogenic
downconverter W.A. Phillips, D.
Jedamzik, K. Lamacraft, S. Zammattio, R.B. Greed, S.J. Hedges,
P.R. Whitehead, B.F. Nicholson, T.W. Button, P.A. Smith, N.M.
Alford, N. Peters and J. Grier
Summary: A
cryogenic downconverter has been designed and built to
demonstrate the integration of semiconducting and
superconducting components in a complete subsystem cooled by a
closed cycle Stirling cryocooler. The frequency selective
receiver converts 11 GHz (X-band) signals to an IF of 1000 MHz
using a high temperature superconducting (HTS) microstrip
input filter with a 1% bandwidth, a silicon diode mixer and a
local oscillator stabilized by means of a 10 GHz HTS cavity
and driven by a GaAs HEMT. The components are packaged into a
cryogenic unit cooled to 60 K. Details of the system
integration are presented, together with microwave and thermal
test results. |
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A
superconducting and integrated microwave transmitter and
receiver in microstrip using thick-film
YBCO M.W. Hosking, Y.G. Proykova,
A. Hewitt, N.McN. Alford and T.W. Button
Summary:
Results are presented of the design and performance of
a microstrip transmitter/receiver circuit using thick-film
yttrium barium copper oxide on a yttria-stabilised zirconia
substrate. The resonant circuit is in the form of a ring
resonator and the active component is a transferred electron
device integrated within the circumference of the ring. In
receive mode, the circuit operates as a self-oscillating
mixer. Operating frequencies lie in the range 8 to 16 GHz and
measurements include: Q-factor by injection phase locking;
oscillator output power and conversion loss. |
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High-temperature
superconducting wide band delay
lines S.H. Talisa, M.A. Janocko,
D.L. Meier, C. Moskowitz, R.L. Grassel, J. Talvacchio, P.
LePage, D.C. Buck, R.S. Nye, S.J. Pieseski and G.R.
Wagner
Summary: Stripline non-dispersive
delay lines with 20 GHz of bandwidth were designed and
fabricated using YBCO thin films deposited on both sides of
2-inch-diameter, 10-mil thick LaAlO/sub 3/ wafers. A
double-wound spiral configuration was used yielding a line
length of approximately 150 cm. Novel approaches were used to
minimize the effect of air gaps between the two substrates
needed to form the stripline structure, and to realize a wide
band transition from the coaxial external connections to
stripline. Experimental results showed 5 dB of insertion loss
at 20 GHz, with 1 dB amplitude ripple over most of the 0-20
GHz, range for a 22.5 ns delay. |
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A
robust fabrication process for a refractory integrated SQUID
gradiometer D. Hutson, R.G.
Weston, R.J.P. Bain, M.J. Lawrenson, C.M. Pegrum, K. Popova
and R. Scarfone
Summary: We describe a
process used successfully to fabricate large second-order
planar gradiometers with integrated DC SQUIDs on two-inch
silicon wafers. All the refractory materials (Nb, Mo and
SiO/sub 2/) are deposited by magnetron sputtering. The
Josephson junctions are based on the well-established
Nb/AlO/sub x//Nb trilayer technology. All Nb layers are
patterned by Reactive Ion Etching using a procedure optimized
by experimental design. Since only one gradiometer can fit on
a wafer, extra care had to be taken in both the design of the
device and the fabrication process to ensure that the yield
was high. Excellent process latitude is achieved by sufficient
built-in design margins to accommodate any tolerance
difficulties during fabrication. |
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Effects
of aluminum over-layer thickness on characteristics of niobium
tunnel junctions fabricated by DC magnetron
sputtering A. Nakayama, H.
Nagashima, J. Shimada and Y. Okabe
Summary:
We have fabricated Nb/AlO/sub x//Nb Josephson tunnel
junctions using a sputtering apparatus with a load-lock
system. The junctions that had 50 /spl mu/m/spl times/50 /spl
mu/m area showed a V/sub m/ value (the product of the critical
current and the subgap resistance at 2 mV) as high as 50 mV at
a current density of 160 A/cm/sup 2/. Moreover, junctions
having different thicknesses of the Al overlayer were
concurrently fabricated on one wafer to study the dependence
of the current-voltage characteristics on this Al over-layer.
The I-V characteristics were also calculated by McMillan's
tunneling model and were compared with the measured I-V
characteristics. |
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Superconducting
integrated circuit fabrication with low temperature ECR-based
PECVD SiO/sub 2/ dielectric
films J.E. Sauvageau, C.J.
Burroughs, P.A.A. Booi, M.W. Cromar, R.P. Benz and J.A.
Koch
Summary: A superconducting integrated
circuit fabrication process has been developed to encompass a
wide range of applications such as Josephson voltage
standards, VLSI scale array oscillators, SQUIDs, and
kinetic-inductance-based devices. An optimal Josephson
junction process requires low temperature processing for all
deposition and etching steps. This low temperature process
involves an electron cyclotron resonance-based plasma-enhanced
chemical vapor deposition of SiO/sub 2/ films for interlayer
dielectrics. Experimental design and statistical process
control techniques have been used to ensure high quality oxide
films. Oxide and niobium etches include endpoint detection and
controlled overetch of all films. An overview of the
fabrication process is presented. |
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Fabrication
of submicron Nb/AlO/sub x/-Al/Nb tunnel junctions using
focused ion beam implanted Nb patterning (FINP)
technique H. Akaike, T. Watanabe,
N. Nagai, A. Fujimaki and H. Hayakawa
Summary:
We have successfully fabricated 0.2 /spl mu/m/sup 2/
Nb/AlO/sub x//Nb tunnel junctions using the focused-ion-beam
implanted Nb patterning (FINP) technique for junction
definition. The success was due to improvement of the edge
profile of the counter electrode. The vertical edge profile
was realized with the large etching selectivity of Ga
implanted Nb over unimplanted Nb by controlling the reactive
neutrals in the plasma. The critical current I/sub c/ and the
quality parameter V/sub m/ of 0.2 /spl mu/m/sup 2/ junctions
were 10.5 /spl mu/A and 11 mV, respectively. The R/sub
sg//R/sub n/ was 12. The maximum to minimum spread in I/sub c/
of 60 series junctions with areas of 0.5 /spl mu/m/sup 2/ was
/spl plusmn/10%. |
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The
fabrication and characterization of NbCN/AlN
heterostructures Z.H. Barber,
D.M. Tricker and M.G. Blamire
Summary: Very
high quality niobium nitride based
superconductor-insulator-superconductor (SIS) junctions have
been prepared using aluminium nitride barrier layers deposited
by dc reactive magnetron sputtering. These barriers have been
shown to grow epitaxially on high quality epitaxial niobium
carbonitride (NbCN) base electrodes. High total gap voltages,
equal to the maximum that can be expected theoretically,
illustrate that there are no degraded layers at the
superconductor/insulator interfaces. We have also demonstrated
the first SISIS double barrier devices. Transmission electron
microscopy has been used to study the growth of a thick AlN
layer sandwiched between NbCN and the microstructure of
NbCN/AlN multilayers prepared with several different
orientation relationships. |
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Nb/AlN/Nb
Josephson junctions with high critical current
density A.W. Kleinsasser, W.H.
Mallison and R.E. Miller
Summary: We have
produced Nb/AlN/sub x//Nb Josephson tunnel junctions with the
aims of improving the control of critical current density
J/sub c/ in the high-J/sub c/ range and exploring the
possibility of high-J/sub c/ junctions with low subgap
quasiparticle currents. Conventional Nb/AlO/sub x//Nb junction
barriers are formed by oxidizing a thin Al overlayer on the Nb
base electrode, and precise control of the oxidation process
is difficult at low levels of oxygen exposure. The reactivity
of Al with N/sub 2/ is very low, and AlN/sub x/ barriers are
therefore formed using an N/sub 2/ plasma. We report the
fabrication of AlN/sub x/ barrier junctions with J/sub c/ as
large as 4 mA//spl mu/m/sup 2/ and compare their properties to
Nb/AlO/sub x//Nb ones of similar J/sub c/. |
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NbN/AlN/NbN
tunnel junctions fabricated at ambient substrate
temperature Z. Wang, A. Kawakami,
Y. Uzawa and B. Komiyama
Summary: We have
prepared NbN/AlN/NbN tunnel junctions at ambient substrate
temperature. The AlN barriers are fabricated by reactive rf
magnetron sputtering in the N/sub 2/ sputtering gas. We
describe the electric and crystalline properties of the NbN
and AlN thin films, and discuss tunneling characteristics and
the properties of the junction interface. Even though the
NbN/AlN/NbN trilayers were deposited without intentional
heating, the junctions had a large gap voltage (V/sub g/=5
mV), sharp quasiparticle current rise (/spl Delta/V/sub
g/=0.16 mV), and small subgap leakage current (V/sub m/=25
mV). A high critical current density (J/sub c/=8 KA/cm/sup 2/)
is obtained in junctions with 1.5 nm thick AlN barriers. These
results show that high-quality NbN/AlN/NbN tunnel junctions
can be prepared at ambient substrate
temperatures. |
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Stress
and source conditions of DC magnetron sputtered Nb
films R.S. Amos, P.E. Breyer,
H.H. Huang and A.W. Lichtenberger
Summary: We
have studied the quality of Nb films from two different DC
magnetron sources in a vein similar to previous work at
Fujitsu Laboratories and NIST. In particular we are interested
in the effects of target erosion on Nb film quality and on
operating conditions of the magnetron sources. We find that
the concept of a current-pressure (I-P) stress line of
constant voltage (NIST), though giving qualitative guidance on
proper source operating conditions, is not a sufficiently
accurate model to set either of our magnetron source
conditions over the life of the targets. In particular we find
that: (1) the shape of our I-P "lines" change with target
usage, (2) the stress values attributed to different points on
a given I-P line at one "snapshot" in the target life are
often different, and (3) the stress attributed to a given
point on an I-P line may change over the life of a target.
Alternative source operation strategies for maintaining stress
free films will be discussed and the influence of other
parameters including temperature, substrate material, source
distance, substrate motion and target to target repeatability
will also be examined. |
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Effect
of growth conditions on the electrical properties of
Nb/Al-oxide/Nb tunnel
junctions W.H. Mallison, R.E.
Miller and A.W. Kleinsasser
Summary: We have
investigated the dependence of the critical current density
J/sub c/ of Nb/AlO/sub x//Nb Josephson tunnel junctions on
substrate temperature T/sub s/ and oxygen exposure E (the
product of oxidation time and pressure) during growth. For low
O/sub 2/ exposures, J/sub c/ depended sensitively on exposure,
J/sub c//spl prop/E/sup -1.6/, independent of temperature for
77 K |
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An
improved etching process used for the fabrication of submicron
Nb/AlO/sub x//Nb Josephson
junctions M. Aoyagi, M. Maezawa,
H. Nakagawa, I. Kurosawa and S. Takada
Summary:
It is important to develop a reliable and reproducible
fabrication process of submicron Nb/AlO/sub x//Nb Josephson
junctions to improve the integration level and the operating
speed of the Josephson LSI circuit. For this purpose, we have
developed an improved etching process by introducing a dummy
etching process and using a scanning electron microscope (SEM)
as an etching end-point detector. The dummy etching process
improves the anisotropy of a reactive ion etching (RIE)
process using CF/sub 4/. The etching residue around a junction
is detected easily and correctly by the SEM observation. We
have successfully fabricated Nb/AlO/sub x//Nb Josephson
junctions with critical current density of 10/sup 4/ A/cm/sup
2/ using the cross-line patterning (CLIP) method and electron
beam lithography, where the junction size was varied from 2
/spl mu/m to 0.5 /spl mu/m at 0.1 /spl mu/m intervals.
High-quality submicron junctions for integrated circuits with
suitable critical current variations were
obtained. |
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Monolithic
flux transformer-coupled high-T/sub c/ DC SQUID
magnetometers J.W.M. Hilgenkamp,
G.C.S. Brons, S. Hoogeveen, J. Flokstra and H.
Rogalla
Summary: YBa/sub 2/Cu/sub 3/O/sub
7-x/ based monolithic flux transformer-coupled high-T/sub c/
DC SQUID magnetometers operating up to 73 K have been
realized. The devices are characterized by high values of the
modulation voltage, up to 32 /spl mu/V at 40 K. A minimal
white noise level of 0.10 pT//spl radic/Hz was obtained above
200 Hz, and 0.64 pT//spl radic/Hz at 1 Hz and 55 K. The
temperature dependence of the modulation voltage, the
effective sensing area and the field sensitivity are
discussed. Model-calculations have been performed to
investigate high frequency resonances in the washer-input coil
structure. Methods for damping are considered. |
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Integrated
YBa/sub 2/Cu/sub 3/O/sub 7/ multi-loop magnetometers at 77
K D. Reimer, M. Schilling, S.
Knappe and D. Drung
Summary: We present a
multi-loop DC SQUID magnetometer operated at 77 K. In a
multi-layer process YBa/sub 2/Cu/sub 3/O/sub 7/, PrBa/sub
2/Cu/sub 3/O/sub 7/, and SrTiO/sub 3/ films are deposited by
KrF-excimer laser deposition on SrTiO/sub 3/(100) substrates.
The preparation consists of four film deposition and three
patterning steps. We employ YBa/sub 2/Cu/sub 3/O/sub 7/
Josephson junctions with artificial barriers of PrBa/sub
2/Cu/sub 3/O/sub 7/ in a ramp-type geometry. The
characterization is made by electrical transport and by noise
measurements. The measured magnetic field sensitivity of 1.25
nT//spl Phi//sub 0/ of our device fits well with the
calculated value of 1.17 nT//spl Phi//sub 0/. |
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DC-SQUIDs
and flux transformers in YBa/sub 2/Cu/sub 3/O/sub 7/
magnetometers at 77 K M.
Schilling, R. Scharnweber and S. Volkl
Summary:
For biomagnetic applications magnetometer devices are
prepared in a multilayer process based on KrF-excimer laser
deposition of superconductor and insulator layers as well as
semiconducting barriers. For patterning conventional
photolithography and argon-ion etching are used. In the
DC-SQUIDs we employ Josephson junctions with artificial
barriers of PrBa/sub 2/Cu/sub 3/O/sub 7/ in a ramp-type
geometry. As insulating layers in the flux transformers we use
SrTiO/sub 3/. Both, the DC-SQUIDs and the input-coils operate
up to temperatures of 86 K. The characterisation of the
devices is made by electrical transport and by noise
measurements. For the use as sensitive magnetometers the DC
SQUIDs are either used in inductively shunted magnetometers
with galvanic coupling to a large pick-up coil or are coupled
to flux transformers in a flip-chip arrangement. |
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SNS-DC-SQUIDs
and flux transformers for integrated magnetometers in
flip-chip technique B. Meyer, J.
Hollkott, C. Francke, R. Wunderlich and J.
Muller
Summary: YBa/sub 2/Cu/sub 3/O/sub
7-/spl delta///Ag/YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
Josephson-junctions across steps in MgO substrates were used
to fabricate SNS-DC-SQUIDs in the step-and-gap geometry. The
necessary break of the YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta//-film at the step was confirmed by transmission
electron microscopy investigations. The removal of the
Ag-layer eliminates the shunt resistance on top of the HTSC
which increases the normal resistance R/sub N/ by more than
two orders of magnitude with only a slight reduction in I/sub
C/. The junctions can be described by the SINS-formalism,
which allows high I/sub C/R/sub N/-products with large values
of the normal resistances R/sub N/. For thin-film flux
transformer epitaxial YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta///SrTiO/sub 3//YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
trilayers were grown using a co-sputter process. Test coils
exhibited a current density in excess of 8/spl times/10/sup 5/
A/cm/sup 2/ and insulation resistivities of 10/sup 8/ /spl
Omega/cm at 77 K. By coupling the flux transformers to SQUIDs
using a flip-chip technology the magnetic field response were
increased by a factor of 9. |
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High-T/sub
c/ superconducting image surface
magnetometers N. Tralshawala,
J.H. Miller Jr. and D.R. Jackson
Summary: We
present an overview of the concepts of image surface
magnetometry, and analyze various shapes of superconducting
shields in the presence of uniform background noise fields and
current sources that simulate biomagnetic sources. We show
that, for certain geometries and sizes, these shields can
selectively shield background noise fields as opposed to
signals of interest. We also show that clever use of these
shields can, in some cases, allow an undisturbed measurement
of the signals of interest while attenuating noise fields by
as much as four orders of magnitude. |
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Characteristics
of a NiO barrier layer for high-T/sub c/ superconducting
tunnel junction M. Moriya, T.
Hobayashi and T. Goto
Summary:
Characteristics of a NiO barrier layer for high-T/sub
c/ superconducting tunnel junctions were investigated. Bi/sub
2/Sr/sub 2/CaCu/sub 2/O/sub x/ (BSCCO) films were deposited on
a MgO or SrTiO/sub 3/ substrate using a dc hollow cathode
sputtering system. In situ superconducting BSCCO films
deposited in Ar+20%O/sub 2/ gas at T/sub s/=680/spl deg/C on a
MgO substrate were c-axis oriented 2212 phase. A NiO layer was
formed by reactive sputtering in Ar+20%O/sub 2/ gas using a
NiO hollow cathode, and the layer on the BSCCO film was of
[100] and [110] orientation. The current-voltage
characteristics of an Ag/NiO/BSCCO junction with a NiO barrier
layer 5 nm thick were investigated. In the G-V curves of some
junctions, a zero bias conductance peak was observed. It is
assumed that this behavior is probably due to the nonuniform
thickness of the barrier layer. The junction with a thicker
barrier layer (18 nm) showed tunnel current characteristics
without anomaly. |
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YBa/sub
2/Cu/sub 3/O/sub 7/(-/spl delta/) a-axis films and planar
junctions R.G. Wichern, E.M.C.M.
Reuvekamp, G.J. Gerritsma and H. Rogalla
Summary:
In order to prepare planar junctions, multilayers were
sputtered, using YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// as
superconductor and PrBa/sub 2/Cu/sub 3/O/sub 7/(-/spl delta/)
as barrier material. The sandwiches are a-axis oriented. Out
of these, single junctions were etched, planarized with
CeO/sub 2/. Finally gold contacts were sputtered. The
junctions are squares of size 20/spl times/20 to 100/spl
times/100 /spl mu/m/sup 2/. A prerequisite for successful
preparation of junctions from a-axis oriented multilayers is a
study of such films. Films deposited by RF off-axis sputtering
were characterized electrically, Their morphology was
investigated by XRD, AFM and TEM. The films are very smooth
and have a grain size of below 100/spl times/100 nm/sup 2/. To
improve T/sub c/ and crystal quality, template layers were
used. The T/sub c/ of a single film is about 62 K; by using a
template layer up to 78 K can be reached. For a-axis oriented
growth not only a reduction of the deposition temperature is
important, but also the growth rate must be high enough. Best
results were obtained at rates higher than 150 nm/h. The first
planar junctions show a supercurrent, but otherwise rounded
I-V curves. |
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Heterostructure
applications of in-plane oriented a-axis YBa/sub 2/Cu/sub
3/O/sub 7-x/ films on LaSrGaO/sub
4/ I. Takeuchi, Z. Trajanovic,
J.L. Peng, Z.Y. Li, S.N. Mao, P.A. Warburton, C.J. Lobb and T.
Venkatesan
Summary: We have fabricated
various heterostructures using in-plane oriented a-axis
YBa/sub 2/Cu/sub 3/O/sub 7/(-x) and PrBa/sub 2/Cu/sub 3/O/sub
7/(-x) on LaSrGaO/sub 4/ substrates.
Superconductor-insulator-superconductor multilayers were
fabricated with LaSrGaO/sub 4/ and Nd/sub 2/CuO/sub 4/ as
dielectric layers. For such structures with approximately 3000
/spl Aring/ of Nd/sub 2/CuO/sub 4/, both top and bottom layers
had T/sub c/ (R=0)/spl ges/85 K. YBa/sub 2/Cu/sub 3/O/sub
7-x//PrBa/sub 2/Cu/sub 3/O/sub 7-x//YBa/sub 2/Cu/sub 3/O/sub
7-x/ ramp-edge junctions were fabricated in the b-direction of
the a-axis fame, and an I/sub c/R product of 1 mV was obtained
at 4.2 K. |
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Single
and stacked Josephson junctions based on c-axis YBCO/PBCO
multilayers M.A. Bari, B.
Ghyselen, E.J. Tarte, R.E. Somekh, Y. Yan, J.E. Evetts, M.G.
Blamire, N.G. Chew and R.G. Humphreys
Summary:
Using whole wafer superconducting device technology we
have fabricated vertically stacked sandwich junctions with
c-axis oriented YBCO/PBCO/YBCO trilayers and double barrier
junctions. The resulting devices exhibit supercurrents through
130 nm at 4.2 K. We have observed RSJ-like I-V curves, Shapiro
steps and almost Fraunhofer-like dependence of the critical
current as a function of magnetic field. The scaling behaviour
of devices fabricated on perovskite (SrTiO/sub 3/ and
LaAlO/sub 3/) and MgO substrates differ. The results indicate
a certain uniformity for the barriers on the scale of the size
of the junction. We propose different mechanisms for
supercurrent and quasiparticle transport through the PBCO
barrier for the two substrate types. |
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Anomalous
temperature dependence of critical current in
YBaCuO/PrBaCuO/YBaCuO trilayer Josephson
junctions H. Akoh, H. Sato and S.
Takada
Summary: We have observed an anomalous
temperature dependence of the critical current I/sub c/ in all
(103)-oriented YBaCuO/PrBaCuO/YBaCuO trilayer Josephson
junctions with barrier thicknesses of 50 nm and an Ar plasma
treatment for the barriers. I/sub c/ of the junction increases
drastically at around 40 K as temperature is increased, has a
maximum value at about 65 K, and decreases towards the
critical temperature of the junction. The normal resistance of
the junction, on the other hand, decreases exponentially with
increasing temperature. The anomalous temperature dependence
of I/sub c/ may come from the proximity effect, taking into
account the semiconductor-like properties of the PrBaCuO
barrier. |
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YBCO/metallic
oxide/YBCO trilayers for high-T/sub c/ superconducting SNS
junctions Xiaofan Meng, O.
Takahashi and T. Van Duzer
Summary: Some
metallic oxides are prospective barrier materials for
high-T/sub c/ superconducting SNS junctions. Among them,
SrVO/sub 3/ is a metallic oxide with a bulk resistivity of
1-1000 /spl mu//spl Omega/-cm and a cubic perovskite-type
crystal structure. The lattice constant of SrVO/sub 3/ is 3.84
/spl Aring/ which is close to that of the high-T/sub c/
superconductor YBa/sub 2/Cu/sub 3/O/sub 7-x/ (YBCO, a=3.82
/spl Aring/, b=3.89 /spl Aring/). We report the fabrication of
metallic SrVO/sub 3/ thin films and YBCO/SrVO/sub 3//YBCO
trilayers using pulsed laser ablation. The crystal structure
and surface morphology of the films were studied by X-ray
diffraction and AFM. The electrical properties of the films
were measured by the standard four probe method. The potential
application of SrVO/sub 3/ thin films for the barriers of
high-T/sub c/ superconducting SNS junctions is
discussed. |
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Properties
of tunnel junctions with [103]YBa/sub 2/Cu/sub 3/O/sub
y//SrTiO/sub 3//[013]YBa/sub 2/Cu/sub 3/O/sub y/ layered
structure T. Matsui, T. Suzuki,
H. Kimura, D. Yamaguchi, A. Ueda and H.
Kamijo
Summary: Properties of tunnel
junctions have been studied in a [103]-oriented YBa/sub
2/Cu/sub 3/O/sub y//SrTiO/sub 3//[013]-oriented YBa/sub
2/Cu/sub 3/O/sub y/ ([103]YBCO/STO/(013)YBCO) layered
structures. In the junctions, we observed similar electrical
properties to those in [001]-oriented
YBCO/barrier/[001]-oriented YBCO junctions, such as broad gap
like structure and a conductance peak at zero bias voltage.
Cross-sectional observation for the junction revealed that
facets were mainly formed by [100]-, [010]- and [001]-planes
at the bottom of the top [103]YBCO layer and by [010]- and
[001]-planes at the bottom [013]YBCO surface, respectively.
The observation also revealed the existence of amorphous-like
layers at both the top [103]YBCO/STO and STO/bottom [013]YBCO
interfaces. |
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Fabrication
and properties of YBCO tunnel junctions by ion beam
sputtering X.Y. Cai, K. Usami, T.
Kobayashi and T. Goto
Summary: Au/SrTiO/sub
3//YBCO tunnel junctions were fabricated by ion beam
sputtering. The electrodes of YBCO and SrTiO/sub 3/ barrier
layer were deposited on MgO [100] substrate at 700/spl deg/C
and 550/spl deg/C respectively. The electrodes of YBCO had a
T/sub c/ of 70/spl sim/80 K. SrTiO/sub 3//YBCO bilayers have
been examined by X-ray diffraction and the results show that
both the YBCO and barrier layer were well oriented. The
current-voltage (I-V) and dV/dI-V characteristics of the
junctions were measured. In a pin hole free junction, the
resistance dip, corresponding to the density of states, was
obtained at voltage of 22 mV. |
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The
effect of trapped flux upon the magnetic field dependence of
the critical current of Josephson
junctions E.J. Tarte, H.W. Lean
and J.R. Waldram
Summary: Measurements of the
magnetic field dependence of the critical current I/sub c/(B)
of Josephson junctions, involving high temperature
superconductors, often give evidence that the supercurrents
are spatially non-uniform. However, flux trapping can
complicate the interpretation of I/sub c/(B) curves. A model
has been developed for the behaviour of SNS type junctions in
a trilayer geometry containing trapped flux. We have
investigated, using this model, combined with simulations, how
the features of the I/sub c/(B) curve change as the number of
trapped fluxlines increases. For a uniform junction,
flux-trapping distorts the I/sub c/(B) curve and suppresses
the maximum critical current by 1//spl radic/N/sub f/ where
N/sub f/ is the number of fluxlines. The effect of trapped
flux on current density correlation functions derived using
the Wiener-Khinchine theorem from I/sub c/(B) curves has also
been investigated and is described. In addition we discuss the
relevance of the model to planar geometries. |
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A
microwave technique for characterization of SNS and
grain-boundary junctions J.
Wosik, Lei-Ming Xie, M.F. Davis and J.C.
Wolfe
Summary: We have utilized a magnetic
field modulated microwave absorption technique for
characterizing SNS and grain-boundary junctions. The technique
is based on the measurements of the first derivative microwave
absorption P, with respect to an applied magnetic field B at
9.5 GHz, as a function of dc magnetic B/sub dc/. A homodyne
detection system is used. Due to flux quantization in a
non-uniform junction a series of equally spaced microwave
absorption lines can be observed for B/sub dc/ and, in
strongly coupled junction cases, the dependence of I/sub c/ on
magnetic field and temperature can be extracted. Both the
intra-grain boundary in a melt-textured YBa/sub 2/Cu/sub
3/O/sub x/ bulk material and thin film single grain boundary
junction (GBJ) YBa/sub 2/Cu/sub 3/O/sub x/ were investigated.
The result of the measurements agrees with a model in which
the grain boundary consists of several sub-junctions in
parallel. |
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Epitaxial
growth of NbN and NbC/sub x/N/sub 1-x/ films on 3C-SiC
film-covered Si wafers A. Shoji,
S. Kiryu and S. Kohjiro
Summary: Epitaxial
NbN and NbC/sub x/N/sub 1-x/ (x<0.3) films were fabricated
on 3C-SiC film-covered Si wafers. It is found that epitaxial
NbN films fabricated on 3C-SiC/Si substrates have about one
degree higher T/sub c/'s than those for epitaxial NbN films
fabricated on MgO substrates. T/sub c/ and normal-state
resistivity of fabricated epitaxial NbC/sub x/N/sub 1-x/ films
depended on the 3C-SiC overlayer thickness of substrates. From
results of R-T characteristic measurements, it is deduced that
contact resistance of 3C-SiC and NbN strongly depends on the
growth orientation of crystals. |
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Oxygen
annealing of ex-situ YBCO/Ag thin-film
interfaces J.W. Ekin, C.C.
Clickner, S.E. Russek and S.C. Sanders
Summary:
The resistivity of YBCO/Ag interfaces has been measured
for different oxygen annealing temperatures for a series of
ex-situ fabricated thin-film contacts having sizes from 16
/spl mu/m/spl times/10 /spl mu/m down to 4 /spl mu/m/spl
times/4 /spl mu/m. The interface resistivity began to decrease
after annealing at 10 minutes in one atmosphere oxygen. After
annealing at 400/spl deg/C, the contact resistivity decreased
by several orders of magnitude to the 10/sup -7/ range. The
500-nm thick Ag layer showed surface diffusion and
agglomeration for annealing temperatures above 400/spl deg/C;
this temperature thus represents a practical limit for oxygen
annealing the YBCO/Ag interface system for more than 10
minutes. Rapid cooling of the chip after annealing led to a
severe loss of critical current density in the YBCO layer,
which could be restored by reannealing and cooling at a slower
rate of 50/spl deg/C/min. The relative shape of the
conductance-vs.-voltage characteristics of the YBCO/Ag
interface were essentially unaltered by oxygen annealing; the
overall parabolic shape, superconducting gap features, and
magnetic-scattering zero bias anomaly remained constant, even
though the contact conductance increased by several orders of
magnitude. These data suggest main reduction in interface
resistivity enhancement of the effective contact area, not a
change in interface conduction mechanism. |
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Evidence
for tunneling and magnetic scattering at in situ
YBCO/noble-metal interfaces S.C.
Sanders, S.E. Russek, C.C. Clickner and J.W.
Ekin
Summary: We report low-temperature
conductance data for in situ YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta// (YBCO)/Ag, YBCO/Au, and YBCO/Pt planar c-axis
interfaces. Analysis of the conductance data for these
interfaces, which have resistivities as low as 1/spl
times/10/sup -8/ /spl Omega//spl middot/cm/sup 2/, indicates
that tunneling is the predominant transport mechanism.
Zero-bias conductance peaks are present for all of the in situ
interfaces. These peaks are analyzed in the framework of the
Appelbaum model and are attributed to the presence of isolated
magnetic spins at the interface. The presence and similarity
of the peaks for each noble-metal overlayer supports the
hypothesis that the magnetic spins are inherent to the YBCO
surface. |
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Electrical
interface structure in YBa/sub 2/Cu/sub 3/O/sub 7-x//metal
contact H. Terai, A. Fujimaki, Y.
Takai and H. Hayakawa
Summary: We have
investigated the electrical contacts between YBa/sub 2/Cu/sub
3/O/sub 7-x/ (YBCO) and Au. The dI/dV characteristics of the
c-axis-oriented YBCO/Au/Nb junctions reveal the existence of a
tunnel barrier at the YBCO/Au interface. The experimental
results of the YBCO/LaGaO/sub 3//Au/Nb junction suggest p-type
degenerate semiconductor-like behavior of YBCO along the
c-axis direction. The anomalously small I/sub c/R/sub n/ of a
few /spl mu/V in the c-axis direction are interpreted as the
band bending at the YBCO surface. On the other hand, the
experimental I/sub c/R/sub n/ value of 120 /spl mu/V in the
a-axis-oriented YBCO/Au/Nb junction is understood within the
scope of conventional theory. |
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The
YBCO[001]/Ag interface: correlation between specific contact
resistance and interfacial
microstructure Z.H. Gong, J.K.
Grepstad and R. Fagerberg
Summary: The
influence of the sample temperature during metallization on
the electrical performance of silver contacts to c-axis
oriented YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// (YBCO) thin
films has been investigated. The specific contact resistance,
/spl rho//sub c/, was measured for contacts of different
lateral dimensions, prepared by in situ Ag deposition at
different temperatures and defined by standard
photolithography. When corrected for a non-uniform current
distribution, this data shows that on average /spl rho//sub c/
is at least a factor 4 lower for contacts prepared by
metallization on a heated (T/sub sub//spl ap/600/spl deg/C)
YBCO surface than for contacts prepared by metallization at
room temperature (RT). The improved electrical performance
correlates with a distinct difference in the interfacial
microstructure of similar contacts, previously observed with
high-resolution transmission electron
microscopy. |
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Combined
photodiode and high-T/sub c/ transition edge bolometer
function on zirconia buffered silicon
membranes E. Steinbeiss, W.
Michalke, H. Neff and B. Schwierzi
Summary:
We report on a novel photoreceiver on silicon
membranes, comprising both, an efficient photodiode or quantum
detector and a transition edge bolometer on the same substrate
material. The photodiode action of the device originates from
the silicon substrate and delivers a fast optical response,
with a limited sensitivity range at wavelength <1.1 /spl
mu/m. The bolometer response, in contrast, is broadband, but
rather slow with response times in the ms regime. The
combination of both detectors thus represents a new optical
receiver concept, and should be useful for a broad range of
optical applications. |
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Reduced
temperature processing of YSZ buffer layers for HTSC
transition edge bolometers M.
Burnus, T. Heidenblut, G. Hefle, O.K. Semtchinova, B.
Schwierzi, W. Michalke, E. Steinbeiss, H. Neff and J.
Laukemper
Summary: Using the steep change in
the resistance at the superconducting transition edge a
sensitive and spectral broadband membrane type bolometric
detector prototype was developed. Response S, noise equivalent
power NEP and the time constant /spl tau/ were examined.
Employing inhibit technology and prefabrication of silicon
membranes, the developed process sequence clearly separates
the fabrication into silicon processing technology and
commonly explored HT/sub c/-superconductor deposition with
impact on cost effective future batch fabrication. Buffer
layer epitaxy at reduced deposition temperature improves
production yield (membranes!) and a recently developed
passivation technique saves process steps. Applying the
maximum bias current the bolometer prototypes already reveal
detectivities in excess of 1/spl times/10/sup 8/ [cm Hz/sup
1/2/ W/sup -1/] and a time constant of the order of
milliseconds. |
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Microfabricated
free-standing epitaxial Y-Ba-Cu-O microbolometers on silicon
substrates R. Barth, J. Siewert,
B. Spangenberg, C. Jaekel, H. Kurz, B. Utz, W. Prusseit, H.
Kinder and H. Wolf
Summary: The fabrication
sequence of Y-Ba-Cu-O air-bridge microbolometers on silicon
substrates is described. A comparison of air-bridge
microbolometers and bolometers on bulk silicon is given. The
bolometric response of the bolometers is studied with chopped
IR illumination at a wavelength of 1.3 /spl mu/m. The
influence of the fabrication technique on the bolometer
performance is discussed. Measurements of the voltage noise in
free-standing Y-Ba-Cu-O microbolometers are presented and
compared with the predicted values. |
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Progress
toward a low-noise temperature regulation using a
superconductive high-T/sub c/
microbridge E. Lesquey, C.
Gunther, S. Flament, R. Desfeux, J.F. Hamet and D.
Robbes
Summary: Our results measuring I-V
characteristics of YBCO/MgO microbridges show that large
current sensitivities (10 mA/K) as a function of temperature
can be obtained, roughly independently of the applied voltage
V up to a few hundred mV. This offers the possibility of
working with high values of the dynamic resistance so that the
phonon noise associated to the thermal boundary resistance,
located at the YBCO/MgO interface, becomes dominant. A noise
equivalent temperature of 10/sup -8/ K//spl radic/Hz (T=85 K,
f>1 kHz) has already been obtained in a 0.2/spl
times/12/spl times/10 /spl mu/m/sup 3/ microbridge. We
describe a process involving the periodical sampling of the
I-V characteristics that eliminates 1/f amplifier noise and
returns the current value (temperature dependent) at fixed
voltage bias (/spl plusmn/1 mV). This output, locked to a
reference voltage through a commercial temperature regulator,
leads to temperature fluctuations less than 100 /spl mu/K/sub
pp/ in a 10 Hz bandwidth. These results are promising to
enhance performances of high-T/sub c/ microbolometers as
infrared detectors. |
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Optical
mixing in thin YBa/sub 2/Cu/sub 3/O/sub 7-x/
films M. Zorin, G.N. Gol'tsman,
B.S. Karasik, A.I. Elantev, E.M. Gershenzon, M. Lindgren, M.
Danerud and D. Winkler
Summary: High quality,
j/sub c/ (77 K)>10/sup 6/ A/cm/sup 2/, epitaxial YBa/sub
2/Cu/sub 3/O/sub 7-x/ films of 50 nm thickness were patterned
into ten parallel 1 /spl mu/m wide strips. The film structure
was coupled to a single-mode fiber. Mixer response was
obtained at 0.78 /spl mu/m using laser frequency modulation
and an optical delay line. Using two semiconductor lasers at
1.55 /spl mu/m wavelength the beating signal was used to
measure the photoresponse up to 18 GHz. Nonequilibrium
photoresponse in the resistive state of the superconductor was
observed. Bolometric response dominates up to 3 GHz, after
which the nonequilibrium response is constant up to the
frequency limit of our registration system. Using an electron
heating model the influence of different thermal processes on
the conversion loss has been analyzed. Ways of increasing the
sensitivity are also discussed. |
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Thermal
budget simulations and device performance of microstructured
high-T/sub c/ transition edge bolometers on
silicon M. Berg, J. Laukemper, H.
Neff, E. Steinbeiss, W. Michalke, M. Burnus and T.
Heidenblut
Summary: Silicon represents the
material of choice for fast superconducting high quality
transition edge bolometers. The performance of these devices
sensitively depends on their thermal properties where the heat
flux critically affects time constant, optical response and
noise behavior. In this work extensive numerical Finite
Element-calculations have been performed for various bolometer
configurations, using the ABAQUS-code. A high degree of
thermal isolation can be established through microstructuring
techniques. The bolometric performance of a prototype device
is compared with the simulated data. Values of the detectivity
D* as high as 1/spl times/10/sup 10/ cm Hz/sup 1/2/ W/sup -1/
already should be feasible, while a time constant in the
regime below 10 ms would be retained. |
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Silicon
ion implantation of YBaCuO films for bolometer
application X. He, J. Musolf, E.
Waffenschmidt, K. Heime, H. Wolf and K.
Pierz
Summary: Silicon ion implantation was
used to shift the critical temperature of YBaCuO films
continuously to lower temperatures. The variation of T/sub c/
and other superconducting properties with ion fluence was
investigated in detail. Based on these results a new bolometer
structure was designed, fabricated and characterised. The
sensor area of the bolometer consists of a locally implanted
area with a lower critical temperature, while the contact pads
and connecting lines retain the original T/sub c/. At the
operating temperature the bolometer has a exactly defined
temperature sensitive area and shows a lower contact
resistance. Finally the feasibility of integrated bolometer
arrays is discussed. |
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Mixing
and detection in YBaCuO step-edge Josephson junction arrays up
to 670 GHz J. Konopka, I. Wolff,
S. Beuven and M. Siegel
Summary:
Submillimeter wave detectors and mixers based on
YBa/sub 2/Cu/sub 3/O/sub 7/ (YBCO) step-edge Josephson
junctions incorporated into planar antennas were designed and
tested up to 670 GHz at temperatures from 12 to 65 K. A
quasi-optic coupling system with a LaAlO/sub 3/ lens was used.
In some samples the noise intrinsic in the detection process
does not follow the Johnson noise law but has a minimum, which
for a given sample may occur in the temperature range between
35 to 50 K. Harmonic mixing recorded at 670 GHz proves that
the system equilibrium is established in a time shorter than
500 fs. |
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A
380 ps, 9.5 mW Josephson 4-Kbit RAM operated at a high bit
yield S. Nagasawa, Y. Hashimoto,
H. Numata and S. Tahara
Summary: We have
developed a Josephson 4-Kbit RAM with improved component
circuits and a device structure having two Nb wiring layers. A
resistor coupled driver and sense circuit are improved to have
wide operating margins. The fabrication process is simplified
using bias sputtering, as a result, its reliability is
increased. The RAM is composed of approximately 21000
Nb/AlO/sub x//Nb Josephson junctions, Mo resistors, Nb
wirings, and SiO/sub 2/ insulators. Experimental results show
a minimum access time of 380 ps and power dissipation of 9.5
mW. Maximum bit yield of 84% is obtained in minimum magnetic
field of about 20 /spl mu/G. We confirm that most of fail bits
are caused by trapped magnetic flux, and the RAM functions
properly for 98% of the memory cells after measuring fail bit
map several times. |
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Characterization
of a superconductive sigma-delta analog to digital
converter D.L. Miller, J.X.
Przybysz, D.L. Meier, Joonhee Kang and A.H.
Worsham
Summary: Sigma-delta analog to
digital converters (ADCs) use a combination of oversampling
and feedback to concentrate quantization noise outside the
frequency band of interest. Subsequent digital filtering can
then be used to suppress the quantization noise and yield a
large signal to noise ratio. Sigma-delta ADCs dominate the
high performance audio market, where the signal band is
limited to frequencies below 50 kHz and 8 octave oversampling
requires a sampling rate of only 25.6 MHz. Przybysz et al.
have described a superconductive circuit capable of >40 GHz
sampling, thereby extending the useful bandwith to tens of
MHz. In this paper, we describe the realization of that
circuit and present measurements of its performance. Spectral
analysis of the modulator performance shows spur-free dynamic
range of over 78 dB and third order intermodulation products
less than -68 dBc. Quantization noise shaping is also
demonstrated. |
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Design
of a 10 K NbN A/D converter for IR focal plane array
sensors L.R. Eaton, D.J. Durand,
R. Sandell, J.W. Spargo and T. Krabach
Summary:
We are implementing a 12 bit SFQ counting ADC with
parallel-to-serial readout using our established 10 K NbN
capability. This circuit provides a key element of the analog
signal processor (ASP) used in large infrared focal plane
arrays. The circuit processes the signal data stream from a
Si:As BIB detector array. A 10 mega samples per second (MSPS)
pixel data stream flows from the chip at a 120 megabit bit
rate in a format that is compatible with other superconductive
time dependent processor (TDP) circuits being developed. We
will discuss our planned ASP demonstration, the circuit
design, and test results. |
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Implementation
of a FFT radix 2 butterfly using serial RSFQ
multiplier-adders O.A. Mukhanov
and A.F. Kirichenko
Summary: We have designed
a Decimation-in-Time (DIT) radix 2 butterfly integrated
circuit. This circuit will be used to implement the 32-point
Fast Fourier Transform (FFT) in a parallel data flow
architecture. The radix 2 butterfly circuit uses serial RSFQ
math and consists of four single bit-wide serial multipliers
and eight carry-save serial adders. The circuit with 16-bit
word-length employs only 3400 junctions, occupies an area of
3.8/spl times/2.0 mm/sup 2/, and dissipates less than 1.1 mW
power. The multiplier is implemented using the unique RSFQ
bit-clock-pipelined schema. We have successfully tested a
library of serial multiply-add elements: the 8-bit multiplier
at 6.3 GHz and adders with dc bias margin /spl plusmn/20%.
Finally, we have demonstrated full operation of the radix 2
butterfly chip with 5-bit word length. |
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Development
of a biomagnetic measurement system for brain
research M. Ueda, A. Kandori, H.
Ogata, Y. Takada, T. Komuro, K. Kazami, T. Ito and H.
Kado
Summary: The tail of the dewar of the
authors' system has a special shape that makes it possible to
measure the brain activity of anyone lying on a bed regardless
of head shape or size. It allows the parietal, one side of the
temporal and the occipital regions to be measured
simultaneously. In the system, 128 axial first-order
gradiometers are mounted at intervals of about 26 mm. The
diameter and baseline length of the pickup coil are 14 mm and
50 mm, respectively. The authors use square-shaped
double-washer DC-SQUIDs with additional positive feedback to
improve the flux resolution. System reliability is improved by
hermetically sealing the SQUID in a ceramic package and
including a heater resistor to eliminate trapped flux. To
decrease the liquid helium evaporation rate, output cables are
made with flexible printed circuits. The read-out electronics
are based on the Direct Offset Integration Technique, which is
a highly simplified feedback method. The white noise level
measured in a magnetically shielded room is less than 10
fT//spl radic/Hz above 5 Hz. This system has successfully been
applied to measuring auditory evoked fields. |
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Active
noise compensation for multichannel magnetocardiography in an
unshielded environment W.A.M.
Aarnink, P.J. Van Den Bosch, T.-M. Roelofs, M. Verbiesen, H.J.
Holland, H.J.M. Ter Brake and H. Rogalla
Summary:
A multichannel high-T/sub c/-SQUID-based heart scanner
for unshielded environments is under development, Outside a
magnetically shielded room, sensitive SQUID measurements are
possible using gradiometers. However, it is difficult to
realize large-baseline gradiometers in high-T/sub c/
materials, Therefore, the authors developed two active noise
compensation techniques. In the Total Field Compensation
technique, a Helmholtz type coil set is placed around the
sensors. One magnetometer is used as a zero detector
controlling the compensation current through the coil set. For
Individual Flux Compensation, the reference signal is sent to
the separate SQUIDs (or their flux transformer circuits) to
compensate the local environmental noise fluxes, The latter
technique was tested on low-T/sub c/ rf-SQUID magnetometers,
each sensor set to a field resolution SQUID magnetometers,
i.e. 0.1 pT/sub RMS///spl radic/Hz. The authors were able to
suppress the environmental disturbances to such an extent that
magnetocardiograms could be recorded in an ordinary
environment. Here the two suppression techniques are described
and experimental results are presented. |
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Development
of semi-portable DC-SQUID
magnetometer A. Kandori, M. Ueda,
H. Ogata and H. Kado
Summary: A semi-portable
DC-SQUID magnetometer with a liquid helium continuous flow
cryostat has been developed. The cryostat is 340 mm long and
50 mm in outer diameter. The pick-up coil is a co-axial, first
order, differential type, 20 mm in diameter and 30 mm in
baseline. The distance between the pick-up coil and the outer
surface of the cryostat is 5 mm. It is easy to set this
cryostat on the chest wall or on a human head. The cool down
time is about 20 minutes, which is much shorter than that for
a conventional storage Dewar. The white noise level, measured
in a magnetically shielded room, is 8.7 fT//spl radic/Hz at 30
Hz. Noise at 1 Hz is about 30 fT//spl radic/Hz. Noise from
temperature fluctuations (<9 mK) and drift (4.22 K /spl
sim/ 4.55 K) is negligible. The consumption rate of liquid
helium is 10 l/h. Here, the authors show the measurement of a
magnetocardiogram in a magnetically shielded
room. |
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Image
processing techniques for NDE SQUID
systems C.H. Barbosa, A.C. Bruno,
L.F. Scavarda, E.A. Lima, P. Costa Ribeiro and C.
Kelber
Summary: Image processing techniques
were used to enhance magnetic data generated by SQUID
nondestructive evaluation of conducting plates. The process
consists of low-pass filtering the acquired data with a FIR
filter with order depending on the standoff distance and
background noise. In addition a high-pass FIR filter is used
to enhance the magnetic field disturbance due to the flaw. The
technique was tested on magnetic field data generated through
a dc current applied to flawed aluminum test samples, and
detected by using an RF-SQUID system. It was observed that
when the standoff distance exceeds 5 times the size of the
flaw, image inspection is difficult. Applying the enhancement
algorithm, magnetic field disturbances could be visualized at
distances 10 times the size of the flaw. |
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Measurements
of surface-breaking flaws in ferromagnetic plates by means of
an imaging SQUID
susceptometer A.C. Bruno, A.P.
Ewing and J.P. Wikswo Jr.
Summary: We
detected sub-millimeter surface-breaking flaws in
ferromagnetic plates using an imaging SQUID susceptometer. The
normal component of the field was imaged with an axial, first
order gradiometer with 3 mm diameter coils and a 4 cm
baseline. We mapped the field above mild steel test samples,
detecting field distortions due to surface flaws with volumes
as small as 0.1 cubic millimeter. A comparison is made with
conventional flux leakage methods. Our method of observing
distortions in a perpendicularly applied field may be more
sensitive for detecting surface-breaking flaws. Image
enhancement techniques successfully removed background signals
with low spatial frequencies. |
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Magnetomechanical
behavior of steel via SQUID
magnetometry J. Banchet, J.
Jouglar, P.-L. Vuillermoz, P. Waltz and H.
Weinstock
Summary: Steel bars were subjected
to stress-strain hysteresis cycles in a horizontal
tensile-testing machine while changes in the vertical
component of the magnetic field above these bars was recorded
by a DC SQUID second-order gradiometer. Magnetic Barkhausen
noise was observed after repeated cycling and especially at
stress levels for which the magnetic field was at an extremum
value. Of greatest practical interest is the fact that the
area of the magnetomechanical hysteresis loop (/spl Delta//spl
Phi//sub z/-/spl sigma/) increased dramatically-by orders of
magnitude-over a large number (up to 10/sup 5/) of fatigue
cycles. This may have important implications for the in situ
nondestructive evaluation of steel. |
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Eddy
current evaluation of airframes using refrigerated
SQUIDs W.N.
Podney
Summary: A superconductive quantum
interference device, RF SQUID, fixed to the cold pad of a
Heliplex HS-4 refrigerator shows a baseline noise of 1.6/spl
times/10/sup -4/ flux quanta in a one hertz bandwidth at
frequencies above about 25 Hz. The refrigerator adds noise
below 25 Hz. Remote pickup loops couple flux to the SQUID
through a cryogenic umbilical, 500 mm long, attached to the
cold pad. It enables scanning a 100/spl times/100 millimeter
section of airframe without moving the expander, which
connects to compressors through flexible gas lines 3 m long.
Thermal conduction through copper braiding in the umbilical
keeps pickup loops at 5.5 K, 3 mm from an airframe at ambient
temperature. Drive currents of a few amperes, oscillating at
one to three hundred Hertz enable identifying 5 to 10 percent
material loss through 10 to 15 mm of aluminium. |
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Integrated
LTS gradiometer SQUID systems for measuring of magnetic field
distributions in an unshielded
environment P. Weber, V.M.
Zakosarenko, K.-H. Berthel, K. Bluthner, J. Schambach, L.
Warzemann, G. Kirsch, T. Dohler and R.
Stolz
Summary: Planar dc SQUID gradiometers
with integrated antenna were designed for measurement of field
distributions with gradients much smaller than 1 pT/cmHz/sup
1/2/ in an unshielded environment. Four types of
first-order-gradiometer SQUIDs were fabricated in Nb-Pb
technology and investigated. Their layouts are highly
symmetrical and they can be made also with HTS materials.
Further reduction of the effect of disturbances was achieved
with a second order gradiometer realized electronically. The
stable function of the systems under unshielded conditions is
shown. |
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Study
of DyBaCuO DC SQUIDs for low noise and high flux
focusing Y. Higashino and T.
Umezawa
Summary: We have fabricated DyBaCuO
DC SQUIDs by MBE growth on MgO substrates containing 45/spl
deg/ step-edge Josephson junctions. They showed RSJ-like
current-voltage characteristics and periodic modulation of
voltage aroused by an applied magnetic field at 77 K. The flux
resolution of the 1.9 mm square washer SQUID was measured to
3/spl times/10/sup -4/ /spl Phi//sub 0//Hz/sup 1/2/ at 1 Hz,
which corresponds to a magnetic field sensitivity of 14
pT/Hz/sup 1/2/. Effective flux capture areas were investigated
for varying SQUID size of washer and hole. |
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Microwave
performance of YBa/sub 2/Cu/sub 3/O/sub 7-x/ resonators
coupled to single-junction
SQUIDs M.A. Hein, S. Schmoe, M.
Strupp, H. Piel, Y. Zhang and A.I.
Braginski
Summary: The effects of microwave
current and dc magnetic field on quality factor and resonant
frequency at 3 GHz of planar resonators, which were
differently coupled to hysteretic microwave SQUIDs, are
discussed. The dissipative response is analyzed in terms of a
single-junction SQUID, and its coupling to a resonant tank
circuit. The temperature dependences and field periodicities
of all relevant parameters are discussed, and conditions for
optimized operation are deduced. The results indicate
potential for further improvement of the performance of
microwave SQUID magnetometers. |
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Reproducible
step-edge junction SQUIDs Y.Q.
Shen, Z.J. Sun, R. Kromann, T. Holst, P. Vase and T.
Freltoft
Summary: High-T/sub c/
superconducting YBCO SQUIDs have been developed based on
step-edge junctions. The step-edges were fabricated by using
electron-beam lithography and Ar-ion milling on SrTiO/sub 3/
substrates. The V(/spl Phi/) peak-to-peak voltage is around 10
/spl mu/V, and the I/sub c/R/sub n/ product is 150 /spl mu/V
at 77 K. The SQUIDs prepared on the same substrate show
reproducible parameters within 30%. At 77 K the noise
properties of the SQUIDs have been studied. At lower
frequencies (1 Hz-100 Hz), we observe a flat noise level just
below 10/sup -4//spl Phi//sub 0//Hz/sup 1/2/ probably limited
by switching effects. Above 100 Hz the noise is gradually
reduced to 10/sup -5//spl Phi//sub 0//Hz/sup 1/2/ at 1 kHz.
The geometry of the step-edges has also been investigated by
scanning electron microscopy, and the relation between the
properties of the SQUID and the step height is
reported. |
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High
T/sub c/ SNS step-edge junctions and SQUIDs by using; YBa/sub
2/Cu/sub 3/O/sub 7//CaRuO/sub 3/ double
layer Soon-Gul Lee, Keunseop
Park, Hyuk Chan Kwon, Yong Ki Park, Jong-Chul Park and Doo-Sup
Hwang
Summary:
Superconductor-normal-superconductor (SNS) step-edge
junction dc SQUIDs were fabricated from YBa/sub 2/Cu/sub
3/O/sub 7/ (YBCO) films with CaRuO/sub 3/ (CRO) on top as the
normal metal. The films were made by pulsed laser deposition
(PLD) and patterned by photolithography and ion milling. The
junctions and SQUIDs had to be annealed in oxygen environment
for a much longer period of time (5-48 hours) compared with
standard YBCO film preparation (as deposited or 1 hour),
indicating that the top CRO film blocks oxygen in and out of
the YBCO film. Before annealing T/sub c/'s of CRO/YBCO double
layers and junctions made from them were <70 X and <50
K, respectively, and increased to >88 K and >77 K,
respectively after long time annealing. Current-voltage curves
of the junctions showed well-behaved
resistively-shunted-junction (RSJ) properties and the
temperature dependence of the junction critical current was
roughly linear. SQUIDs made of those junctions showed voltage
modulation in response to applied fields at 77
K. |
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High
T/sub c/ bi-epitaxial junctions and dc SQUIDs structured by
focused ion beam etching R.P.J.
Ijsselsteijn, J.W.M. Hilgenkamp, D. Velhhuis, J. Flokstra, H.
Rogalla, C. Traeholt and H.W. Zandbergen
Summary:
Focused ion beam etching has been used to pattern dc
SQUIDs into previously characterised template bi-epitaxial
grain boundary junctions. Using this technique the screening
parameter /spl beta//sub L/ can be optimised for a chosen
temperature (in our case 30 K). Electrical characteristics,
including noise measurements, are presented. A minimal white
noise level of 22 /spl mu//spl phi//sub 0//spl middot/Hz/sup
-1/2/ (1.8/spl middot/10/sup -29/ J/spl middot/Hz/sup -1/) has
been obtained at 20 K. Using bias current modulation the 1/f
noise could almost completely be suppressed down to 1 Hz in
the entire temperature range (10-65 K). |
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Optical
diagnostics for fabrication of YBCO thin film DC
SQUIDs A.N. Obraztsov, A.G.
Maresov, I.I. Vengrus, O.V. Snigirev and S.I.
Krasnosvobodtsev
Summary: Optical reflectance
spectra of thin YBCO films on SrTiO/sub 3/ bicrystals were
measured in a photon energy range of 1-3 eV at room
temperature. Raman spectra measurements in the range 200-700
cm/sup -1/ were performed. The best samples were shown to have
high reflectance anisotropy and a well-defined Raman peak /spl
nu//sub 1/=500+1 cm/sup -1/. YBCO thin films on a bicrystal
substrate that successfully passed optical control were used
for Josephson junctions and DC SQUID fabrication. The
fabricated SQUIDs operated at 77.3 K in the flux locked loop
mode and had a typical white noise (1-2)/spl times/10/sup -5/
/spl Phi//sub 0//Hz/sup 1/2/ at frequencies higher than
200-500 Hz. The best magnetic field resolution was 650
fT/Hz/sup 1/2/ at frequencies f>200 Hz. |
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Normal-state
properties and Josephson effects in HTS weak links produced by
electron beam S.K. Tolpygo, S.
Shokhor, B. Nadgorny, J.-Y. Lin, M. Gurvitch, S.Y. Hou and
J.M. Phillips
Summary: A description is given
of the fabrication method and Josephson properties of high
temperature superconducting junctions produced by focused
electron beam writing. The nature of a weak link, I-V
characteristics, transition to flux flow, and magnetic field
modulation are discussed in some detail. The materials aspects
such as the mechanism of e-beam damage to HTS, threshold
energy, junction stability, and some technological issues such
as reproducibility and uniformity are also
addressed. |
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Current-voltage
characteristics of shunted Josephson weak links with excess
current R.G. Seed, C. Vittoria
and A. Widom
Summary: Many superconducting
Josephson weak link junctions are not adequately or accurately
modeled by the resistively shunted junction model. For point
contact junctions, step edge junctions and grain boundary
junctions, a large excess current in the I-V characteristic is
often observed. A new model has been proposed, which provides
a more accurate technique of describing the behavior. Using
this theory of shunted weak link junctions with excess
current, calculations are presented here which accurately
describe the magnitude and position of microwave induced
current steps in the dc current versus voltage characteristics
of such devices. |
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Progress
in understanding the physics of HTS Josephson
junctions M.Y. Kupriyanov and
J.S. Tsai
Summary: The experimental results
obtained in high-T/sub c/ Josephson junctions are reviewed
with the emphasis on intrinsic Josephson effect and long-range
proximity effect junctions (LRPJ). The possibility of the
experimental observation of the intrinsic Josephson effect is
discussed. A theoretical model based on resonant tunneling via
localized states is proposed for the description of normal and
supercurrent flow in LRPJ. |
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Optical
response of superconducting Nd/sub 1.85/Ce/sub 0.15/CuO/sub
4-y/ and YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// thin
films S. Bhattacharya, S.N. Mao,
M. Rajeswari, W. Jiang and T. Venkatesan
Summary:
The normal state and transition edge optical response
of epitaxial thin films of n-type superconductor Nd/sub
1.85/Ce/sub 0.15/CuO/sub 4-y/ has been measured. In contrast
to the optical response of p-type superconductors such as
YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// the normal state
optical response of these films were not proportional to the
temperature derivative of the resistance. The normal state
optical response of films with different transition
temperature (and, therefore, different oxygen content) were
also remarkably different from each other. We attribute the
observation of anomalous optical response to the possible
presence of photoconductivity in Nd/sub 1.85/Ce/sub
0.15/CuO/sub 4-y/. We also discuss the feasibility of
fabricating bolometers based on superconducting p-n
bilayers. |
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Temperature
dependence of the Josephson critical current in Bi/sub
2/Sr/sub 2/CaCu/sub 2/O/sub 8+x/ break
junctions R.S. Gonneli, I.
Puttero, G.A. Ummarino and V.A. Stepanov
Summary:
We measured the I-V characteristics of break junctions
obtained at 4.2 K in single crystals of Bi/sub 2/Sr/sub
2/CaCu/sub 2/O/sub 8+x/ that exhibited a stable nonhysteretic
Josephson effect. The product I/sub c/R/sub N/ at 4.2 K was
about 10 mV and the I-V curves followed the Resistively
Shunted Junction (RSJ) model up to the T/sub c/ of the
crystals. The temperature dependence of the critical current
I/sub c/(T) is fitted by a new model that takes into account
the effect of an intrinsically depressed order parameter at
the surface of a superconductor with a short coherence length
and, for comparison, by a model that introduces the effect of
a proximity layer and of a finite transparency at the junction
interfaces. The results can indicate that the intrinsic
lowering of the pair potential at the sample surfaces is the
cause of the deviations of our I/sub c/R/sub N/ from ideal BCS
value. |
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Low
magnetic field sensitivity of c-axis transport in BSCCO (2212)
single crystals Ji Ung Lee, G.
Hohenwarter, R.J. Kelley and J.E. Nordman
Summary:
We have examined the sensitivity to low magnetic fields
of c-axis transport in BSCCO (2212) bulk single crystals. A
uniform field is applied along the ab planes of a mesa
structure which was formed by etching. Four terminal
volt-ampere curves in liquid nitrogen show a field dependent
critical current and flux flow region followed by a multiple
branch region, suggestive of stacks of hysteretic
junctions. |
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Two-GHz
microstrip thin-film resonators of Nb and YBa/sub 2/Cu/sub
3/O/sub 7/ J.D. Goettee, W.J.
Skocpol, D.E. Oates and P.M. Mankiewich
Summary:
Dissipation and phase noise have been measured for
2-GHz linear microstrip resonators on 0.5-mm LaAlO/sub 3/.
Fifty-ohm YBCO resonators with Nb ground planes (YBCO/Nb)
showed quality factors of approximately 100,000 at 2 GHz and
4.2 K, somewhat less than measured in all-Nb resonators of the
same geometry. The corresponding surface resistance of 10
microhms was maintained to average current densities of 1
MA/cm/sup 2/. All-YBCO resonators were measured to higher
temperatures, and showed significant excess dissipation above
about 60 K. The normalized phase noise of S/sub y/=-20/spl
plusmn/2 was maintained to at least 30 K. This resonator was
also operated in a resonator-stabilized oscillator
configuration. The effect of package interactions on
microstrip devices was also investigated. |
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Passivation
of YBaCuO coplanar microwave
structures E. Waffenschmidt, J.
Musolf, Xiaoyin He, K. Heime, S. Hofschen and I.
Wolff
Summary: Thin layers of Al/sub 2/O/sub
3/ and SiO/sub x/ were examined as dielectric passivations for
thin films and coplanar microwave structures made of YBaCuO.
The efficiency of the 300 nm thick material was shown by
measuring the microwave surface resistance R/sub S/ (24.5 GHz,
77 K) of passivated YBaCuO layers before and after heat
treatment in inert atmosphere. No significant changes were
observed after heating for 1 h at 200/spl deg/C, whereas R/sub
S/ of an unprotected sample increased strongly. After 1 h at
300/spl deg/C R/sub S/ of the passivated samples increased
from 10 m/spl Omega/ to values between 70 m/spl Omega/
(SiO/sub x/) and 270 m/spl Omega/ (Al/sub 2/O/sub 3/) while
the unprotected samples lost their superconductivity, The
degradation was mainly caused by loss of oxygen, since the
unprotected sample could be recovered by annealing in O/sub 2/
at 650/spl deg/C. The effect on the properties of microwave
structures was calculated and measured using 25 /spl mu/m wide
coplanar line resonators on LaAlO/sub 3/ at 5 GHz. No
significant change of the quality factor was found after
coating the structure with 300 nm SiO/sub x/ and Al/sub
2/O/sub 3/. The shift of the resonance frequency was less than
1%. The performance of a higher order filter showed
neglectable change. |
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Temperature
dependence of surface impedance of pulsed-laser-deposited YBCO
films J.H. Clark, G.B. Donaldson,
J.C. Gallop and R.M. Bowman
Summary: One
promising application of HTS materials is as the reference
resonator element for a stable frequency source. A high Q
superconducting resonator operated at low reduced temperature
(T/T/sub c//spl Lt/1) should offer excellent frequency
stability due to its low temperature coefficient of resonant
frequency. HTS planar resonators appear to be particularly
promising since a reduced temperature of 0.1 may be readily
achieved with a closed-cycle cryocooler. We report here
microwave measurements made on YBCO films grown by pulsed
laser deposition (PLD), using both a Nb cavity and a
parallel-plate resonator configuration, with particular
emphasis on the variation of resonant frequeney with
temperature. We compare the data with simple theoretical
models and find evidence from the low temperature data for a
low energy gap parameter /spl Delta/(0)=6 meV. Some
predictions of attainable frequency stability of planar
resonator structures are also made. |
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YBCO
X-band microstrip linear resonators on (1I02)- and
(1I00)-oriented sapphire
substrates C.H. Mueller, F.A.
Miranda, S.S. Toncich and K.B. Bhasin
Summary:
YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// (YBCO) films on
sapphire substrates have been tested for planar microwave
applications such as filters and resonators. We have measured
the unloaded quality factors (Q/sub 0/) of X-band microstrip
linear resonators patterned into YBCO films on R-plane
(1I02-oriented) and M-plane (1I00-oriented) sapphire
substrates with CeO/sub 2/, and MgO buffer layers,
respectively. For the fW on M-plane sapphire, the T/sub c/ and
x-ray FWHM values were 87-88 K and 1.2/spl deg/, respectively,
while for those on R-plane sapphire the values were 88-89 K
and 0.4/spl deg/. Despite the superior properties of the film
on R-plane, the YBCO on M-plane sapphire resonators had Q,
values over 2000 at 77 K while those on R-plane sapphire had
Q, values of less than 600. This could be correlated with the
anisotropy of the R-plane sapphire as evidenced by the
observed dependence of the shape of the resonance on the
orientation of the resonator relative to the in-plane
direction of the substrates. Possible causes for this behavior
will be discussed. |
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Fabrication
of YBCO superconducting dual mode resonator for satellite
communication Sang Yeol Lee,
Kwang Yong Kang and Dal Ahn
Summary:
Superconducting YBa/sub 2/Cu/sub 3/O/sub 7-x/ (YBCO)
thin films have been grown epitaxially on (100) MgO substrates
of laser ablation technique. Superconducting properties of
YBCO thin films on MgO substrates have been investigated by
X-ray diffraction pattern, scanning electron microscope,
transport and magnetized T/sub c/ measurements.
Superconducting dual mode disk resonators were designed by
microwave design software, EEsof and fabricated by
photolithography and wet-etch process using YBa/sub 2/Cu/sub
3/O/sub 7-x/, superconducting thin films with T/sub c/ of 87
K. The unloaded quality factor of the superconducting dual
mode disk resonator was measured to be 1312 at 77 K by a
HP8510B vector network analyzer. A clear resonant frequency
splitting in the frequency range of 7.7-9.7 GHz was observed
in a perturbed dual mode disk resonator. This type of dual
mode disk resonator could be utilized as a dual mode resonator
filter for satellite communication. |
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Role
of perturbations for dual mode superconducting microstrip
resonators fabricated by laser
ablation Sang Yeol Lee, Kwang
Yong Kang and Dal Ahn
Summary: The comparison
of frequency response characteristics between various types of
superconducting dual mode resonators has been performed.
Epitaxial superconducting YBa/sub 2/Cu/sub 3/O/sub 7-x/ (YBCO)
thin films have been have been grown on MgO substrates by
laser ablation. Perturbed disk and ring types of
superconducting dual mode resonators were patterned by
photolithography and a wet-etch process. Unlike the
unperturbed case, dual mode resonators have different resonant
properties for the perturbed case depending on the position of
the perturbation. We observed the same resonant peak splitting
properties at the fundamental resonances of the perturbed dual
mode disk and ring resonators. Peak properties caused by
perturbation in the dual mode resonators could be used in
implementing a two pole bandpass filter by
itself. |
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Effects
of microstructures on microwave properties in Y-Ba-Cu-O
microstrip-resonators T.
Yoshitake, H. Tsuge and T. Inui
Summary: We
examined the microwave properties of YBa/sub 2/Cu/sub 3/O/sub
x/ films with different microstructures at 5.7 GHz using a
microstrip resonator technique. The films were prepared with
several types of substrate temperature profiles. Films with
small grains (/spl sim/100 nm) and larger critical current
density show fairly small rf magnetic field dependence of
surface resistance and resonance frequency up to about 50 Oe.
On the other hand, films with large grains (/spl sim/200 nm)
and smaller critical current density show significant changes
in these properties. These results suggest that the coupling
strength at the grain boundaries mainly dominates the power
handling capability, according to a qualitative explanation
based on the coupled-grain model. |
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Ferroelectric
thin film characterization using superconducting microstrip
resonators D. Galt, J.C. Price,
J.A. Beall and T.E. Harvey
Summary: We
describe a novel technique for characterizing the dielectric
response of ferroelectric thin films at microwave frequencies.
The method involves a microstrip resonator which incorporates
a ferroelectric capacitor at its center. To demonstrate this
method rye have fabricated a superconducting microstrip
resonator from a laser-ablated YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta// (YBCO) film on a LaAlO/sub 3/ (LAO) substrate with a
SrTiO/sub 3/ (STO) capacitor at its center. We report the
observed dielectric behavior of the STO laser ablated film as
a function of bias at liquid He and N/sub 2/ temperatures and
at high and low frequencies. It is observed that the
electrically tunable dielectric constant of the STO film is
roughly independent of frequency up to 20 GHz (especially at
high bias). The loss tangent of the STO/LAO capacitor
decreases with increasing bias and is apparently independent
of frequency between 6 and 20 GHz. |
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Nonlinear
thermal effects in the HTSC microwave stripline
resonator A.N. Reznik, A.A.
Zharov and M.D. Chernobrovtseva
Summary: We
report a theoretical study of nonlinear electromagnetic
phenomena for HTSC stripline resonators. We have considered a
thermal nonlinearity resulting from heating of HTSC by
electromagnetic field. It was shown that a microwave input
power excess of some threshold level leads to formation of a
normal-state domain. We have obtained that emergence and
disappearance of the domain have a hysteresis character with
respect to the input power which provides a hysteresis for the
transmission coefficient and frequency response. |
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Quantum
detectors in superconducting
YBCO N. Bluzer and M.G.
Forrester
Summary: A superconducting quantum
detector structure in YBCO is described with a directly
coupled SQUID read out circuit. The detector geometry is
optimized for maximum photoresponse with the use of a
serpentine pattern. The serpentine pattern reduces
quasiparticle diffusion effects and maximizes the photoinduced
changes in the kinetic inductance. The operation of this
sensor is analyzed in terms of geometry and quasiparticle
lifetime to obtain expressions for the signal and noise of
this detector. The background limited infrared performance of
this detector is calculated to be about 5/spl times/10/sup
-17/ NEP. The photoresponse is expected to be limited by the
superconducting energy gap, about 30-40 /spl
mu/m. |
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Nonbolometric
NbN photodetector M.W. Johnson,
A.M. Domino and A.M. Kadin
Summary: There
have been several recent reports of apparently nonbolometric
optical responses in superconducting thin films. The
photoresponse of 10 nm thin superconducting NbN meander lines
on Si is measured at 670 nm using a diode laser modulated to
more than 100 kHz. Several types of photoresponse are
identified, some apparently due to the Si substrate. A fast
photoresponse due to the NbN film with a responsivity of up to
125 V/W of absorbed power was observed. Results are analyzed
in the context of a bolometric model, and the magnitude of the
photoresponse is found to be too large for a purely bolometric
response. Possible nonbolometric alternatives are
discussed. |
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Nonequilibrium
kinetic inductive response of YBCO thin films to low power
laser pulses G. Gol'tsman, P.
Kouminov, I. Goghidze and E. Gershenzon
Summary:
We have discovered a transient nonequilibrium kinetic
inductive voltage response of YBCO thin films to 20 ps pulses
of YAG:Nd laser radiation with 0.63 /spl mu/m and 1.54 /spl
mu/m wavelength. By increasing the sensitivity of the read-out
system with 100 ps resolution time and diminishing the light
intensity (fluence 0.1-2 /spl mu/J/cm/sup 2/) and transport
current (density /spl les/10/sup 5/ A/cm/sup 2/) we were able
to observe a peculiar bipolar signal form with nearly equal
amplitudes for each sign. The integration of the kinetic
inductive response over time gives the result which is
qualitatively, of the same form as the response in the
resistive and normal states: the nonequilibrium picosecond
scale component is followed by the bolometric nanosecond
component. The nonequilibrium response is interpreted as
suppression of the order parameter by excess quasiparticles
followed by a change both in resistance (for the resistive
state) and in kinetic inductance (for the superconducting
state). |
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Nonthermal
kinetic inductance photoresponse of thin superconducting
films M.A. Heusinger, A.D.
Semenov, R.S. Nebosis, Y.P. Gousev and K.F.
Renk
Summary: We report on the photoresponse
of structured superconducting YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta// and NbN films to femtosecond visible light pulses. The
photoresponse signals obtained at temperatures below the
transition temperature consist of a positive voltage peak of
25 ps width for the YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
sample and 40 ps for the NbN sample, each limited by the
temporal resolution of the different setups, followed by a
longer negative voltage transient. We attribute the
photoresponse signals to a nonthermal change of the kinetic
inductance of the superconducting films. We also present a
model describing the dynamics of nonequilibrium quasiparticles
(QP) and phonons, allowing to simulate our results. Our model
provides the physical background for optimization of fast
detectors based on the kinetic inductance photoresponse of
thin superconducting films. |
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Quantum
effects in the hot electron
microbolometer A. Tang and P.L.
Richards
Summary: The theory of the hot
electron microbolometer proposed by Nahum et al. assumed that
the photon energy is thermalized in the electrons in the Cu
absorber before relaxing to the lattice. Since the photons
initially excite individual electrons to /spl planck//spl
omega//spl Gt/k/sub B/T, however, direct relaxation of these
hot electrons to phonons must also be considered, Theoretical
estimates suggest that this extra relaxation channel increases
the effective thermal conductance for /spl planck//spl
omega//spl Gt/k/sub B/T and influences bolometer noise.
Calculations of these effects are presented which predict very
useful performance both for ground-based and space-based
astronomical photometry at millimeter and submillimeter
wavelengths. |
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The
single-electron transistor as an ultrasensitive microwave
detector J.M. Hergenrother, J.G.
Lu and M. Tinkham
Summary: We have measured
single-electron tunneling transistors with superconducting
islands and conclude that they may be used as ultrasensitive
detectors of microwave radiation for frequencies /spl ges/80
GHz. These devices contain a small superconducting Al island
that is weakly coupled to a bias circuit through two
small-capacitance tunnel junctions and a capacitive gate. At
low bias voltages and temperatures, a single quasiparticle may
only be introduced to the island through photon-assisted
tunneling. Once this occurs, the quasiparticle is trapped on
the island for /spl sim/1 /spl mu/s because it takes a
relatively long time for this specific quasiparticle to tunnel
off. While it is trapped, charge is transported through the
system two electrons at a time. Since the photon-assisted
transition merely switches the detector current on, this
device is not limited to one electron tunneled through the
system per absorbed photon. Measurements indicate that at
least 100 electrons can tunnel for every absorbed photon,
which corresponds to a noise-equivalent power of 3/spl
times/10/sup -20/ W//spl radic/Hz at 80 GHz if the current is
measured with a commercial current amplifier. |
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Application
of Josephson edge type junctions with a PrBa/sub 2/Cu/sub
3/O/sub 7/ barrier prepared with Br-ethanol etching or
cleaning M.I. Faley, U. Poppe,
C.L. Jia, U. Dahne, Yu. Goncharov, N. Klein, K. Urban, V.N.
Glyantsev, G. Kunkel and M. Siegel
Summary:
The technique of the edge preparation for multilayer
Josephson edge type junctions on the basis of c-axis oriented
YBa/sub 2/Cu/sub 3/O/sub 7/ thin films with the help of
etching in Br-ethanol solution was improved. Microwave induced
Shapiro steps, Josephson radiation, and characteristics of
dc-SQUIDs were investigated. The developed technique prevents
the junctions and device properties from degradation due to
aging or thermal cycling. |
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Resonant
tunneling transport in YBaCuO/PrBaCuO/YBaCuO edge-type
Josephson junctions T. Satoh,
M.Y. Kupriyanov, J.S. Tsai, M. Hidaka and H.
Tsuge
Summary: YBaCuO/PrBaCuO/YBaCuO
edge-type Josephson junctions were fabricated and their
transport properties were studied. Josephson effect in these
structure was confirmed by the observation of microwave
induced Shapiro steps and periodic magnetic field dependence
of the critical current. Normal electron transport in the
junctions was well explained by Glazman and Matveev's theory
for hopping transport via localized states. In addition, the
supercurrent transport in PrBaCuO is possibly supported by the
resonant tunneling via the localized states. We estimated the
density of the localized states to be 10/sup 16/ cm/sup
-3/. |
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Fabrication
of field effect devices based on YBaCuO/PrBaCuO/YBaCuO
junctions H. Kimura, Y. Okabe and
H. Kamijo
Summary: In order to investigate an
electric field effect in the junction, the three terminal
device was fabricated. When the gate voltage of +2 V (E=7/spl
times/10/sup 4/ V/cm) was applied, the drain-source resistance
decreased above the temperature of 100 K. However, the
electric field effect could not be observed below the
temperature of 100 K. Above the temperature of 100 K, it is
found that the CuO chain in PBCO behaved itself as a doped
semiconductor (acceptor level=26.5 meV). |
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Properties
of multilevel ramp edge junctions and SQUIDs with
laser-ablated SrTiO/sub 3/
barriers R.B. Laibowitz, J.Z.
Sun, V. Foglietti, R.H. Koch, R.A. Altman and W.J.
Gallagher
Summary: We have fabricated
junctions and DC SQUIDs using laser ablation for both the YBCO
electrodes and the thin SrTiO/sub 3/ (STO) barrier regions in
a variety of device configurations. These SQUIDs operate
reliably at 77 K and preliminary results on a limited number
of devices show that they store reasonably well for periods in
excess of one year, and exhibit only small changes with
repeated cycles (/spl sim/10) between room temperature and 77
K. Noise measurements made using bias reversing on a SQUID (92
pH) at 77 K give a white noise of about 15 /spl mu//spl
Phi//sub 0///spl radic/Hz and a 1/f upturn at about 0.2
Hz. |
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Fabrication
of YBaCuO/nonsuperconductive-YBaCuO/YBaCuO co-planar Josephson
junction by focused ion beam Y.
Soutome, Yunn Ghee Gheem and Y. Okabe
Summary:
A thin film of YBa/sub 2/Cu/sub 3/O/sub 7/(-/spl
delta/) grown on an MgO substrate damaged by a focused ion
beam loses superconductivity due to abnormal growth. We have
fabricated a YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// co-planar
Josephson junction whose coupling region is nonsuperconductive
YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// grown on an MgO
substrate damaged locally by focused ion beam scanning. The
I-V characteristic of the junction behaves like a flux flow
type. At temperatures from 4.2 K to 60 K, Shapiro steps were
observed for the junctions in which the length of the coupling
region was from 0.2 /spl mu/m to 1 /spl mu/m. The highest
I/sub c/R/sub n/ product of the junction was 5.0 mV. The
critical current density decreased exponentially with the
junction length. It is considered that nonsuperconductive
YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// grown on the damaged
substrate works as a normal layer in an S-N-S junction. Also
the junction responded to the magnetic field and behaved like
an asymmetric dc-SQUID. |
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Modeling
of an ADC based on high-T/sub c/ QOJS
comparators T. Harnisch, F.H.
Uhlmann, H. Topfer, D.F. Moore, A.J. Pauza and K.
Lamacraft
Summary: Existing proposals for
high temperature superconductor analog to digital converter
(ADC) circuits suffer performance penalties because of the
difficulty of fabricating devices with small and controlled
inductances. The design of a quasi-one junction SQUID (QOJS)
comparator for a high-T/sub c/ flash ADC is proposed and
discussed. The inductances are calculated with the help of a
three-dimensional field calculation program, and simulations
on the QOJS-comparator are performed using a SPICE-type
simulation program. |
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A
proposal of Josephson binary-to-ternary
converter Fu-Qiang Li, M. Morisue
and T. Ogata
Summary: This paper presents a
novel Josephson converter to perform signal conversion from a
binary system to a ternary system. Most converters perform
conversion in successive steps from the least significant bit
to the most significant bit. Therefore, the circuits become
complicated and operation speed becomes low. In order to
overcome these shortcomings, a novel converter based on
Josephson technology is proposed. The principle of the
converter is described in detail and simulation results for an
8-bit converter are illustrated. The advantages of this
converter are simple construction with a small number of
elements and high speed operation. |
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Performance
of MVTL logic at multi-GHz
frequencies M. Leung, J.W.
Spargo, B.J. Dalrymple, D.J. Durand, M.S. Wire and A.
Spooner
Summary: Demonstrating
superconductive logic circuits at high speeds is crucial in
gaining acceptance by potential users. We are taking an
integrated approach toward demonstrating the potential of such
circuits. Issues addressed include the effects that layout
have upon a circuit and gate (particularly in scaling down the
size of gates to increase density), testing limitations,
designing for minimum crosstalk and ground ripple, and
fundamental limitations to gate performance. In this paper, we
report our progress in resolving and understanding these
issues. Circuits such as shift registers were used to
understand the influence of layout on performance, circuits
such as gate chains and punchthrough detectors to explore
fundamental gate limitations. We also report on signal
processing circuits of several hundred gates tested at clock
frequencies up to several hundred MHz and the relationship
between these results and the fundamental gate
performances. |
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CMOS
amplifier designs for Josephson-CMOS interface
circuits U. Ghoshal, S.V.
Kishore, A.R. Feldman, Luong Huynh and T. Van
Duzer
Summary: We discuss the design of CMOS
amplifiers for Josephson-CMOS interface circuits in three
different application scenarios, these circuits form important
building-blocks of Josephson-CMOS memories, A/D converters
(ADC), and other novel circuits, all these designs have been
implemented in the UC Berkeley Josephson-CMOS
technology. |
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CMOS
self-calibration of Josephson flash-type A/D
circuits S.V. Kishore, U.
Ghoshal, L. Huynh and T. Van Duzer
Summary:
We present CMOS self-calibration and bias circuits for
Josephson circuits. In Josephson technology, process
variations in critical circuit parameters such as junction
critical current, resistance, and inductance adversely affect
the performance. For example, process deviations in junction
critical currents leads to low dynamic range and nonuniform
quantization steps in flash-type A/D converters. While CMOS
technology has a speed disadvantage with respect to Josephson
technology, it does make available highly accurate current
sources that are relatively process independent and difficult
to obtain in Josephson technology. Here, we discuss how the 4
K CMOS self-calibration of a Josephson flash type A/D
converter can be used to improve dynamic range. |
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Hybrid
Josephson-CMOS FIFO A.R. Feldman
and T. Van Duzer
Summary: We describe the
design of a hybrid Josephson-CMOS first-in-first-out memory
(FIFO) for communications and signal processing applications.
The FIFO takes advantage of high speed Josephson logic and
dense CMOS memory. We focus on the low power CMOS ring pointer
architecture employing a dual-port CMOS SRAM array and
illustrate how a high speed Josephson
demultiplexor-multiplexor pair can greatly increase
throughput. We describe a novel eight transistor dual-port
CMOS SRAM cell with low swing write and current-mode read with
an asymmetric SQUID to perform differential current-sensing.
Finally, we discuss the peripheral Josephson demultiplexor and
multiplexor designed in edge-triggered logic. |
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High-power
high-temperature superconducting microstrip filters for
cellular base-station
applications G.-C. Liang, D.
Zhang, C.-F. Shih, M.E. Johansson, R.S. Withers, A.C. Anderson
and D.E. Oates
Summary: We report narrowband
microstrip filters with low insertion loss and high
power-handling capabilities made from YBa/sub 2/Cu/sub 3/O/sub
7/(-x) high-temperature superconducting films. One 5-pole
filter on a LaAlO/sub 3/ substrate, consisting of
backward-coupled and forward-coupled resonators, can handle
over 27 W input power at 10 K. It has 1% fractional bandwidth
and 10-/spl Omega/ internal impedance. The insertion loss
increase in passband at 10 K, as the input power changed from
a few mW to 27 W, is less than 0.25 dB. We also report a
forward-coupled microstrip filter centered at 2 GHz, with a
1.2% fractional bandwidth, 10-/spl Omega/ internal impedance,
and parallel-coupled feed lines. We applied over 10 /spl
Omega/ to the filter at 45 K without noticeable degradation of
the filter performance. The insertion loss at 45 K is less
than 0.2 dB. The return loss is better than 12
dB. |
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Compact
forward-coupled superconducting microstrip filters for
cellular communication Dawei
Zhang, G.-C. Liang, C.F. Shih, R.S. Withers, M.E. Johansson
and A.D. Cruz
Summary: A compact
forward-coupled microstrip filter structure is presented for
narrow-band applications in cellular communications. The
structure consists of a parallel array of fully aligned
half-wavelength resonators. Coupling is controlled by the
spacing of the adjacent resonators, and is based on the even-
and odd-mode phase velocity difference of coupled lines in a
microstrip configuration. Two filter designs, based on the
forward-coupled structure, were fabricated using YBa/sub
2/Cu/sub 3/O/sub 7/ (YBCO) high-temperature superconducting
(HTS) thin films on LaAlO/sub 3/ substrates. One filter, a
9-pole 2.8% fractional-bandwidth YBCO filter at 900 MHz, has
less than 0.27 dB insertion loss and better than 16 dB return
loss. The other filter, a 5-pole 1.2% fractional bandwidth
YBCO filter with 10-/spl Omega/ internal impedance at 2 GHz,
has less than 0.35 dB insertion loss and better than 12 dB
return loss. All designs showed excellent measured frequency
response. |
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Applications
of high-T/sub c/ superconductors in sub-Gigahertz r.f. cavity
resonators A.E. Centeno and P.S.
Excell
Summary: The size of cavity resonators
below 1 GHz may be reduced by using dielectric or helical
loading. With normal conductors, such electrically small
resonators suffer problems of losses and inadequate Q-factor.
However, by using superconductor in the portions with the
highest current density, very good performance may be obtained
with very electrically-small cavities. A cylindrical
dielectric resonator was used to load a corrugated cavity,
having YBaCuO thick-film end plates, and operated at VHF. The
results showed a significant improvement over corrugated
cavities with copper end plates. Investigations have also been
undertaken with high-T/sub c/ superconductor helical loading.
The size of the cavities was electrically very small (about
0.02 of free space wavelength), and results with both bulk and
thick-film helical loading elements were obtained. The results
showed a significant improvement over a similar copper
helically-loaded cavity resonator. |
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YBCO
shielded LaAlO/sub 3/ dielectric resonators for stable
oscillators N. Klein, N.
Tellmann, T. Dahne, A. Scholen, H. Schulz, G. Hofer and H.
Kratz
Summary: We have investigated
dielectric resonators (SDROs) fabricated from single
crystalline LaAlO/sub 3/ shielded by two epitaxial films of
YBa/sub 2/Cu/sub 3/O/sub 7/ (YBCO). At the resonant frequency
of the TE/sub 011/-mode of 5.6 GHz unloaded quality factors
Q/sub 0/ of 8/spl times/10/sup 5/ at 20 K and 4/spl
times/10/sup 5/ at 60 K were obtained. These values were
limited by dielectric losses in LaAlO/sub 3/. At 50 K we
obtained a a Q/sub 0/ of 2/spl times/10/sup 5/ at a level of
dissipated rf power of 2 W corresponding to an average rf
magnetic surface field of 150Oe. Moreover, we used one SDRO as
a feedback for a HP8349 amplifier to measure oscillator phase
noise. At 60 K and helium gas cooling the phase noise was
beyond the sensitivity limit of our HP8565 spectrum analyzer
of about -90dBc/Hz at an offset frequency of 1 kHz. For
operation with Stirling coolers, microphonics dominates the
noise properties. |
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A
compact two-pole X-band high-temperature superconducting
microstrip filter B. Oh, H.T.
Kim, Y.H. Choi, S.H. Moon, P.H. Hur, M. Kim, S.Y. Lee and A.G.
Denisov
Summary: In this paper we examine a
microstrip line filter with three gaps separated by
approximately a quarter wavelength. Two filters, one with gold
and the other with YBCO were fabricated. The thickness of top
conducting microstrips was 600 nm. The ground plane under the
0.5 mm-thick lanthanum aluminate (LaAlO/sub 3/) substrate was
implemented with a 2 micron-thick gold layer for both filters.
These filters showed similar frequency responses with 5% 3-dB
bandwidth. The insertion loss, however, improved from 2.8 dB
to 1.5 dB by using the superconductor. The performance of the
filter was also tested by employing the three dimensional
microwave FEM software, and the simulation result compared
well with the measured data. |
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Microwave
multipole lowpass and bandpass filters fabricated by
high-T/sub c/ superconducting thin
films Kwang-Yong Kang, Sang Yeol
Lee, Seok Kil Han and Dal Ahn
Summary: The
design, fabrication, and measurement of 7-pole microstrip
lowpass filters and 4-pole parallel coupled-line bandpass
filters using superconducting YBa/sub 2/Cu/sub 3/O/sub 7-x/
epitaxial thin films are presented. The YBa/sub 2/Cu/sub
3/O/sub 7-x/ films were grown in situ at 770/spl deg/C and 200
mTorr oxygen partial pressure in a pulsed laser deposition
system. The 7-pole microstrip-line lowpass filter and 4-pole
parallel coupled-line bandpass filter patterned on the laser
ablated YBCO films with dimension of 20 cm/spl times/10 cm/spl
times/0.5 mmt were generated using photolithographic and wet
etching processes. The complete devices packaged in a
3-component type brass test-fixture were characterized. The
results showed the center frequency of 11.2 GHz with 6%
bandwith and less than 1 dB insertion loss(IL) for the case of
bandpass filters below 77 K. |
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Improvements
in superconducting linear phase microwave delay line bandpass
filters H.C.H. Cheung, G. Huang,
M.J. Lancaster, R.G. Humphreys and N.G.
Chew
Summary: Microwave delay line filters
can be designed to specified amplitude and phase
characteristics using a synthesis procedure which takes into
account multiple reflections and losses in the delay lines.
The time domain synthesis procedure has now been extended so
that frequency-dependent loss and delay line dispersion can
also be allowed for. Meanwhile experimental results on linear
phase microstrip and coplanar filters show significant
improvements on stopband attenuation and phase linearity over
previously published data on microstrip devices. |
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Fourier
spectroscopy study of Josephson junction own
radiation A.P. Lipatov, V.A.
Ilyin and A.A. Verevkin
Summary: The
frequency characteristics of Josephson own radiation have been
studied by means of Fourier spectroscopy. The FIR measurements
were performed with the help of Fourier spectrometer coupled
with the Nb Josephson junction. The main feature of this
technique is that one Josephson junction operates as both
generator and detector of own radiation at the same time. The
spectrometer operates either in double-beam mode with
resolution /spl sim/2 GHz or in multi-beam mode with
resolution /spl sim/1 GHz. |
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Modulation
of I-V characteristics of YBCO films and tunnel junctions
under microwave irradiation and tunnel current
injection Qian Wang, Kijin Lee
and Ienari Iguchi
Summary: We present the
measurements on the I-V characteristic modulation of YBCO
films under microwave irradiation and tunnel current
injection. In the case of tunnel current injection through a
Pb(or Au)/MgO/YBCO junction, the critical current I/sub c/ of
a YBCO film decreases drastically with the increase in tunnel
current, and a normal state appears when the injection current
reaches a certain value smaller than I/sub c/, leading to a
current gain greater than one. The I-V characteristics of a
YBCO film under both current injection and external microwave
irradiation (fa=11 GHz) show strong modulation behavior. We
find that the above modulation is mainly caused by the
Cooper-pair breaking effect due to injected quasiparticles
with energy greater than 2/spl Delta/ and not by
heating. |
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Quasioptical
Hilbert transform
spectrometer M.A. Tarasov, A.Ya.
Shul'man, G.V. Prokopenko, V.P. Koshelets, O.Yu. Polyanski,
I.L. Lapitskaya, A.N. Vystavkin and E.L.
Kosarev
Summary: A quasioptical spectrometer
using Hilbert transformation of Josephson junction response
has been designed, fabricated and experimentally studied.
Resistively shunted SIS junctions have been used as the
Josephson sensor placed in the centre of a complementary
logarithmic spiral antenna. The response was studied in the
75-150 GHz frequency band. A resolution below 1 GHz and noise
equivalent power about 10/sup -13/-10/sup -14/ W has been
measured for the 0.7 /spl Omega/ junction. The measured
spectrum is obtained by means of Hilbert transformation via a
novel deconvolution program based on the maximum likelihood
approach. This allows one to diminish the measured interval of
bias voltage and avoid measurements of the noisy part of the
response curve without loss of the spectral
resolution. |
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A
self-biasing cryogenic particle detector utilizing
electrothermal feedback and a SQUID
readout K.D. Irwin, S.W. Nam, B.
Cabrera, B. Chugg, G.S. Park, R.P. Welty and J.M.
Martinis
Summary: We are developing and
testing a new type of superconducting transition edge sensor
for phonon mediated particle detection. This sensor consists
of a superconducting tungsten thin film deposited on a silicon
substrate. The temperature of the film is held constant within
the superconducting transition (T/sub c//spl ap/70 mK) by an
electrothermal feedback process, while the substrate
temperature is well below the film temperature. Phonon energy
deposited in the film is removed by a reduction in feedback
Joule heating, which is measured using a series array of DC
SQUIDs. The resulting signals show improvements in linearity
and signal to noise ratio over our previous transition edge
sensors. |
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An
analysis of superconducting acoustic sensor with Josephson
junction Shu-Ang
Zhou
Summary: This article presents a
theoretical analysis of the effect of an elastic wave incident
upon a deformable Josephson junction, which is a basic
component of superconducting acoustic sensors. The model
introduced for the analysis is based on the generalized London
equations which account for the effect of inertia of
superconducting electron pairs in the dynamically deformed
superconductors that form the junction. The result indicates
possible Josephson pair tunneling current induced by the
transverse elastic wave, but not by the longitudinal elastic
wave. It is shown that for a transverse elastic wave incident
on the Josephson junction, the induced Josephson pair
tunneling current may appear theoretically at any non-zero
frequency, which is different from the well-known
phonon-assisted single electron tunneling phenomenon where a
minimum frequency exists. It is also shown that a DC current
step structure may appear in the current-voltage
characteristics of the deformable Josephson junction biased by
a DC voltage and exerted by a transverse elastic
wave. |
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Resonant
steps in parallel Josephson junction arrays: parametric
instabilities of whirling
modes S. Watanabe, S.H. Strogatz,
H.S.J. van der Zant and T.P. Orlando
Summary:
Circular arrays of underdamped Josephson junctions
exhibit a series of resonant steps in the return path of the
subgap region in the current-voltage characteristics. We show
that the voltage locations of the steps can be predicted by
studying the parametric instabilities of whirling periodic
solutions, and experimentally verify the prediction in a ring
of 8 underdamped junctions. The whirling modes become unstable
in certain voltage intervals, and a branch (a resonant step)
of more complicated solutions emerges from the endpoint of
each interval. We extend the analysis to open-ended arrays and
find that for f=0, the onset of a zero-field step has the same
underlying mechanism. For f>0, combinations of lattice
eigen-frequencies are excited. |
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Phase
locking in two-dimensional arrays of Josephson junctions:
effect of critical-current
nonuniformity R.L.
Kautz
Summary: Numerical simulations are used
to study mutual phase locking in two-dimensional arrays of
Josephson junctions for parameters typical of successful
millimeter-wave oscillators. Such arrays are shown to be very
tolerant of random critical-current nonuniformities. However,
comparison with an equivalent series array reveals that the
locking between rows in a two-dimensional array is principally
due to feedback through the external load and not to internal
coupling between rows. |
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Self-field
effects in two-dimensional Nb Josephson-junction
arrays E. Trias, J.R. Phillips,
H.S.J. van der Zant and T.P. Orlando
Summary:
We have measured two-dimensional niobium Josephson
junction arrays in which self induced fields are important. We
find an increase of the depinning current when /spl
lambda//sub /spl perp//, the penetration depth in the array,
is of the order of one. There is evidence for a destruction of
commensurate vortex states in the arrays as the depinning
current becomes almost independent of the applied magnetic
field. Our data also show that self-field effects change the
array flux-flow dynamics and decrease the effective array
viscosity. |
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600
GHz resonant mode in a parallel array of Josephson tunnel
junctions connected by superconducting microstrip
lines V.K. Kaplunenko, B.H.
Larsen, J. Mygind and N.F. Pedersen
Summary:
The high frequency properties of the one-dimensional
transmission line consisting of a parallel array of
resistively shunted Josephson tunnel junctions have been
studied in the limit of relatively low damping where this
nonlinear system exhibits new and interesting phenomena. Here
we report on experimental investigations of a resonant step
observed at a voltage corresponding to 600 GHz in the dc
current-voltage characteristic of a parallel array of 20
identical small NbAlO/sub x/Nb Josephson junctions
interconnected by short sections of superconducting microstrip
line. The junctions are mutually phase locked due to
collective interaction with the line sections excited close to
the half wavelength resonance. The phase locking range can be
adjusted by means of an external dc magnetic field and the
step size varies periodically with the magnetic
field. |
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Phase
locking experiments in distributed arrays of Josephson
junctions R.P.
Robertazzi
Summary: Arrays of phase locked
Josephson junctions are attractive for use as sub-mm
wavelength voltage controlled oscillators for heterodyne
mixers and free space radiators. We have performed phase
locking experiments on 40 junction, parallel biased arrays of
Josephson junctions coupled through transmission lines of
varying delays. The longest junction to junction delay
implemented was 5.4 ps for a design frequency of 90 GHz, while
the shortest was 1.45 ps, for a design frequency of 345 GHz.
The resonant frequency f/sub 0/ of the arrays was found to be
almost independent of the transmission line delay with f/sub
0/, scaling with the plasma frequency for arrays fabricated at
critical current densities of 10/sup 3/ and 4.5/spl
times/10/sup 3/A/cm/sup 2/. The data indicate that at the
resonant frequency, strong phase locking is present among the
junctions for junction separations significantly less than one
half wavelength even in arrays many wavelengths
long. |
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Phase-locking
of stacked all-niobium junction arrays to external
rf-irradiation A.M. Klushin, H.
Kohlstedt and J. Niemeyer
Summary: We have
experimentally investigated the range of locking to external
rf-bias current for large 3D arrays. Up to 2000 series
connected stacks with two junctions in a stack and 84 series
connected stacks with four junctions in a stack were
incorporated into a microstripline. Our measurement showed a
drastic reduction of the phase locking range with an
increasing number of junctions in an individual stack of the
array. We investigated the dependence of the attenuation in
the microstripline for different numbers of junctions in a
stack. In addition, the attenuation of the rf current in the
neighboring junctions in a stack was measured. |
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Direct
observation of vortex dynamics in two-dimensional
Josephson-junction arrays T.
Doderer, S.G. Lachenmann, R.P. Huebener, P.A.A. Booi and S.P.
Benz
Summary: Spatially resolved images of
the dynamic states of current-biased overdamped
two-dimensional arrays of Nb/AlO/sub x//Nb Josephson junctions
were obtained using low-temperature scanning electron
microscopy. We present two-dimensional imaging results
describing various vortex dynamic regimes in zero applied
magnetic field. The nucleation of current-induced vortices at
the array boundaries and their subsequent motion into the
array interior are observed for bias currents slightly above
the array critical current. With increasing bias current,
vortex-vortex interaction becomes important. Discussions on
the coherent microwave radiation emission are
presented. |
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LTS
Josephson junction critical current uniformities for LSI
applications L.A. Abelson, K.
Daly, N. Martinez and A.D. Smith
Summary:
Manufacturing yields of large scale superconducting
circuits depend strongly on the uniformity of junction
critical currents. We report on junction manufacturing
tolerances based on extensive measurements of Nb- and
NbN-based junction arrays and individual junctions. Transient
waveforms induced by switching of a single junction have
sufficient amplitude to switch other junctions in a series
array. We have measured the effect of sympathetic switching
and developed damping structures to dissipate switching
transients. Comparisons of critical current distributions
measured on individual junctions with critical current
distributions determined from series junction arrays are
presented. In addition, the validity of using series arrays of
large numbers of junctions to assess the critical current
uniformity is discussed. |
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Fabrication
of high quality, deep-submicron Nb/AlO/sub x//Nb Josephson
junctions using chemical mechanical
polishing Z. Bao, M. Bhushan,
Siyuan Ran and J.E. Lukens
Summary: A
reliable process based on Chemical Mechanical Polishing (CMP)
has been developed for the fabrication of high quality,
deep-submicron Nb/AlO/sub x//Nb Josephson junctions on 2 inch
wafers. The Nb counter electrode is defined using low pressure
SF/sub 6/ reactive ion etching (RIE) with a mask of SiO, which
is thermally evaporated through a bilayer resist stencil
patterned by electron beam lithography. After RIE, the entire
wafer is coated with SiO, which is then planarized using CMP
(which also removes the etch mask) to expose the counter
electrode. This technique has produced high quality (V/sub
m//spl sime/60 mV for J/sub c/ of 2 kA/cm/sup 2/) junctions
with areas as small as 0.003 /spl mu/m/sup 2/ demonstrating
that the process does not degrade the junction quality.
Junctions with critical currents of 22 /spl mu/A and areas of
0.006 /spl mu/m/sup 2/ have been fabricated from trilayers
with J/sub c/>300 kA/cm/sup 2/. |
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Electrical
characterization of Nb/Al-oxide/Nb Josephson junctions with
high critical current
densities A.W. Kleinsasser, W.H.
Mallison, R.E. Miller and G.B. Arnold
Summary:
Transport in Nb/AlO/sub x//Nb junctions involves two
parallel channels, barrier defects (pinholes) with
sub-nanometer dimensions and nearly-ideal tunneling regions.
We fit junction characteristics using only a single parameter,
the ratio of the normal state conductances of these current
paths. Our barrier model accounts for the excellent Josephson
behavior and highly non-ideal quasiparticle characteristics of
junctions with critical current densities as high as 4 mA//spl
mu/m/sup 2/. It appears to be quite generally applicable to
tunnel junctions. |
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Characteristics
of high critical current density Josephson junctions with
Nb/AlO/sub x//Nb trilayers H.
Sugiyama, A. Fujimaki and H. Hayakawa
Summary:
We fabricated high critical current density (high J/sub
c/) Josephson junctions, up to 47 kA/cm/sup 2/, consisting of
Nb/AlO/sub x//Nb trilayers by use of high vacuum dc magnetron
sputtering (less than 10/sup -6/ Pa). The relationship Jc/spl
prop/(Pt)/sup -0.5/ can be obtained up to 47 kA/cm/sup 2/,
where P and t are pressure and time, respectively, in
oxidizing an Al surface. In the high J/sub c/ junctions,
microshorts existed in Al surfaces. A property peculiar to
most of the high J/sub c/ junctions was a step appearing at
1/3 gap voltage on their I-V curves. Magnetic field dependence
of this step was different from that of a Fiske
step. |
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Coherent
flux-flow in vertically stacked long Josephson tunnel
junctions A.V. Ustinov, H.
Kohlstedt and C. Heiden
Summary: Vertical
stacks of two Nb/Al-AlO/sub x//Nb long Josephson junctions
with nearly identical parameters have been studied
experimentally. The magnetic coupling between the junctions
was provided by their common electrode of thickness d/spl
sime//spl lambda//sub L/. The I-V characteristics displayed
flux-flow resonances of the two junctions. Two different
mutually phase-locked regimes were found: the lower velocity
anti-phase mode, and the high velocity in-phase mode. These
modes, while staying locked, could be tuned by the magnetic
field in a broad voltage range which corresponds to the
Josephson frequencies of 150-600 GHz for the lower mode and
280-400 GHz for the upper mode. Our observations suggest
applications of the stacked long Josephson junctions as local
oscillators for millimeter and sub-millimeter wave
circuits. |
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A
cryogenic scanning laser microscope for investigation of
dynamical states in long Josephson
junctions J. Helm and J.
Mygind
Summary: The first local oscillators
based on moving magnetic flux quanta in long Josephson
junctions are being developed for superconducting integrated
quasi-optical SIS receivers. In order to further refine these
oscillators one has to understand the complex dynamics of
these devices. Since the local tunnel current is one of the
most important internal junction parameters which together
with the boundary conditions determine the dynamics, it is of
vital importance to experimentally determine the current
density throughout the entire junction with high spatial
resolution. Here we report on measurements on different
oscillator samples, performed with a novel Cryogenic Scanning
Laser Microscope (CSLM) having a spatial resolution of less
than /spl plusmn/2.5 /spl mu/m over a 500 /spl mu/m/spl
times/50 /spl mu/m wide scanning area in the temperature range
2 K-300 K. Even though the dynamical states are extremely
sensitive to external noise this microscope enables us to make
stable in-situ measurements on operating Josephson junctions.
Recent results are presented and discussed. |
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Multilevel
devices of YBa/sub 2/Cu/sub 3/O/sub 7/ with NdGaO/sub 3/
barrier D. Grundler, J.-P.
Krumme, B. David and O. Doessel
Summary: We
have fabricated YBa/sub 2/Cu/sub 3/O/sub 7/ ramp-type
junctions incorporating a barrier layer of NdGaO/sub 3/ with a
nominal thickness of 2 nm. The junctions exhibit pronounced
Josephson effects and operate up to 82 K. The characteristics
are well described within the resistively shunted junction
model. We observe large hysteresis parameters /spl beta//sub
c/ even at elevated temperatures. The output voltage of a
high-T/sub c/ dc SQUID is found to benefit from the intrinsic
junction capacitance. |
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Fabrication
and characterization of ramp edge-type junction and
SQUIDs G.A. Alvarez, M. Kuroda,
M. Matsuda, K. Miyamoto, N. Kasai, M. Koyanagi and T.
Nemoto
Summary: We have investigated the
properties of high-T/sub c/ ramp-edge geometry Josephson weak
links using superconducting YBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta// (YBCO) electrodes and PrBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta//(PBCO) normal-metal layers. Unambiguous evidence of
Josephson behaviour has been observed. Current-voltage
characteristics (CVC) were qualitatively consistent with the
resistively-shunted-junction (RSJ) model. Well developed
Shapiro steps for 8.9 GHz microwave irradiation have been
observed. Furthermore we have fabricated dc-SQUIDs with PBCO
barriers that modulate up to a temperature of 80.6 K. At 4.2 K
we find a flux-voltage modulation depth of /spl ap/36 /spl
mu/V. |
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First
space test of high-T/sub c/
SQUIDs M. Klinger, J.H. Hinken
and S.S. Tinchev
Summary: On September 12,
1993, the German satellite ASTROSPAS was launched on board the
Space Shuttle Discovery, Flight STS-51. The satellite included
the scientific device ORFEUS, as well as the SESAM experiment,
developed by Deutsche Forschungsanstalt fur Luft- und
Raumfahrt in Braunschweig, Germany, to investigate surface
effects. One of the 20 SESAM samples was a chip with 16
high-T/sub c/ RF SQUIDs on a SrTiO/sub 3/ substrate. The
SQUIDs were made using YBCO films and local oxygen-ion
irradiated weak links, at launch time the sample was 19 months
old. No changes were observed in the SQUID operation after
this 10 days flight. This is the first space test of
electronic devices based on high-T/sub c/
materials. |
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Method
for improving voltage modulation depth of high T/sub c/ DC
SQUID with large inductance K.
Enpuku, H. Doi, G. Tokita and T. Maruo
Summary:
Two methods are proposed in order to improve the
voltage modulation depth of high-T/sub c/ DC SQUIDs in the
case of large inductances. One is a damping resistance
parallel to the inductance, and the other is a new SQUID using
three junctions, which we call 3J-SQUID. Numerical simulation
shows the usefulness of the present method. Moreover. It is
shown that the improvement of the voltage modulation depth
results in the improvement of magnetic flux noise in the white
noise region. Therefore, the present method will enable the
use of large inductances. The usefulness of the present method
is also confirmed partly by experimental
results. |
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Inductance
calculation for integrated superconducting structures by
minimizing free energy G.
Hildebrandt and F.H. Uhlmann
Summary: We
present a method to calculate the inductance matrix of three
dimensional superconducting structures by minimizing the free
energy. In the case of high-T/sub c/ superconductors, the
kinetic inductance becomes substantial and an accurate
calculation of inductances is required. The London penetration
depth /spl lambda/ and the kinetic inductance are accurately
included by this method. The results of this program agree
well with measurements of high-T/sub c/ DC-SQUIDs
(superconducting quantum interference devices). |
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Application
of small-signal model to DC SQUID circuit
design W.P.
Geren
Summary: As the performance of HTS DC
SQUIDs continues to improve, their utilization in RF devices
(e.g., amplifiers, nuclear magnetic resonance detectors)
having complex circuitry becomes more attractive. To fully
realize their potential in this application, accurate and
efficient analysis techniques are required to assist the
circuit designer. Beginning with measured V-phi and I-V data
for the device, we have used the small-signal model to
optimize the design of a two-stage low-noise amplifier (LNA)
comprised of DC SQUIDs. Optimization criteria were maximum
gain and minimum noise figure at the upper band edge. We have
shown that the small signal model is an invaluable design tool
which provides the analytical performance data needed to
optimize the SQUID and its attendant RF
circuitry. |
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YBa/sub
2/Cu/sub 3/O/sub 7/(-x) step-edge junctions prepared on
sapphire substrates with YSZ buffer
layer R. Adam, S. Benacka, S.
Chromik, M. Darula, V. Strbik, S. Gazi, R. Kostic and E.
Pincik
Summary: Electrical properties of
YBa/sub 2/Cu/sub 3/O/sub 7-x/(YBCO) step-edge junctions were
investigated. Steps of height approximately 90 nm were
prepared on sapphire substrates by Ar milling. Step angles
were adjusted by the angle of incidence of Ar ions. After
vacuum deposition of the YSZ buffer layer (50 nm thick) an
epitaxial YBCO film was grown by magnetron sputtering. Step
edge junctions were prepared by wet etching. The
current-voltage characteristics were of RSJ type, with I/sub
c/R/sub n//spl ap/0.5 mV at 77 and Shapiro steps were observed
up to 0.2 mV (at 9.2 GHz in the temperature range 4.2-80 K)
and compared with the resistively shunted Josephson junction
(RSJ) model including capacitance and noise. |
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Electron
beam lithographed straight and wavy YBa/sub 2/Cu/sub 3/O/sub
7/ step edge junctions H.R. Yi,
D. Winmer, Z.G. Ivanov and T. Claeson
Summary:
We have developed a process for the fabrication of
YBa/sub 2/Cu/sub 3/O/sub 7/ (YBCO) step edge junctions. This
process greatly improved the uniformity of the step angles,
the straightness and sharpness of the step edges on LaAlO/sub
3/ substrates. We used an electron beam lithography defined
amorphous carbon film as an ion milling mask. By studying
junctions made across straight and wavy step edges, we showed
the importance of the straightness on the quality of YBCO
junctions. Junctions fabricated across these improved step
edges showed less j/sub c/ variations (a factor of 2-3
compared to >10 for standard step edge junctions) and
improved current distribution. We increased the McCumber
constant /spl beta//sub c/ by varying the step height and the
YBCO film thickness (h and t). Hysteresis was observed in the
I-V characteristics at 4.2 K for junctions with h=240 nm and
t=180 nm. The capacitance per unit area was calculated to be
15 fF//spl mu/m/sup 2/. The magnetic field (H) dependence of
the critical current (I/sub c/) showed well-defined periods
with a main peak in the center. The I/sub c/ in the first
minimum can be suppressed to 20-40% in most cases. For some
junctions, I/sub c/ can also be suppressed to zero at higher
temperatures. However, we did not observe a perfect Fraunhofer
pattern in the I/sub c/ vs. H curve. The field period /spl
Delta/H was found to have a w/sup -2/ dependence on the
junction width (w). |
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Fabrication
of YBCO step-edge Josephson junctions by inverted cylindrical
magnetron sputtering technique A.
Di Chiara, F. Lombardi, F. Miletto Granozio, F. Tafuri, M.
Valentino, S. Matarazzo, S. Pagano, B. Ruggiero and M.
Russo
Summary: The Inverted Cylindrical
Magnetron Sputtering (ICMS) technique been used to fabricate
YBCO step-edge dc SQUIDs. Steps are obtained by standard ion
milling procedure on LaAlO/sub 3/ (100) substrates using
Nb-masks patterned by reactive ion etching. Thin films are
then deposited under different conditions (both step and
deposition angles) and patterned by standard lithography and
wet chemical etching. An analysis of junction properties in
terms of step height and film thickness has been carried out.
Measurements on current vs magnetic field and SQUID voltage
response measurements have been performed. Their temperature
dependences have been also considered. Operating temperature
as high as 77 K has been achieved. At 4.2 K the SQUIDs show a
maximum voltage to flux transfer function (/spl part/V//spl
part//spl phi/)/sub max/=870 /spl mu/V//spl Phi//sub 0/ and a
good periodicity of the V-/spl phi/ modulation up to 20 /spl
Phi//sub 0/ without any sign of hysteresis. |
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YBa/sub
2/Cu/sub 3/O/sub 7/ nano-bridge junctions and dc SQUIDs made
by focused ion beam
milling D.H.A. Blank, W. Booij,
H. Hilgenkamp, B. Vulink, D. Veldhuis and H.
Rogalla
Summary: YBa/sub 2/Cu/sub 3/O/sub 7/
nano-bridges with widths ranging from 200 to 800 nm were made
using Focused Ion Beam milling. The I-V characteristics of the
narrowest nano-bridges show, under microwave irradiation,
pronounced Shapiro steps up to the transition temperature. An
inductively shunted single layer SQUID, using these
nano-bridges, has been realised by a combination of Focused
Ion Beam milling and selective epitaxial growth. Flux to
voltage modulation up to 82 K was observed, with a maximum
modulation depth of 3.7 /spl mu/V at 78 K. |
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Current
phase relation of Y/sub 1/Ba/sub 2/Cu/sub 3/O/sub 7/(-/spl
delta/) step edge junction V.
Polushkin, S. Uchaikin, S. Knappe, H. Koch, B. David and D.
Grundler
Summary: The small signal rf
impedance of Y/sub 1/Ba/sub 2/Cu/sub 3/O/sub 7-/spl delta//
step edge junction rf SQUIDs operating in a strongly
nonhysteretic mode has been measured. The phase dependent
inductance L/sub J/(/spl phi/) and the current phase relation
I/sub p/(/spl phi/) of step-edge junctions embedded in SQUIDs
are calculated from measurement data following the
Vincent-Deaver approach. Two of three junctions investigated
revealed a sinusoidal current phase relation. I/sub p/(/spl
phi/) of the third junction seemed to be non-sinusoidal and
hysteretic. A model explaining the origin of the
non-sinusoidality of I/sub p/(/spl phi/) is
proposed. |
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Detection
of the Josephson self-radiation from YBCO step-edge junctions
in millimeter-wave K. Lee and I.
Iguchi
Summary: We have investigated both DC
and AC Josephson effects of the YBa/sub 2/Cu/sub 3/O/sub y/
(YBCO) thin film step-edge junctions; single step-edge
junction on LaAlO/sub 3/ substrate with the step angle about
50-60/spl deg/ and biepitaxial double step-edge junction made
on MgO substrate with a CeO/sub 2/ seed layer. The Josephson
self-radiation was directly detected using the total power
radiometer receiver systems with receiving frequencies of K
band (21-23 GHz) and millimeter-wave (46-48 GHz and 71-73 GHz)
range, respectively. For single step-edge junctions, the
Josephson self-radiation peaks exhibited at the voltages
corresponding to the basic Josephson voltage-frequency
relation. The maximum first-harmonic self-radiation power at
receiving frequency f/sub REC/=72 GHz and Josephson linewidth
were P(I)=2.0/spl times/10/sup -3/W and /spl Delta/f=3.62 GHz
at 4.2 K, respectively. For microwave irradiation, the
harmonic Shapiro steps and additional half integer steps with
their quasi-periodic variation satisfying the Josephson
equation V=(n/m)(hf/2e) were clearly observed. For double
step-edge junctions, we also observed the steps corresponding
to the two junction boundaries on the two steep steps. These
behaviors described with different current-phase relations
corresponding to the crystal orientation relationship between
the two junction boundaries. |
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High
T/sub c/ superconducting step-edge junctions and their
properties in millimeter-wave
band Y.J. Feng, L. Kang, X.B.
Wang, S.Z. Yang, J.P. Zuo, H.B. Wang, W.W. Xu, Q.H. Cheng,
P.H. Wu, S.L. Yan and L. Zhou
Summary:
Superconducting step-edge junctions were fabricated on
step-edges in (100) LaAlO/sub 3/ substrates by
sputter-deposited epitaxial YBaCuO and TlBaCaCuO thin films.
The substrate steps were patterned by ion beam etching using
metal film as a mask. The transport properties of the
junctions were characterized by four-probe electrical
measurements. The critical current-normal resistance product
(I/sub c/R/sub N/) was larger than 0.2 mV (77 K) for most of
the junctions. Clear Shapiro steps were observed in the
current-voltage characteristics of the junctions with 36 GHz
or 95 GHz millimeter-wave irradiation. The high frequency
properties of these high T/sub c/ Josephson junctions showed
that they were quite suitable for the Josephson harmonic mixer
used in the digital phase locked millimeter and sub-millimeter
wave sources. |
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Millimeter
and submillimeter wave responses of YBa/sub 2/Cu/sub 3/O/sub
7/ step-edge Josephson
junctions H. Shimakage, Y. Uzawa,
Z. Wang, A. Kawakami, W. Chujo and B.
Komiyama
Summary: We have fabricated YBCO
step-edge Josephson junctions and measured the responses to
millimeter and submillimeter irradiation. In the substrate
milling process for the purpose of fabricating the step, the
step angle was controlled using a Nb metal mask. At a step
angle of 20 degrees, we obtained Josephson junctions, the
characteristics of which are consistent with the RSJ model. We
estimated the capacitance to be 4.4 fF using the RSJ model,
but such a value for an 8 /spl mu/m wide and 300 nm thick
junction seems too small. When the junctions were irradiated
by 300 GHz radiation, Shapiro steps up to the 4th were
observed. The junctions were used as mixers in the 100 GHz
band, and as harmonic mixers in the 100 GHz LO and 700 GHz RF
bands. Beat signals were observed in both cases. We also
estimated the quasi-optical conversion losses of the step-edge
junctions as mixers. |
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Josephson
behaviour and flux penetration effects in YBCO double
tilt-angle step-edge
junctions C.P. Foley, G.J.
Sloggett, K.-H. Muller, S. Lam, N. Savvides, A. Katsaros and
D.N. Matthews
Summary: YBCO thin-film
step-edge junctions have been prepared whose characteristics
show features corresponding to the two tilt-angle
grain-boundary junctions formed at the step. The I-V
characteristics of these junctions are fitted to high accuracy
by a model consisting of two noisy resistively-shunted
Josephson junctions. In applied magnetic fields up to a few
hundred microtesla, both junction critical currents show
reversible flux modulation, in one case indicating excellent
uniformity of the critical current distribution along the
step. In stronger magnetic fields, the junction critical
current modulation shows evidence of flux penetration into the
film, i.e. the mixed state. Taking demagnetising effects into
account the lower critical field of YBCO at 77 K, /spl mu//sub
0/H/sub e1,e/, is found to be 12 mT. |
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Design
and testing of high-T/sub c/ Josephson pulse driver using
selective SEJs T. Umezawa and Y.
Higashino
Summary: We have designed a novel
Josephson pulse driver based on SFQ circuits using high-T/sub
c/ junction parameters, and fabricated it using selective
SEJs. Simulation showed that the output pulse can be stepped
up to 2.5 mV, which is 13 times larger amplitude than the
input pulse. In the fabricated driver using a microstrip line,
two dozen SEJs were integrated with Au resistors and
inductors. The driver operated at 77 K with a conversion
factor of (1-1.5) at best. |
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Modification
of step-edge grain boundary Josephson junctions by
electromigration J.B. Bulman and
J.M. Murduck
Summary: We report on the
effects of large electric currents (>2 MA/cm/sup 2/)
applied at /spl sim/300 K to step-edge thin-film microbridges
of YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//. These step-edge
Josephson junctions showed an increase in their critical
current (I/sub c/) after application of electromigration
current, I/sub EM/. This increase of I/sub c/ was a permanent
phenomenon. Electromigration was also performed on SNS YBa/sub
2/Cu/sub 3/O/sub 7-/spl delta// thin-film microbridges and an
increase in critical current was observed. |
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Fabrication
of Bi/sub 2/Sr/sub 2/Ca/sub 2/Cu/sub 3/O/sub x/ thin film
grain boundary junctions K.
Ohbayashi, H. Fujii, A. Kuzuhara, T. Ohtsuki, M. Inoue, A.
Fujimaki and H. Hayakawa
Summary: As-grown
high-quality superconducting thin films of the Bi/sub 2/Sr/sub
2/Ca/sub 2/Cu/sub 3/O/sub x/ were prepared by RF magnetron
sputtering with a regulated shuttering technique. 2223 phase
films with a 2201 phase buffer layer were deposited on MgO
(100) substrates under rigorous control of the bismuth content
and valence. As a source of bismuth, Bi(metal) and Bi/sub
2/Sr/sub 2/CuO/sub x/ targets were used. At the preparation no
post-treatment steps were performed. The zero resistivity
critical temperature of the as-grown film was 107.3 K. Using
these films, Bi/sub 2/Sr/sub 2/Ca/sub 2/Cu/sub 3/O/sub x/
step-edge and bicrystal Josephson junctions were prepared. At
step-edge junctions, Josephson current was observed up to 41
K, below this temperature I-V curves were RSJ-like. On the
other hand, bicrystal junctions were fabricated,on the
bicrystal MgO (100) substrate with a misorientation angle of
24/spl deg/. Typical RSJ model I-V curves were observed up to
60 K. The modulation depth goes up to 90%. I/sub c/R/sub n/
values were about 1.0 mV at 4.2 K. |
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RSFQ
pseudo random generator and its possible
applications A.Yu.
Kidiyarova-Shevchenko and D.Yu. Zinoviev
Summary:
We have analyzed theoretically and simulated a set of
4-bit RSFQ-logic-based Pseudo Random Generators (PRG). These
circuits have been fabricated using low-T/sub c/ niobium
technology. We have also investigated experimentally an XOR
cell and a shift register with parallel outputs that have been
used as compound parts of the PRGs. Experimentally measured
margins for DC power supply voltage for a PRG with a serial
output, an XOR cell and shift register were 10%, 15%, and 15%
respectively. In this paper we discuss various possible
applications of a PRG in testing RSFQ circuits and also as a
source of "quasiwhite" digital noise. |
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RSFQ
arithmetic blocks for DSP
applications S.V. Polonsky, Jao
Ching Lin and A.V. Rylyakov
Summary: We have
designed a Rapid Single-Flux-Quantum (RSFQ) bit-serial
real-time pipeline multiplier for digital signal processing
(DSP) applications. A single-bit module of this multiplier
consists of 96 Josephson junctions and uses a
B-flip-flop-based carry-save adder (CSA). For HYPRES' standard
1-kA/cm/sup 2/ Nb process with 3.5 /spl mu/m-diameter
Josephson junctions the module occupies all area of 350/spl
times/600 /spl mu/m/sup 2/. Simulations show that the circuit
should dissipate 28 /spl mu/W of power at 2.6 mV dc supply
voltage and operate at frequencies of up to 25 GHz. We have
successfully tested all cells of the module and verified
correct operation of a simplified version of the module at low
frequencies. According to numerical simulations, the speed of
the multiplier is limited by the CSA. In order to overcome
this bottleneck we have developed a concept of a fast
carry-save pipeline adder based on XOR gates which uses an
RSFQ-specific algorithm for carry bit
calculation. |
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4.6
GHz SFQ shift register and SFQ pseudorandom bit sequence
generator Joonhee Kang, A.H.
Worsham and J.X. Przybysz
Summary:
Superconductive electronics can provide low power, GHz
speed spread spectrum satellite communications. The key
components to construct the spread spectrum modem are an
analog filter and a digital pseudorandom bit sequence
generator, Various SFQ logic circuits are required to
construct a code generator. These circuits include a shift
register, a reset switch, and an XOR or XNOR. To make a 4 bit
15 sequence code generator, a four stage shift register with a
fan-out of two on each stage was designed. These circuits,
fabricated with eight level Nb/AlO/sub x//Nb Josephson
junction integrated circuit process, showed correct operation
at low speed digital tests. The low speed digital test was
done by using a "catcher", the combination of a read SQUID and
a Josephson transmission line (JTL) which were magnetically
coupled to each other. High speed testing of the shift
register used a latch amplifier, which amplified an SFQ pulse
to a latching output voltage of about 2 mV. This test showed
correct operation of the shift register at speeds of up to 4.6
GHz. |
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Operation
of a 1-bit quantum flux parametron shift register (latch) by
4-phase 36-GHz clock M. Hosoya,
W. Hioe, K. Takagi and E. Goto
Summary: The
Quantum Flux Parametron (QFP) is a SFQ-type logic device which
uses a single flux quantum (SFQ) to represent 1-bit of
information. QFP circuits use a multi-phase external ac power
which also acts as the clock for synchronization, hence QFP
circuits are highly pipelined. The clock frequency must be
increased to improve the throughputs of the circuits, so the
control of a high frequency clock is a key technology for the
QFP. This paper describes a clock distribution technique which
utilizes the characteristics of a standing wave. Using this
technique, the operation of a 1-bit QFP shift register by a
4-phase clock up to 36 GHz is shown. In the 4-phase clock
operation of QFPs, the input is given in phase 1, the QFP
switches in phase 2, the output is held during phase 3, and
the QFP resets in phase 4. Therefore, the 4-phase 36-GHz
operation means that each QFP switches or resets in less than
7 ps. |
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A
new design approach for High-T/sub c/ based RSFQ
logic V.K. Kaplunenko, Z.G.
Ivanov, A. Bogdanov, E.A. Stepantsov, T. Claeson, T. Holst,
Z.J. Sun, R. Kromann, Y.Q. Shen, P. Vase, T. Freitoft and E.
Wikborg
Summary: We suggest a new design of
Rapid Single Flux Quantum (RSFQ) logic circuits which is based
on a single superconducting layer and does not require a
superconducting ground plane. The small inductances of about
10 pH, that are obligatory for the RSFQ applications, are
formed as narrow slits with width comparable to the London
penetration depth (/spl cong/0.15 /spl mu/m). The design
allows us to decrease the geometric size of the RSFQ cell and
can be applied to low-T/sub c/ circuits as well. Test circuits
have been implemented using YBaCuO grain boundary junctions on
assymmetric 32/spl deg/Y-ZrO/sub 2/ bi-crystals to measure the
slit inductance per unit length and the mutual inductance of
neighboring slits. A typical inductance of a 0.4 pm slit was
determined to be 0.7pH//spl mu/m. We present a new design and
a computer simulation of a flip-flop circuit based on these
inductance measurements. To realize these circuits
experimentally one needs at least two grain boundaries,
separated by a distance of 10 to l5 /spl mu/m, or to use
bi-epitaxial or step-edge junction technology. |
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Picosecond
optoelectronic study of superconducting microstrip
transmission lines J.F.
Bulzacchelli, Hae-Seung Lee, K.G. Stawiasz, S. Alexandrou and
M.B. Ketchen
Summary: The ballistic transport
of picosecond digital signals along terminated microstrip
lines is a key feature of single flux quantum (SFQ) logic. In
this work, we have used fast photoconductors driven by a
femtosecond laser to measure directly for the first time the
propagation and termination of picosecond pulses along Nb
microstrip lines. Electrical pulses as short as 0.8 ps
full-width-at-half-maximum (FWHM) have been measured. After
propagating distances of 200 /spl mu/m, 1 mm, and 6.5 mm, the
pulses broadened to 1.0, 1.2, and 1.8 ps (FWHM), respectively.
In the frequency domain, attenuation is found to be negligible
up to the gap frequency of Nb(0.7 THz), beyond which
attenuation increases rapidly. We have also measured the
reflections of the picosecond pulses off different
terminations: open circuit, short circuit, and various
resistors. The effective suppression of reflections with
matched resistive loads is demonstrated up to frequencies
approaching 1 THz. |
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On-chip
picosecond delay measurement of RSFQ digital logic
gates D.K. Brock, S.S. Martinet
and M.F. Bocko
Summary: Because RSFQ circuits
are intended to operate at multi-GHz frequencies, a logical
requirement for developing the technology is a method of
accurately measuring the picosecond delays associated with
individual logic circuits. A technique has been developed for
on-chip measurements of such RSFQ gate delays. The central
element in this scheme is a race between a path of calibrated
variable delay and a path of unknown delay. Modification of
the canonical RSFQ RS flip-flop circuit yields a multiple
state destructive readout cell (MDRO), in which one can
configure the number of flux quanta to be stored. This circuit
has been experimentally verified for groups of two flux
quanta. Used in concert with the confluence buffer, this
scheme can provide the RSFQ designer with sub-picosecond pulse
arrival delay information crucial for higher order circuit
simulation. A detailed experimental process is presented from
which this timing information can be extracted using basic
low-speed measurement techniques. |
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An
optoelectronic testing system of rapid, single-flux quantum
circuits M. Currie, Chia-Chi
Wang, D. Jacobs-Perkins, R. Sobolewski and T.Y.
Hsiang
Summary: We have generated picosecond
voltage pulses on a superconducting microstrip line by using a
metal-semiconductor-metal photodiode as an optoelectronic
switch. These pulses are fed into a two-Josephson-junction
pulse shaper to generate single-flux quantum (SFQ) pulses.
Using a reflective electro-optic sampling system, SFQ pulses
are directly observed for the first time. This important
demonstration of nonintrusively detecting electrical signals
from superconducting microstrip lines at the level of rapid,
single-flux quantum (RSFQ) circuits opens up a new way to test
such circuits, on issues such as design verification, jitter,
and failure-mode testing. Further, we propose a variable-rate
optoelectronic clock for testing the functional speed of RSFQ
logic circuits, with an adjustable clock rate up to 38
Gb/s. |
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Operation
of a superconductive demultiplexer using rapid single flux
quantum (RSFQ) technology S.B.
Kaplan and O.A. Mukhanov
Summary: A
superconductive demultiplexer was designed, simulated, and
tested as an interface between ultra-fast superconductive
circuits and slower room-temperature electronics. The modular
RSFQ shift-and-dump circuit was designed as a register of
Non-Destructive Read-Out (NDRO) cells, which are timed by
pulses from the system clock. Data is read out from a 1:N
demultiplexer every N clock periods by applying a read-out
pulse to the register's NDRO input. Circuit simulations and
results for the successful experimental test of a 2-stage
demultiplexer will be discussed. |
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4-bit
rapid single-flux-quantum
decoder A.F. Kirichenko, V.K.
Semenov, Y.K. Kwong and V. Nandakumar
Summary:
We describe the design of a fast single-flux-quantum
decoder which can be used, e.g., in fast RAMs, general-purpose
microprocessors, and communication channel switches. The core
of the circuit is a tree of the single-bit SFQ demultiplexer
with toggle (rather than the reset-set) control. Three new
RSFQ cells: the demultiplexer, D flip-flop with complementary
outputs, and serial XOR with large parameter tolerances (dc
bias margins of /spl plusmn/25%, /spl plusmn/26%, and /spl
plusmn/27%, respectively) have been developed for the decoder
project. We have designed the first 16-bit prototype of the
decoder for 1-kA/cm/sup 2/ niobium-trilayer technology and
tested it at low frequencies. The circuit was completely
operable except for 3 (of 16) output SFQ/DC converters.
Simulations show that the circuit should allow data rate in
excess of 60 Gbit/s and channel switching time below 20
ps. |
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Field
effects on the dielectric property of YBCO bicrystal grain
boundary junctions K. Nakajima,
K. Yokota, H. Myoren, J. Chen and T.
Yamashita
Summary: Electric field effects on
YBCO grain boundary Josephson junctions combined with inverted
MIS (Metal, Insulator, Superconductor) structures were
studied. Current steps and hysteresis recognized in
current-voltage curves were strongly affected by the field.
The current steps were attributed to the self-excited
resonances, i.e., Fiske steps. Both the effects were
interpreted by the field dependence of the effective
dielectric constant of the grain boundary which has a certain
contribution from the large dielectric constant of SrTiO/sub
3/ substrates. The effective dielectric constant normalized
with barrier thickness of the junction was estimated to be
about 40 nm/sup -1/ for the zero gate voltage and was
decreased by a factor of 2 with the electric field of /spl
plusmn/16 kV/cm. This feature is assumed adequate for tuning
the phase velocity in the bicrystal grain
boundaries. |
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The
SUPFET, a new photodetector with ultrathin YBaCuO/PrBaCuO
multilayer channel A. Jager and
J.-C. Villegier
Summary: Several electric
field effect devices have been built with YBaCuO/PrBaCuO
layers and multilayers; The layers are deposited by an
inverted cylindrical magnetron sputtering process (ICM) on MgO
substrates. This process has been proved to give very good
performances even for thinner and ultra thin films. The films
used for the field effect transistor devices consist of one or
two bilayers of YBaCuO and PrBaCuO with a nominal thickness of
each material of about 4 nm. Small channel geometries of
50/spl times/60 microns are etched by argon ion milling and
the channel is covered by a silicon dioxide dielectric layer
(50-100 nm). The gate contacts as well as the drain and source
contacts are made by sputtered gold pads. These devices are
tested in static and dynamic measurements: the silicon dioxide
layer inhibits symmetric I-V characteristics of the dielectric
layer with high breakdown field strength up to 4 MV/cm. The
gate capacity of a few pF allows the test of the device in a
kHz frequency range. Tests with sine wave gate voltages show
low distortion of the output signal with a voltage gain of
about 0.01. Smaller dielectric layers could raise the gain
close to one. The results of these field effect experiments
are compared with optically induced effects. The optical
measurements are performed with a helium-neon laser (633 nm)
with a power density of 600 W/cm/sup 2/. The laser pulses with
frequencies up to 1 MHz give responses somewhat similar to the
observed field effect responses. Combining field effect and
optical irradiation, it Is found that the laser pulses seem to
create charge carriers, screening the field effect. Based on
this principle a new photodetector is proposed. |
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Modified
deposition procedure for high quality YBa/sub 2/Cu/sub 3/O/sub
7-x//SrTiO/sub 3/ bilayers V.
Talyansky, K. Petersen, C. Doughty, X.X. Xi and T.
Venkatesan
Summary: The degradation of an
ultrathin YBCO layer under SrTiO/sub 3/ due to oxygen
deficiency poses a fundamental problem in growing a bilayer
which may be patterned into a superconducting FET. Annealing
between depositions while growing the bilayer can help
increase the T/sub c/ of the YBCO while retaining acceptable
quality of the SrTiO/sub 3/. This study found T/sub c/ in the
range of 60-80 K for a 4 unit-cell thick YBCO film under
SrTiO/sub 3/. |
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Superconducting
field effect devices with high transition temperature and
critical current density C.
Doughty, V. Talyansky, C. Kwon, A.T. Findikoglu, X.X. Xi and
T. Venkatesan
Summary: We have investigated
buffer layers of Pr/sub 0.55/Y/sub 0.45/Ba/sub 2/Cu/sub
3/O/sub 7-/spl delta// (PY)BCO for YBa/sub 2/Cu/sub 3/O/sub
7-/spl delta// (YBCO)/SrTiO/sub 3/ field effect devices. The
transitions of single unit cell thick YBCO films in
(PY)BCO/YBCO/(PY)BCO trilayers depend strongly on the buffer
layer thickness, with optimum T/sub c//spl ap/40 K obtained at
a buffer layer thickness of 5nm. SuFET devices deposited on
such an optimized buffer layer exhibit substantial
improvements in channel quality. For a 3.6 nm thick channel,
transition temperature >55 K and critical current density
/spl sim/10/sup 6/ A/cm/sup 2/ are obtained. The modulations
observed in both the normal and superconducting states are
consistent with those obtained in earlier work on
non-weak-link dominated samples. |
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Electric
field effect of SrTiO/sub 3//YBa/sub 2/Cu/sub 3/O/sub 7-x/
multilayers grown by all-MBE T.
Nakamura, H. Tokuda and M. Iiyama
Summary:
Epitaxial SrTiO/sub 3//YBa/sub 2/Cu/sub 3/O/sub 7-x/
(STO/YBCO) multilayers for a superconducting field-effect
transistor (SuFET) were fabricated by an ozone assisted
Molecular Beam Epitaxy (MBE) method. To eliminate
interdiffusion at the interface, we deposited high quality STO
films at around 500/spl deg/C on YBCO films with clean
surfaces. At this temperature, interdiffusion was negligible
through in-situ Auger Electron Spectroscopy (AES). The
electric field effect in a Ag/STO/YBCO device configuration
also indicated the suppression of the interfacial layer
between the STO and YBCO film. |
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Electric
field effect in Sm/sub 1-x/Ca/sub x/Ba/sub 2/Cu/sub 3/O/sub y/
bicrystal junctions Z.W. Dong,
V.C. Matijasevic, P. Hadley, S.M. Shao and J.E.
Mooij
Summary: A three terminal device was
fabricated by depositing a thin film of Ca-doped SmBa/sub
2/Cu/sub 3/O/sub y/ on a bicrystal SrTiO/sub 3/ substrate and
then structuring a gate over the resulting junction. The
channel shows RSJ-like Josephson junction behavior. By
applying a voltage to the gate, a large electric field effect
was observed. The largest field effect was observed in films
where 30% of the Sm was replaced by Ca. The critical current
of the junction was modulated 23% by the application of an
electric field of 5/spl times/10/sup 5/ V/cm. This electric
field is about 100 times smaller than the electric field
necessary for the field effects observed in homogeneous films.
The sign of the field effect is consistent with that expected
for a carrier-depleted grain boundary region. |
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Transistor
performance of high-T/sub c/ three terminal devices based on
carrier concentration
modulation K. Joosse, Y.M.
Boguslavskij, L. Vargas, G.J. Gerritsma and H.
Rogalla
Summary: Electric field effect
devices and quasiparticle injection effect devices are good
candidates for the realization of three terminal devices from
high-T/sub c/ materials, since they take explicit advantage of
the low carrier concentration in these compounds. We describe
the fabrication and operation of both types of devices, and
discuss their performance as transistor-like
elements. |
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Superconducting
junctions using a 2DEG in a strained InAs quantum well
inserted into an InAlAs/InGaAs MD
structure T. Akazaki, J. Nitta,
H. Takayanagi and K. Arai
Summary: A newly
fabricated three-terminal Josephson junction is coupled with a
two-dimensional electron gas (2DEG) in a strained InAs quantum
well inserted into an InAlAs/InGaAs modulation-doped
structure. The 2DEG is confined in the InAs quantum well and
has a maximum mobility of 155000 cm/sup 2//Vs at a
sheet-carrier density of 1.86/spl times/10/sup 12/ cm/sup -2/
at 10 K. The supercurrent flows through the 2DEG and can be
controlled by adjusting the gate voltage. The critical current
and normal resistance are measured as a function of the gate
voltage, and the sheet-carrier density dependence of the
critical current is obtained. We also measure the temperature
dependence of the critical current at different gate voltages.
The results indicate that, when using this junction, the
superconducting characteristics can range between the clean
and dirty limits. |
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Three-terminal
field effect superconducting device using SrTiO/sub 3/
channel A. Yoshida, H. Tamura, H.
Takauchi, T. Hato and N. Yokoyama
Summary: As
a first step toward fabricating transistors to control
supercurrent, we fabricated two- and three-terminal devices
that have coplanar Nb electrodes coupled with a SrTiO/sub 3/
substrate. In the two-terminal devices, the Nb electrodes were
coupled with an Nb-doped SrTiO/sub 3/ substrate with a carrier
concentration of 2/spl times/10/sup 19/ cm/sup -3/. Electrode
spacing was about 50 nm. The devices showed Josephson effect
at 4.2 K. Three-terminal devices were made on a thinly doped
surface of a non-doped 0.4-mm-thick SrTiO/sub 3/ substrate
with gate electrodes on the non-doped area of the substrate.
Resistance of the three-terminal devices was controlled by
applying voltages to the gate electrode at 4.2
K. |
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Microwave
radiation from Josephson junctions built in micro-strip
line V.V. Kurin, M.Yu. Levichev,
V.A. Markelov, V.D. Gelikonova, P.A. Shisharin, S.I.
Borovitsky and A.M. Klushin
Summary: In this
paper we present the results of investigation of high
frequency dynamics of Josephson junction array built in
niobium strip line with fin-line antenna. Mutual interaction
between junctions and microwave radiation produced by the
array is investigated. |
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Resonances
in two-dimensional array oscillator
circuits P.A.A. Booi and S.P.
Benz
Summary: We present experimental results
on the emission from phase-locked two-dimensional arrays of
Josephson junctions. We have coupled the emission from 10/spl
times/10 arrays to a room-temperature mixer through a fin-line
antenna and WR-12 waveguide. A single voltage-tunable peak was
detected up to 230 GHz. A stripline resonance in antenna
reduced the array's dynamic resistance and thereby the
emission linewidth to as low as 10 kHz. We extract an
effective noise temperature of 14 K from the linewidth data.
When the array's emission was coupled to an on-chip detector
junction through a dc blocking capacitor, we detected
voltage-tunable emission from 75 GHz up to 300 GHz, and in
some circuits emission above 400 GHz. Here, the coherent power
spectrum depends on internal resonances. |
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Performance
of Josephson array systems related to fabrication techniques
and design F. Muller, J.
Kohlmann, F.X. Hebrank, T. Weimann, H. Wolf and J.
Niemeyer
Summary: Arrays of Nb/Al/sub 2/O/sub
3//Nb Josephson tunnel junctions show dc characteristics of
high quality when the trilayer is deposited direct on polished
Si wafers. Underlayers such as rf-sputtered SiO/sub 2/, can
considerably degrade the junction parameters. These results
suggest that voltage standard chips should be produced with a
cover instead of a groundplane. First results of attenuation
measurements on such circuits are presented and discussed.
Furthermore, a new and more simple fabrication process without
a window-insulating layer and only two photolithographic steps
is presented. Arrays of several thousands of junctions showed
no problems of any kind with trapped flux. |
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Josephson
voltage standard microwave circuits operating at 10
GHz H.-G. Meyer, H.-J. Kohler, G.
Wende and A. Chwala
Summary: A new type of
microwave circuit for the generation of frequency-scaled
voltages is investigated. The circuit is designed as a
superconducting microstrip line resonator and series arrays of
Josephson tunnel junctions located within the rf current
antinodes. The circuits are designed to obtain highly accurate
voltages at low rf power level and low frequencies of about 10
GHz. For a resonator circuit with 432 junctions driven at
about 10 GHz we have observed steps up to 0.25 V, the lifetime
of which is about 20 minutes. |
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Hybrid
integration of microwave oscillators with Josephson series
arrays for the use as voltage
standards F.X. Hebrank, P.
Gutmann, F. Muller, E. Vollmer and J.
Niemeyer
Summary: We have designed and
fabricated a new type of Josephson device to be hybrid
integrated with microstripline oscillators. For optimum
matching of the Josephson series array to the oscillator the
samples make use of a new stripline design. The first circuits
were fabricated in a simplified Nb/Al/sub 2/O/sub 3//Nb
technology and exhibit excellent dc characteristics and good
microwave coupling to the junctions of the array. At 70 GHz
constant voltage steps up to 350 mV could be observed. By
hybrid integrating different samples with a new 10-GHz
oscillator, constant voltage steps were created. For this
experiment the Josephson current density had to be low enough
to reduce the plasma frequency of the junctions to well below
the driving frequency. |
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Step-edge
and stacked-heterostructure high-T/sub c/ Josephson junctions
for voltage-standard arrays S.P.
Benz, C.D. Reintsema, R.H. Ono, J.N. Eckstein, I. Bozovic and
G.F. Virshup
Summary: We have explored two
high-transition-temperature Josephson junction technologies
for application in voltage standard arrays: step-edge
junctions made with YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
and Au normal-metal bridges, and stacked series arrays of
Josephson junctions in selectively doped, epitaxially grown
Bi/sub 2/Sr/sub 2/CaCu/sub 2/O/sub 8/ heterostructures. For
both kinds of junctions, Shapiro steps induced by a microwave
bias were characterized as a function of power. We compare the
technologies with respect to critical current and normal
resistance uniformity, maximum achievable critical current,
critical-current normal-resistance product, and operating
temperature. |
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High-T/sub
c/ multilayer magnetometers with improved 1/f
noise F. Ludwig, E. Dantsker, D.
Koelle, R. Kleiner, A.H. Miklich, D.T. Nemeth, J. Clarke, D.
Drung, S. Knappe and H. Koch
Summary: We have
fabricated three types of high T/sub c/ magnetometers using a
YBa/sub 2/Cu/sub 3/O/sub 7-x/-SrTiO/sub 3/-YBa/sub 2/Cu/sub
3/O/sub 7-x/, multilayer process: multiturn flux transformers
coupled to single layer dc SQUIDs in a flip-chip arrangement,
multiturn flux transformers integrated with dc SQUIDs, and
multiloop magnetometers (fractional turn SQUIDs). The magnetic
field noise of the best flip-chip magnetometer was 74 fTHz/sup
-1/2/ at 1 Hz and 31 fTHz/sup -1/2/ at 1 kHz. The magnetic
field noise of the multiloop magnetometer, measured in a YBCO
tube, was 37 fTHz/sup -1/2/ at 1 Hz and 18 fTHz/sup -1/2/ at 1
kHz. |
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Low
noise HTS gradiometers and magnetometers constructed from
YBa/sub 2/Cu/sub 3/O/sub 7-x//PrBa/sub 2/Cu/sub 3/O/sub 7-y/
thin films M.N. Keene, J.S.
Satchell, S.W. Goodyear, R.G. Humphreys, J.A. Edwards, N.G.
Chew and K. Lander
Summary: D.C. SQUID based
gradiometers and magnetometers have been fabricated using thin
films of YBa/sub 2/Cu/sub 3/O/sub 7/ and PrBa/sub 2/Cu/sub
3/O/sub 7/ on MgO substrates. Flip-chip magnetometers with 1
cm and 6.25 cm/sup 2/ substrates have been constructed. Our
device on the larger substrate with a 430 mm/sup 2/ pickup
loop had a sensitivity of (42/spl plusmn/3) fT//spl radic/Hz
above 3 Hz and (75/spl plusmn/7) fT//spl radic/Hz at 1 Hz.
Numerical simulations of d.c. SQUIDs at 77 K have been
conducted over an inductance range from 2 to 1000 pH and a
critical current range from 3.2 to 322 /spl mu/A. The results
emphasise the need to reduce SQUID inductances in order to
obtain lower flux noise. Three layer gradiometric SQUIDs with
c-axis microbridge junctions and low inductance have been
fabricated. First order gradiometric flux transformers were
also made with twin 20 turn spiral SQUID input coils and a
pair of larger area balanced sensing coils. These were mounted
with the gradiometric SQUIDs in a flip chip configuration to
complete the highly symmetrical gradiometers. Measurements at
79 K on one gradiometer gave a gradient sensitivity of (49/spl
plusmn/3) pT/m//spl radic/Hz at 300 Hz and (103/spl plusmn/7)
pT/m//spl radic/Hz at 1 Hz. |
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Low-noise,
single-layer YBa/sub 2/Cu/sub 3/O/sub 7-x/ DC SQUID
magnetometers at 77 K R. Cantor,
L.P. Lee, M. Teepe, V. Vinetskiy and J.
Longo
Summary: We describe a low-noise dc
Superconducting QUantum Interference Device (SQUID)
magnetometer that is fabricated from a single layer of YBa/sub
2/Cu/sub 3/O/sub 7-x/ on a 2 cm/spl times/2 cm bicrystal
substrate. The magnetometer design consists of a single-turn
pickup loop that is directly coupled to a low inductance
SQUID. Using conventional flux-locked loop electronics with
bias current reversal, the white flux noise of several of
these magnetometers operated at 77 K is observed to be as low
as 2.2 /spl mu//spl Phi//sub 0///spl radic/Hz above 10 kHz,
increasing to about 5.7 /spl mu//spl Phi//sub 0///spl radic/Hz
at 1 Hz. The field-to-flux conversion efficiency is measured
to be 4.6 nT//spl Phi//sub 0/, resulting in a white magnetic
field noise of to fT//spl radic/Hz above 10 kHz, increasing to
26 fT//spl radic/Hz at 1 Hz. |
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Investigation
of thin film DC SQUID gradiometer using a single YBCO
layer P. Seidel, V. Zakosarenko,
F. Schmidl, L. Dorrer, H. Schneidewind, S. Linzen, E.V.
Il'ichev and M. Darula
Summary: Thin film DC
SQUID gradiometers with a large effective pickup area using
only a single YBa/sub 2/Cu/sub 3/O/sub 7-x/ layer and step
edge Josephson junctions on SrTiO/sub 3/ substrate have been
prepared. The planar gradiometer consist of two loops coupled
directly to a small area SQUID in the center of the structure.
The main advantage in comparison to magnetometers is the
possibility of direct measurements in magnetically unshielded
environment. At 77 K without bias reversal technique we obtain
a white noise level about 3.6/spl times/10/sup -5/ /spl
Phi//sub 0//Hz/sup 1/2/ or 700 fT/cmHz/sup 1/2/. Some
peculiarities for a two SQUID arrangement with 4 Josephson
junctions are observed and simulated on the base of the RSJ
model. |
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Integrated
high-T/sub c/ SQUID
magnetometer B. David, D.
Grundler, J.-P. Krumme and O. Doessel
Summary:
We have fabricated an integrated SQUID magnetometer
based on Y/sub 1/Ba/sub 2/Cu/sub 3/O/sub 7/ step-edge
Josephson junctions. A tight coupling between the input coil
and the SQUID washer has been achieved with a coupling
coefficient K of 0.9. Noise measurements on our SQUIDs showed
a nearly frequency independent flux noise of 50 /spl mu//spl
Phi//sub 0///spl radic/Hz at 77 K. 1/f-noise contributions at
lower temperatures were always completely suppressed by bias
reversal. From our measurements of the field sensitivity and
the flux noise we can estimate a field resolution of the
magnetometer of 60 fT//spl radic/Hz down to 1
Hz. |
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Double
barrier long Josephson junctions with a contact to the
intermediate superconducting
layer H. Kohlstedt, A.V. Ustinov
and F. Peter
Summary: We demonstrate a double
barrier long Josephson tunnel junction device of overlap
geometry with an external electric contact to the middle
electrode. The junctions were fabricated with a standard
Nb/Al-AlO/sub x//Nb process. To exhibit fluxon coupling
effects in stacked junctions, the intermediate Nb layer
thickness between two barriers has to be of the order of the
London penetration depth, i.e. 90 nm for sputtered Nb films.
By using a planarization process, we were able to avoid steep
steps on the wafer and so to reduce the intermediate layer
thickness to 90 nm. Double-junction stacks with areas from
10/spl times/10 /spl mu/m/sup 2/ to 20/spl times/600 /spl
mu/m/sup 2/ were fabricated. In the best stacks, the
difference in the critical currents of two junctions was less
than 3%. Clear voltage locking effects were observed in
current-voltage (I-V) characteristics. |
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Comparison
of simulation and experiment for a Josephson fluxonic
diode F. Raissi and J.E.
Nordman
Summary: With a slight modification
to the control line and its bias configuration, a long
Josephson junction vortex flow transistor structure can become
a so-called fluxonic diode containing fluxon and antifluxon
"doped" regions in analogy to a pn junction. Such structures
have been made with Nb-Pb tunnel junctions allowing testing of
the same device with a number of different doping
configurations. This paper compares experimental results with
a one dimensional numerical simulation. Different
configurations for the diode have been modeled with
Stewart-McCumber loss parameters ranging between 50 and 1400.
The simulation clarifies the origin of a number of
experimental observations, including a peculiar dependence of
resonance induced step behavior on loss parameter, and a limit
to the value of the gradient of doping in the transition
region below which an asymmetric I-V curve representing
forward and reverse biases is obtained. In forward bias, the
I-V curve above a threshold current is roughly linear and
devoid of resonance structure, provided injection of carriers
occurs from one region to the other. Injection is a function
of loss and the asymmetry of doping. |
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Internal
resonances in periodically modulated long Josephson
junctions B.H. Larsen, J. Mygind
and A.V. Ustinov
Summary: Current-voltage
(I-V) characteristics of long Josephson junctions with a
periodic lattice of localized inhomogeneities are studied. The
interaction between the moving fluxons and the inhomogeneities
causes resonant steps in the IV-curve. Some of these steps are
due to a synchronization to resonant Fiske modes in the
sub-junctions formed between the inhomogeneities. The voltage
positions of the resonant steps oscillate as function of the
applied magnetic field with a period corresponding to the
inclusion of one magnetic flux quantum, /spl Phi//sub 0/=h/2e,
per sub-junction. A qualitative explanation that takes into
account the interaction between the resonance in the
sub-junction and the magnetic flux density waves excited in
the whole junction is given. |
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Properties
of autonomous and injection locked flux flow
oscillators J. Mygind, V.P.
Koshelets, A.V. Shchukin, S.V. Shitov and I.L.
Lapytskaya
Summary: Flux flow oscillators
(FFO) have been experimentally investigated at frequencies up
to 850 GHz. At 440 GHz the received power in an on-chip
integrated SIS mixer is 5 /spl mu/W. The first experimental
measurements of the FFO linewidth as a function of applied dc
bias current and magnetic field have been performed both for
two autonomous FFOs and with one of the FFOs injection-locked
to a narrow-band external microwave source. By beating the two
autonomous FFOs an integral spectral linewidth as low as 750
kHz is measured at 280 GHz. Mechanisms leading to a broadening
of the FFO linewidth are discussed. Experimentally it is shown
that the FFO can be used as harmonic generator. |
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Fabrication
of all-NbCN flux-flow oscillators with a tapered slotline
antenna and off-chip detection of their radiation
power S. Kiryu, S. Kohjiro, A.
Shoji, S. Kodaira, K. Kawaguchi and J.
Inatani
Summary: All-NbCN flux-flow
oscillators (FFO) with tapered slotline antenna (TSA) were
fabricated on MgO substrates. A five-step microstrip
transformer was used to couple an FFO, which has a low
impedance, to a TSA having a high impedance, The microstrip
transformer is designed to have a return loss more than 20 dB
at the center frequency. We have measured submillimeter wave
radiation from the oscillators using an off-chip
silicon-composite bolometer. Radiation from a fabricated FFO
was detected in a bias voltage range from 1.18 mV to 1.48 mV,
which corresponds to a frequency range from 570 GHz to 710
GHz. |
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Dynamics
of triangular and tetrahedral Josephson junction oscillator
arrays S.P. Yukon and N.C.H.
Lin
Summary: Triangular and tetrahedral
arrays of Josephson junctions are considered as rf oscillator
sources. Enhanced power production is possible due to a)
series rf voltages developing in junctions transverse to the
forcing current and b) modular array design. Exact solutions
are found for the basic triangular array
elements. |
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Experimental
study of fluxon resonances in window-type long Josephson
junctions N. Thyssen, A.V.
Ustinov, H. Kohlstedt, S. Pagano, J.G. Caputo and N.
Flytzanis
Summary: We report first systematic
measurements of zero-field steps in I-V characteristics of
long Nb/Al-AlO/sub x//Nb Josephson junctions made in a window
of a stripline structure. We compared the data for junction
series of the same dimensions but with different ratio of the
junction width W to the width of the idle window part W'
surrounding them. Zero-field steps were found to be stable
only in structures with W'/W<3. With increasing the ratio
W'/W, the effective fluxon propagation velocity is found to
increase and fine structure resonances appear on fluxon
resonant steps. Experimental data are compared with numerical
simulations using the modified two-dimensional sine-Gordon
equation and qualitative agreement is found. |
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Temperature
dependence and magnetic field modulation of critical currents
in step-edge SNS YBCO/Au
junctions N. Missert, L.R. Vale,
R.H. Ono, C.D. Reintsema, D.A. Rudman, R.E. Thomson and S.J.
Berkowitz
Summary: We compare the electrical
transport properties of superconductor-normal
metal-superconductor SNS step-edge YBCO/Au junctions where the
Au is deposited at 100/spl deg/C and 600/spl deg/C. For both
types of junctions we observe resistively shunted junction
current-voltage characteristics. The critical currents I/sub
c/ in all cases are similar for a given ratio of YBCO
thickness-to-step height, while the normal resistance R/sub n/
for the Au deposited at 600/spl deg/C is consistently 25%
lower than for the Au deposited at 100/spl deg/C. The
normalized temperature dependence of the I/sub c/R/sub n/
product is nearly identical for all junctions with Au
deposited at high temperatures but varies among junctions on a
single chip for Au deposited at 100/spl deg/C. Low magnetic
field modulation of the critical current can show either the
expected Fraunhofer-like pattern or a double-junction
modulation for both types of devices. The modulation period is
consistently a factor of 3 lower for the high-temperature
deposited Au. |
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Voltage-current
characteristics and noise properties of SNS
junctions A. Flett, M.S.
Colclough, Y. He, C.M. Muirhead, R.A. Robinson and K.
Char
Summary: We report measurements of V/I/B
characteristics for a number of YBCO/N/YBCO junctions where
the N layer is Co doped YBCO. The field dependence of about
half the junctions tested showed I/sub c//B characteristics
which approached 100% modulation for T>80K far field
directions both perpendicular to the plane of the junction and
along the width of the junction. Other junctions showed an
anomalous field modulation which decreased as the temperature
was increased. More detailed measurements are reported for one
junction which showed fairly large modulation. The V/I
characteristics were found to be in very good agreement with a
thermally rounded RSJ model in the temperature range 74-80 K.
The voltage noise peaked at I/sub c/, and had a 1/f dependence
in the range measured. It had a value of 8 nV Hz/sup -1/2/ at
1 Hz and 75 K. |
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Comparative
study of the stationary properties of high-T/sub c/
proximity-coupled Josephson
junctions K.A. Delin and A.W.
Kleinsasser
Summary: Much recent research
aimed at developing high temperature Josephson junctions for
electronics applications is based on superconductor-normal
metal-superconductor (SNS) edge junctions which, in some
instances, exhibit excellent current-voltage characteristics,
high critical current-resistance products, and low noise. We
review the data available in the published literature and
conclude that, despite the useful performance of these
junctions, there is little evidence that the behavior of most
reported high-T/sub c/ SNS devices can be described by
conventional proximity effect theory. |
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Co-doped-YBCO
SNS junctions for superconductive integrated
circuits A.E. Lee, J.A. Luine and
C.L. Pettiette-Hall
Summary: We have
established a high temperature superconductor SNS junction
fabrication process and are reproducibly fabricating junctions
whose behavior is rooted in the physics of the proximity
effect. SNS edge junctions are being fabricated using YBa/sub
2/Cu/sub 2.8/Co/sub 0.2/O/sub 7-/spl delta// (Co-YBCO) as the
normal barrier, and YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
(YBCO) as the superconductor. In the small junction regime,
the junctions have RSJ characteristics with I/sub c/R/sub
n//spl sim/ 50 /spl mu/V at 77 K. Junction normal resistance
values are consistent with known values of the barrier bulk
resistivity and junction geometry, indicating that the
interface resistance between YBCO and Co-YBCO is not
significant. We have demonstrated I/sub c/ and R/sub n/ 1-/spl
sigma/ spreads of 33% and 17%, respectively, for 6-junction
strings. Barrier thickness and/or morphology variations appear
to significantly contribute to these spreads. |
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Novel
tri-stable elements for binary RSFQ
circuitry D.Y. Zinoviev and O.A.
Mukhanov
Summary: A set of tri-stable RSFQ
cells has been designed, simulated, fabricated in Hypres, Inc.
using 1 kA/cm/sup 2/ low-T/sub c/ Niobium technology and
successfully tested. The elements (including a generic X cell,
XOR and inverted XOR cells) are fully compatible with binary
RSFQ circuits and do not require any input/output conversion.
Their use provides an effective way to simplify some complex
functional RSFQ blocks. We also describe a novel automated
setup for testing of digital superconductive devices which has
been used for experimental study of the cells. |
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Single
flux quantum circuits using the residue number
system Qing Ke and M.J.
Feldman
Summary: We have designed and
developed superconducting single flux quantum (SFQ) digital
signal processing circuits using the residue number system
(RNS). RNS arithmetic is a complete alternative to binary
arithmetic for performing digital computations, which appears
to have many advantages for SFQ circuits. We present a scheme
for performing all RNS arithmetic functions using Josephson
shift registers alone, and suggest that this Is advantageous
for high-temperature superconductor computational circuits. We
have designed a one-decimal-digit adder, realized with
Nb-based superconducting circuitry. Its most complex
component, the mod5 adder, has been simulated to show perfect
functionality and subcell simulated margins are compared with
the experimental results. |
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Design
and operation of a Quantum Flux Parametron bit-slice
ALU W. Hioe, M. Hosoya, S.
Kominami, H. Yamada, R. Mita and K. Takagi
Summary:
The design of Quantum Flux Parametron (QFP) majority
logic circuits presents a number of unique constraints. For
example, interconnects must be kept short and have a common
small inductance. The former suggests that the bit-slice
architecture is well suited to QFP circuits. In order to test
this conjecture, a suitably complex logic circuit was designed
and a small part of it was fabricated. A design for a
16-function bit-slice arithmetic-logic unit (ALU) was found
that satisfied the constraints. It can compute on n-bit
operands in 2n+4 QFP stages. A reduced version of the
bit-slice ALU cell, containing 30 QFP's, was fabricated and
successfully tested at low speed. The design experience showed
that complex combinatorial QFP logic circuits are possible.
Larger circuits will be feasible with computer-aided
tools. |
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A
Single Flux Quantum cross-bar switch and
demultiplexer A.H. Worsham, J.X.
Przybysz, Joonhee Kang and D.L. Miller
Summary:
A Single Flux Quantum (SFQ) demultiplexer and a
cross-bar switch for a high speed data switch are described.
Both circuits were error-free in simulation to 15 Gbps. The
cross-bar switch was two input, two output (2/spl times/2) and
used /spl sim/400 /spl mu/A control signals to set the data
path. The switch has been demonstrated at over 15 Gbps/line
using average voltage measurements. The correct routing of a
bit stream was demonstrated at 2.488 Gbps. |
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Rapid
single flux quantum random access
memory S.V. Polonsky, A.F.
Kirichenko, V.K. Semenov and K.K. Likharev
Summary:
A new design concept for the Josephson-junction random
access memory (RAM) has been developed. In contrast to
previous RAMs based on single flux quantization (SFQ), in our
system READ and WRITE operations employ ballistic transfer of
SFQ pulses along bit lines (either Josephson transmission
lines, or passive superconducting microstrip lines, or their
combination). The basic memory cells are the single-junction
SQUIDs, connected serially by the bit lines and inductively
coupled to word lines. READ and WRITE operations are performed
by sending SFQ pulses in appropriate directions along bit
lines, and DC currents of appropriate polarity into word
lines. This approach allows design of very dense memories with
n/spl les/2 Josephson junctions per bit, memory cell area
smaller than 80 /spl lambda//sup 2/ (where /spl lambda/ is the
minimum feature size), and the critical parameter margin well
above /spl plusmn/20%. In this paper we present the general
structure of the RSFQ RAM, as well as design and results of
testing of the basic memory cell and decoder circuitry using
Hypres' 3.5-/spl mu/m, 1-kA/cm/sup 2/ Nb-trilayer
technology. |
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Adder-accumulator
cells in RSFQ logic S.S.
Martinet, D.K. Brock, M.J. Feldman and M.F.
Bocko
Summary: We are in the process of
designing a Finite Impulse Response (FIR) filter for use in a
Digital Signal Processing (DSP) system based entirely on Rapid
Single Flux Quantum (RSFQ) logic. One aspect of this project
involves the development of the arithmetic unit of the filter,
in this case an adder-accumulator multiplier. This article
describes two cells can perform the function of accumulated
addition in the adder-accumulator multiplier. We have
fabricated both cells and tested them at low
speed. |
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Implementation
of novel "push-forward" RSFQ Carry-Save Serial
Adders A.F. Kirichenko and O.A.
Mukhanov
Summary: We have developed a novel,
so-called "push-forward" design approach in Rapid
Single-Flux-Quantum (RSFQ) logic. This approach leads to a
more efficient circuit design at the gate level using fewer
Josephson junctions combined with reasonable circuit parameter
margins. Other advantages include higher operational speed and
smaller power dissipation. This novel method is based on a
specific type of interaction (pushing forward) between single
flux quanta already stored by RSFQ gates and newly arriving
data SFQ pulses. It implies a reuse of an internal gate memory
as well as realization of multi-quantum storage. Using this
push-forward design approach, we have designed, optimized,
fabricated, and successfully tested two versions of Carry-Save
Serial Adders for digital signal processing
applications. |
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Ta-based
tunnel junctions for energy resolving X-ray
detection M.G. Blamire, F.S.
Porter, E.C.G. Kirk and K. Van Vechten
Summary:
We report the results of a programme to develop an
energy-resolving superconducting tunnel junction based on a Ta
X-ray absorber. The design is based on a vertical
heterostructure consisting of a Nb underlayer to act as a
quasiparticle reflector, a thick Ta absorber layer and an Al
trap layer. The upper surface of this trap layer is oxidised
to form the tunnel barrier. The counterelectrode consists of
an Al and thin Nb layer with thicknesses controlled to give
approximately equal energy gaps in both electrodes and minimal
absorption in the Nb counterelectrode. The effect of
electro-magnetic barrier resonances on detection performance
has been evaluated. Very high quality junctions have been
fabricated, tested and evaluated for X-ray energy
resolution. |
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Response
of Nb-based tunnel junctions to synchrotron
radiation K. Ishibashi, T. Noda,
K. Maehata, H. Nakagawa, H. Akoh, S. Takada, T. Nakashima,
H.M. Shimizu, M. Yoshizawa and M. Katagiri
Summary:
Superconducting tunnel junctions have potential high
energy-resolution for X-ray detection. The excellent
performance may be suited for experiments making use of X-rays
from a synchrotron radiation. The characteristics of the
Nb-based junction were studied to know the response of
Nb-based junctions to the synchrotron radiation. We obtained
the dependence of the detector pulse height on X-ray energies
in a range of 4 to 15 keV. |
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Quasiparticle
lifetimes in epitaxial niobium and tantalum
films P.A. Warburton and M.G.
Blamire
Summary: By using three-terminal
double tunnel junction devices at 2.2 K we have injected
quasiparticles into epitaxial thin films of niobium and
tantalum. The two junctions are coupled by quasiparticle
diffusion and the diffusion of recombination phonons through
the sapphire substrate. A comparison of our experimental
results with a random walk simulation of the quasiparticle
diffusion process enabled us to estimate the lifetime of the
injected quasiparticles. The quasiparticle lifetime is not
recombination limited in epitaxial Nb and Ta films.
Furthermore Ta is less susceptible to the (as yet
undetermined) loss mechanisms which govern the quasiparticle
lifetime. This result indicates that tunnel junction particle
spectrometers utilising Ta absorbers may display better energy
resolution than those with Nb absorbers. |
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Suppression
of extrinsic resolution limiting factors in epitaxial
superconducting tunnel junction
detectors F.S. Porter, D. Van
Vechten, M.G. Blamire and E.C.G. Kirk
Summary:
Superconducting tunnel junctions have been shown to
have potential as high resolution X-ray detectors. Recent
reductions in the noise environment of our experiment have
yielded a substantial increase in the resolution of our Nb/Ta
junctions. The junctions used in the experiment are epitaxial
base layer devices including a thick Ta absorber and have
survived more than 30 cycles to low temperatures. Current
experiments with a /sup 55/Fe source have yielded an energy
resolution of 68 eV at 5.89 keV with a quantum efficiency of
13%. Additional measurements using a higher energy /sup 109/Cd
source are also reported. We discuss how a reduction of
extrinsic and quasi-extrinsic noise sources affects the
performance of the detectors and why we believe we are still
not observing the intrinsic limitations of these
junctions. |
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Modeling
the spectra of superconducting tunnel junction x-ray
detectors D. Van Vechten, F.S.
Porter, K.S. Wood, M.G. Blamire and E.C.G.
Kirk
Summary: SIS tunnel junctions (STJD) are
predicted to have exceptionally good energy resolution as
x-ray detectors. This paper spectra illustrative of the
current state of the art. They were obtained when /sup 55/Fe
and /sup 109/Cd x-ray sources bombarded an epitaxial base
layer Nb/Ta/Al/AlO/sub x//Al/Nb junction having a diamond
shape and sides 15 microns long. Our model of energy loss via
the escape of photoelectrons early in the energy cascade is
demonstrated to lie qualitatively correct. Earlier results
based on fine-grained junctions suggested that such small area
devices will have a large characteristic "foot" (asymmetric
broadening of low energy side) on the peaks in the spectra
that correspond to complete capture of the incident energy in
the device. Our device is small, yet its full energy peaks
lack significant feet. We conclude that this device is in the
fast diffusion limit. This result contradicts the suggestion
that Andreev reflection should severely restrict lateral
diffusion in clean superconducting bilayers. |
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Low-energy
response of superconducting tunnel junction X-ray
spectrometers S.E. Labov, L.H.
Hiller, C.A. Mears, M. Frank, H. Netel, F. Azgui and A.T.
Barfknecht
Summary: Thin film structures
incorporating metallic superconducting layers and tunnel
junctions can be configured as low-energy X-ray spectrometers.
We present results obtained when low-energy X-rays are
absorbed in niobium films coupled to aluminum layers that
serve as quasiparticle traps in an Nb/Al/Al/sub 2/O/sub
3//Al/Nb tunnel junction X-ray detector. The linearity of the
pulse height as a function of energy Is discussed along with
the energy dependence of the observed resolution and its
relation to the broadening mechanisms. A resolution of 14 eV
at 1 keV has been measured with our detector cooled to 0.3
K. |
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New
modes guided by a thin superconducting
film O. Buisson and J.
Richard
Summary: New modes guided by an
aluminum superconducting film deposited on a SrTiO/sub 3/
dielectric have been observed in the 100 MHz-1 GHz frequency
range. Such modes have been understood as a propagating plasma
modes of the superconducting electrons. We present impedance
measurements which indicate plasma modes resonances. An
equivalent electrical circuit is proposed in order to simulate
the frequency dependent impedance of our sample. |
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High
speed current switching of homogeneous YBaCuO film between
superconducting and resistive
states B.S. Karasik, I.I.
Milostnaya, M.A. Zorin, A.I. Elantev, G.N. Gol'tsman and E.M.
Gershenzon
Summary: Transitions of thin
structured YBaCuO films from superconducting (S) to normal (N)
state and back induced by a supercritical current pulse has
been studied. A subnanosecond stage in the film resistance
dynamic has been observed. A more gradual (nanosecond) ramp in
the time dependence of the resistance follows the fast stage.
The fraction of the film resistance which is attained during
the fast S-N stage rises with the current amplitude.
Subnanosecond N-S switching is more pronounced for smaller
amplitudes of driving current and for shorter pulses. The
phenomena observed are viewed within the framework of an
electron heating model. The expected switching time and
repetition rate of an optimized current controlling device are
estimated to be 1-2 ps and 80 GHz respectively. |
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A
superconducting microwave
switch G.D. Poulin, F.A. Hegmann,
J. Lachapelle, S.H. Moffat and J.S. Preston
Summary:
We describe a superconducting microwave switch. The
switch comprises a tapering microwave transmission line which
can he switched from a very low loss ON state to a high
impedance OFF state with a DC voltage applied to the
transmission line through a bias-tee. Switching is essentially
thermal in nature, occurring due to the formation of a 'hot
spot' in the transmission line. Thermal runaway is avoided
through the use of voltage rather than current biasing. Once
switched, the transmission line attenuates the applied
microwave signal. An isolation of 20 dB is readily achievable.
The intrinsic response time of the hot spot to applied
microwave fields was estimated to be approximately 1 /spl mu/s
by measuring the frequency dependence of the transmitted
signal. |
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Multilayer
ferroelectric-high T/sub c/ structures with poled
ferroelectric layers G.L. Larkins
Jr., M.Y. Avello, J.B. Boyce and D.K. Fork
Summary:
We have observed shifts of from 0.5 to -6/spl deg/K in
the T/sub C(ONSET/) of YBa/sub 2/Cu/sub 3/O/sub 7-x/(123) in
laser ablated thin film 123-BaTiO/sub 3/ multilayer structures
on (100) oriented LaAlO/sub 3/ upon poling of the BaTiO/sub 3/
with a positive potential. Poling was carried out at between
120 and 150/spl deg/C in air with an applied field of about
10/sup 5/ V/cm after which a positive shift in the T/sub
C(ONSET/) of the 123 by an amount of approximately 1/spl deg/K
was observed. Samples were also poled at room temperature
(20/spl deg/C) with an applied field of 10/sup 6/ V/cm
(2-6/spl deg/K shift observed depending on T/sub c/ (R=0)).
Negative potentials showed no apparent shift in T/sub
C(ONSET/). A dc-poling with no applied field at 150/spl deg/C
for 10-30 minutes in air was observed to restore the R vs. T
curve to its original, unpoled, state. Details of the
deposition parameters, structures and the mast recently
obtained results will be presented possible explanations for
the effect will also be discussed. |
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Low-noise
slot antenna SIS mixers J.
Zmuidzinas, N.G. Ugras, D. Miller, M. Gaidis, H.G. LeDuc and
J.A. Stern
Summary: We describe quasi-optical
SIS mixers operating in the submillimeter band (500-750 GHz)
which have very low noise, around 5 h/spl nu//k/sub B/ for the
double-sideband receiver noise temperature. The mixers use a
twin-slot antenna, Nb/Al-Oxide/Nb tunnel junctions fabricated
with optical lithography, a two-junction tuning circuit, and a
silicon hyperhemispherical lens with a novel antireflection
coating to optimize the optical efficiency. We have flown a
submillimeter receiver using these mixers on the Kuiper
Airborne Observatory, and have detected a transition of H/sub
2//sup 18/O at 745 GHz. This directly confirms that SIS
junctions are capable of low-noise mixing above the gap
frequency. |
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Integrated
sub-MM wave receivers V.P.
Koshelets, S.V. Shitov, A.M. Baryshev, I.L. Lapitskaya, L.V.
Filippenko, H. van de Stadt, J. Mees, H. Schaeffer and T. de
Graauw
Summary: The concept of a fully
integrated superconducting receiver looks very attractive for
sub-mm space astronomy where low weight, power consumption and
volume are required. The possibility to integrate on a few
chips the different planar components: a SIS mixer, a
superconducting local oscillator (LO), an intermediate
frequency amplifier followed by superconducting circuits for
digitizing and processing of down converted signals, is
discussed. A first implementation of a real integrated
quasioptical receiver for frequencies up to 500 GHz is
described. The one-chip receiver comprises a double dipole
antenna, parallel biased SIS array mixer and Josephson Flux
Flow Oscillator (FFO) with matching circuits. The results of
extensive investigations of the integrated receiver as well as
design and investigation of novel superconducting elements are
presented. |
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30
THz mixing experiments on high temperature superconducting
Josephson junctions E.N.
Grossman, L.R. Vale, D.A. Rudman, K.M. Evenson and L.R.
Zink
Summary: We have investigated YBa/sub
2/Cu/sub 3/O/sub 7-/spl delta//
superconductor-normal-superconductor Josephson junctions as
mixers of 30 THz radiation. We have directly observed (2nd
order) difference frequencies from 10 MHz to 12.8 GHz between
two CO/sub 2/ laser lines. Applying a third microwave signal
to the junction, we have observed CO/sub 2/ laser difference
frequencies up to 27 GHz. The d.c. bias dependence of the
difference frequency signal, as well as other evidence,
suggests two distinct mixing mechanisms: hot-electron mixing
in the junction banks at high d.c. biases, and bolometric
Josephson mixing at low d.c. biases. The latter is the first
observation of Josephson mixing at CO/sub 2/ laser frequencies
in high-T/sub c/ junctions. The Josephson mixing has generated
observable mixing products up to 6th order. |
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NbN
hot electron superconducting mixers for 100 GHz
operation G.N. Gol'tsman, B.S.
Karasik, O.V. Okunev, A.L. Dzardanov, E.M. Gershenzon, H.
Ekstrom, S. Jacobsson and E. Kollberg
Summary:
NbN is a promising superconducting material for
hot-electron superconducting mixers with an IF bandwidth
larger than 1 GHz. In the 1OO GHz frequency range, the
following parameters were obtained for 50 /spl Aring/ thick
NbN films at 4.2 K: receiver noise temperature (DSB) /spl
sim/1000 K; conversion loss /spl sim/10 dB; IF bandwidth /spl
sim/1 GHz; and local oscillator power /spl sim/1 /spl mu/W. An
increase of the critical current of the NbN film, increased
working temperature, and a better mixer matching may allow a
broader IF bandwidth up to 2 GHz, reduced conversion losses
down to 3-5 dB and a receiver noise temperature (DSB) down to
200-300 K. |
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High-resolution
superconducting X-ray spectrometers with aluminum trapping
layers of different
thicknesses C.A. Mears, S.E.
Labov, L.H. Hiller, M. Frank, H. Netel, F. Azgui and A.T.
Barfknecht
Summary: Superconducting tunnel
junctions coupled to superconducting absorbers may be used as
high-resolution, high-efficiency X-ray spectrometers. We have
tested devices with niobium X-ray absorbing layers coupled to
aluminum layers that serve as quasiparticle traps. We present
a study of device performance as a function of thickness of
the trapping layers. We measured the best energy resolution
using a device with a high-quality barrier and 200 nm-thick
trapping layers on both sides of the tunnel barrier. This
energy resolution was 36 eV full width at half maximum at 6
keV, about 4 times better than that obtainable using
semiconductor ionization detectors. |
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Subgap
characteristics of Nb/AlOx/Nb tunnel junctions with high
critical current density M.
Maezawa, M. Aoyagi, H. Nakagawa, I. Kurosawa and S.
Takada
Summary: We have investigated subgap
characteristics of Nb/AlOx/Nb tunnel junctions with high
critical current density (high-J/sub c/). A good agreement of
the experimental data with the solution of Werthamer's
equation clearly shows that steep current steps observed at
odd submultiples of the gap voltage, which cannot be explained
by multiparticle tunneling and/or multiple Andreev reflection,
are mainly caused by Josephson self-coupling. Our experimental
results suggest that Josephson self-coupling is important to
high-J/sub c/ tunnel junctions. |
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Characterization
of Andreev reflection barriers by low frequency noise
spectroscopy in all-thin-film superconducting point
contacts K. Hamasaki, T. Ikuta,
A. Tachibana and T. Fukumoto
Summary:
Low-frequency noise properties of all-thin-film
superconducting point contacts have been investigated. Device
characterization is also reported here. The quasi particle
behavior is well explained by the Andreev reflection. The
low-frequency noise spectral density scaled by frequency and
normal resistance is studied as a function of junction
(contact) resistance. |
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Effect
of temperature on the resonant macroscopic quantum tunneling
in small Josephson junctions B.
Ruggiero and P. Silvestrini
Summary: The
study of the quantum behaviour of Josephson junctions is
interesting not only by itself, but also for the technological
importance in electronics employing superconducting weak
links. Recently great attention has been devoted to the
effects of Resonant Macroscopic Quantum Tunneling (RMQT)
between levels the same energy in neighbouring wells of the
potential shape describing the junction. This can produce
voltage spikes along the supercurrent branch of the I-V curves
and peaks in the current switching distributions. Schmidt,
Clealand, and Clarke have presented a detailed analysis of the
resonant tunnel dynamics for the T=0 case. The present paper
is based on a different theoretical approach, first proposed
by Larkin and Ovchinnikov, which allows one to include
explicitly the temperature. We study the phenomenon in its
time dependence and this allows us to consider the lifetime of
the voltage spikes as well as the effect of the RMQT on the
quantum escape rate out of the V=0 state. |
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Advantages
of superconducting Coulomb-blockade
electrometers D. Song, A. Amar,
C.J. Lobb and F.C. Wellstood
Summary: We have
measured the current-voltage gate charge characteristics and
noise in superconducting Coulomb-blockade electrometers from
50 mK to 1.05 K. The Al-AlO/sub x/-Al junctions in our devices
have capacitances which range from 0.3 fF to 1 fF and
tunneling resistances from 20 k/spl Omega/ to 200 k/spl
Omega/. We find that our normal and superconducting
electrometers have comparable charge noise but that the latter
have much larger modulation which persists to significantly
higher temperatures. The maximum operating temperature in the
superconducting state is close to T/sub c/. This behavior Is
consistent with a simple model and makes the superconducting
electrometer preferable for many applications. |
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Electrical
field effect in highly resistive NbN
microbridge N. Yoshikawa, N.
Miura, Xiao Chen, K. Yokoyama and M.
Sugahara
Summary: We investigate conduction
properties and electrical field effect of highly resistive NbN
microbridges. The bridge region consists of NbN thin films
which have granular structure with /spl sim/10 nm. The
dimension of the microbridge is approximately /spl sim/200 nm
in length and /spl sim/50 nm in width. The highly resistive
(100 k/spl Omega/) microbridges exhibit nonlinear
current-voltage (I-V) characteristics at low temperatures
which are similar to those of an array of single electron
tunneling (SET) junctions. The offset voltage ranges from 2 mV
to 300 mV at 4.2 K depending on the bridge resistance and the
bridge width. Periodic modulation of bridge conductance is
observed when external gate electric field is applied to the
bridges. These results coincide fairly well with the
simulation based on the SET array model. |
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Complex
dynamical behavior in RCL-shunted Josephson
junctions C.B. Whan and C.J.
Lobb
Summary: We present numerical simulation
results on the dynamical behavior of resistively, capacitively
and inductively shunted Josephson tunnel junctions (RCLSJ). We
found Josephson oscillations, chaotic oscillations,
subharmonic oscillations and relaxation oscillations dominate
the dynamics of the circuit in this order as we increase the
inductance of the shunt. Long apparently chaotic transient
states were found in the intermediate range values of the
shunt inductance. Difficulties in comparing simulation with
experiments due to the existence of the long transients are
discussed. |
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Reduction
of telegraph noise in superconducting short weak
links H. Ohta, T. Matsui, K.
Shinada, Y. Yamada, T. Munaka and Y.
Fujiyama
Summary: It has been proved that, in
the large channel number limit, the Josephson current of short
weak links derived with a quantum mechanical scattering theory
is analytically equal to the Josephson current derived with a
classical transport equation in the dirty limit. It means that
the former expression of the Josephson current can explain
temperature dependence of the maximum critical current of
short weak links in the dirty limit as well as in the clean
and tunnel limits. The proved generality of the expression of
the Josephson current helped us find a reproducible method to
reduce telegraph noise in devices of short weak links and get
a 130-channel dc-SQUID system. |
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Synchronous
switching in vertically stacked Josephson
junctions H. Yamamori, A.
Fujimaki, Y. Takai and H. Hayakawa
Summary:
Vertically stacked Josephson junctions with different
thickness of 2, 4, 8, 14, 20, 40 nm for the intermediate
electrode have been experimentally investigated. In the double
junction, the synchronous switching between the lower and
upper junctions is observed. Though simultaneous switching is
also observed in the series-connected Josephson junction, some
differences only in the double junction with thin intermediate
Nb layer such as 4 nm or 8 nm are observed. We have also
fabricated three stacked junctions and four stacked junctions
and have investigated the magnetic field dependence of the
critical currents. |
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Three-terminal
Josephson device with direct bias-current controlled phase
difference I.P. Nevirkovets, M.G.
Blamire and J.E. Evetts
Summary: We have
fabricated and characterized the Nb/Al-AlO/sub
x/-Nb/Al-AlO/sub x/-Nb three-terminal double junction
Josephson device in which the phase difference across the
whole device is controlled by the tunnel current flowing
through one of the junctions. The device reveals current gain
about 10 and has good isolation of the input and output
circuits. |
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Single
layer YBaCuO-gradiometer G.M.
Daalmans, L. Bar, M. Kuhnl, D. Uhl, M. Selent and J.
Ramos
Summary: A single layer
YBaCuO-gradiometer galvanically coupled to DC-SQUIDs were
prepared on bicrystal substrates. The devices were operated at
77 K without any shielding. The best performance obtained was
a field gradient resolution of 0.5 pT/cm/spl radic/(Hz) for a
device with a baseline of 7 mm and a pickup-area of 2 cm/sup
2/. |
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Noise
performance of high-T/sub c/ DC SQUID
magnetometers A.A. Fife, G.
Anderson, V. Angus, C. Backhouse, K. Betts, M.B. Burbank, R.A.
Cragg, K. Ferguson, F. Habib, P.R. Kubik, J. Nomura, M. Smith,
P. Spear, W. Westera, H. Zhou, J. Vrba, B. Heinrich, A.E.
Curzon, J.C. Irwin, J. Chrzanowski, X.M. Burany, S. Govorkov,
P. Brown and W.B. Xing
Summary: High-T/sub c/
DC SQUID magnetometers operating at 77 K have been fabricated
from epitaxial YBCO and SrTiO/sub 3/ films and characterized.
The DC SQUID washers incorporated either bicrystal or
step-edge microbridge junctions of widths down to about 3 /spl
mu/m. Three types of DC SQUID magnetometer are described-(a) a
single layer device with a direct-coupled loop; (b) a DC SQUID
plus flip-chip coupled flux transformer; (c) a fractional turn
device with a direct-coupled multi-loop. The 1/f noise in the
spectra of uncoupled DC SQUIDs and some magnetometers is
significantly reduced by using AC bias modulation. Low
frequency energy sensitivities of uncoupled SQUIDs at 77 K
have been improved by use of AC bias to 7/spl times/10/sup
-30/ J/Hz at 1 Hz (45 pH inductance). For flip-chip coupled
magnetometers (15-turn input coil, pick-up coil area 13 mm/sup
2/), excess low frequency noise was observed, only partially
reduced by AC biasing, with field sensitivities of 1 pT
rms//spl radic/(Hz) and 130 fT rms/spl radic/(Hz) above 200
Hz. |
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DC
SQUID magnetometers with the directly coupled pick-up
loop Keunseop Park, Soon-Gul Lee,
Hyuk Chan Kwon, Yong Ki Park and Jong-Chul
Park
Summary: DC SQUID magnetometers with a
directly coupled square pick-up loop have been made from
single layer YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// thin
films using step edge junctions or bicrystal grain boundary
junctions on SrTiO/sub 3/ substrates. YBa/sub 2/Cu/sub 3/O/sub
7-/spl delta// thin films were deposited by off-axis RF
sputtering or laser ablation and patterned by photolithography
and Ar ion milling to form the SQUID, pick-up loop and
modulation coil. The SQUIDs showed RSJ like current vs.
voltage characteristics and voltage modulation in response to
external fields at 77 K. The SQUID inductance was 55-140 pH,
pick-up loop size was 47 mm/sup 2/ and the effective area of
magnetometers estimated from the measured modulation period
was 0.2-0.4 mm/sup 2/. The magnetic field noise was 7.4/spl
times/10/sup -13/ T//spl radic/(Hz) at 10 Hz and 77
K. |
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Nonlinear
response in thin film magnetometer sense loops at 77
K J.W. Purpura, T.R. Clem and
R.F. Wiegert
Summary: The onset of nonlinear
response to applied magnetic field in GdBa/sub 2/Cu/sub
3/O/sub 7-/spl delta// thin film magnetometer sense loops was
measured in equipment performing at 77 K. As the magnetic
field applied to the magnetometers was ramped, the output
magnetic flux of the sense loops was monitored with a YBa/sub
2/Cu/sub 3/O/sub 7-/spl delta// DC superconducting quantum
interference device flip-chip coupled to the loop sample's
output washer. In experiments devised to minimize circulating
current in the magnetometers, nonlinear onset fields ranging
from 26 to 120 /spl mu/T were measured for samples having
linewidths ranging from 20 to 800 /spl mu/m. The loops also
exhibited hysteresis in conjunction with the nonlinear
behavior. These results indicate that nonlinear hysteresis is
an issue for magnetometer loops operating in the Earth's
field. |
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Electromagnetic
nondestructive evaluation with simple HTS SQUIDs: measurements
and modelling L.N. Morgan, C.
Carr, A. Cochran, D.McA. McKirdy and G.B.
Donaldson
Summary: For AC EM NDE research,
the field sensitivity of a SQUID should be around 100 pT, in a
bandwidth of 5 Hz or less in the frequency range from 1 Hz to
10 kHz or more. Existing HTS SQUIDs and commercial electronics
can already satisfy these demands. Moreover, the small size of
HTS SQUIDs and the large dynamic range of SQUID systems permit
measurements even in some magnetically unshielded
environments. Here, we describe non-contacting AC EM NDE with
a simple, small, single layer HTS SQUID. We present results
demonstrating the detection of a subsurface feature in
aircraft-grade aluminium by horizontal field measurement.
Although they indicate the potential usefulness of HTS SQUIDs,
variation between nominally identical data has been much
greater than expected. This is because of fundamental HTS
SQUID problems and the fact that experimental constraints on
SQUID position, induction coil geometry and stand-off led to a
far from optimum system design. We have analysed the problem
using FEM; here we present selected results and indicate how
they may affect future designs. |
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Integration
of step-edge grain boundary Josephson junctions with YBCO
multilayers for electronics
applications K.P. Daly, J.M.
Murduck, C.L. Pettiett-Hall and M. Sergant
Summary:
We discuss our multilayer YBCO process which uses
step-edge junctions. Key issues are dielectric defect density,
wiring layer critical current over edges of underlying
features and junction critical current uniformity. We have
demonstrated an average defect density of about 450/cm/sup 2/
over many wafers. Wiring critical current exceeds 1 mA//spl
mu/m of line width. We have demonstrated SQUIDs at 77 K using
this process. |
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Process
issues and components for HTS digital integrated circuit
fabrication A.P. Marathe, F.
Ludwig, T. Van Duzer and L. Lee
Summary: An
etch-back planarization technique has been developed to
planarize SrTiO/sub 3/ insulating layers, which may be used in
a YBCO IC process. Films of YBCO have been deposited on the
planarized SrTiO/sub 3/ surface. Structural and electrical
characterization of these films suggests that the planarized
surface can support the growth of epitaxial, c-axis oriented
YBCO films. Experiments to evaluate and compare coupling
efficiency in YBCO and Nb thin film transformers are also
described. Easy flux penetration in YBCO films may reduce the
efficiency of transformer coupling below that found for Nb
transformers. The current coupling for Nb transformers, as
extracted from the SQUID threshold curves, was found to be
high (M/L/spl sim/0.93). The coupling in YBCO transformers, as
measured from the voltage modulation of bicrystal grain
boundary junction SQUIDs, was found to be much lower (M/L/spl
sim/0.75). |
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Properties
of passive structures for multilayer HTS digital
circuits J. Talvacchio, M.G.
Forrester and J.R. Gavaler
Summary: The
passive structures required for HTS digital circuits that must
be formed at high temperature (650-750/spl deg/C) were
evaluated by fabricating crossovers, vias, YBCO/YBCO contacts,
and multiple coverage of steps with trilayer structures of
YBCO/epitaxial insulator/YBCO. Two insulator materials were
used, high-/spl epsiv/ SrTiO/sub 3/ and relatively low-/spl
epsiv/ Sr/sub 2/AlTaO/sub 6/ (SAT). The deposition conditions
for both insulators had to be optimized to simultaneously
obtain smooth surfaces, sufficiently high oxygen diffusion
rates to re-oxidize underlying YBCO, and resistivities in
planar capacitor structures of >10/sup 9/ /spl Omega/-cm at
77 K. The particular process used to clean film surfaces after
photolithography and Ar ion milling was also critical in
obtaining smooth surfaces for a subsequently deposited film
layer. For the non-planar capacitor structures formed at
crossovers, the effective resistivity of insulators decreased
as a function of linewidth, particularly for lines less than
10 /spl mu/m wide. However, even for narrow lines patterned in
the top YBCO layer, critical current densities, J/sub c/(77
K), exceeded 106 A/cm/sup 2/. |
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Vertical
c-axis microbridge junctions in YBa/sub 2/Cu/sub 3/O/sub
7//PrBa/sub 2/Cu/sub 3/O/sub 7/ thin
films S.W. Goodyear, N.G. Chew,
R.G. Humphreys, J.S. Satchell and K. Lander
Summary:
The fabrication and measurement of microbridge
junctions in the vertical c-axis direction of YBCO/PBCO/YBCO
evaporated thin films is described. Single junctions show
critical current modulation with applied magnetic field, the
period scaling with junction size. The IV characteristics show
Shapiro steps to high order when irradiated with microwaves.
Initial measurements of linear arrays suggest that with
further optimisation of the processing steps a reproducible
junction technology could emerge. Very low inductance (L/spl
ap/5-15 pH) SQUIDs have been demonstrated with dV/d/spl
Phi/>1 mV//spl Phi//sub 0/ at 50 K. The vertical SQUID loop
geometry of these SQUIDs has allowed a direct determination of
the penetration depth as a function of
temperature. |
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Multilayer
Josephson junction flux quantum
devices S. Lomatch, E.D. Rippert
and J.B. Ketterson
Summary: We describe the
properties of flux quantum circuitry employing the relatively
young technology of multilayer Josephson junctions with n
superconductor-insulator (SI) layers. Multilayer junctions can
be employed as both passive and active devices to increase
circuit integration density, allow for new logic/voltage
thresholds and higher impedances, and improve thermal noise
stability. We present the results from numerical simulations
of a conventional RSFQ circuit and two novel circuits with
multilayer junction designs. Neural circuitry is a focus of
our novel multilayer designs. We also discuss layout and
fabrication issues, considering the recent progress in the
fabrication of Nb multilayer junctions with AlN tunnel
barriers, which exhibit intrinsic overdamping at the level of
each SI layer. Included in this discussion is a long term
assessment of a multilayer approach in view of deep sub-micron
and high T/sub c/ technologies. |
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Broadband
interfacing of superconducting digital systems to room
temperature electronics D.F.
Schneider, J.C. Lin, S.V. Polonsky, V.K. Semenov and C.A.
Hamilton
Summary: We have developed and
tested simple and inexpensive electronics for interfacing
Rapid Single-Flux-Quantum (RSFQ) Josephson-junction circuits
to room temperature digital systems. Voltage-level
(Non-Return-to-Zero) bit signals with a swing of /spl sim/150
uV, developed on-chip by standard SFQ/DC converters, and in
some cases amplified to 1.5 mV swing by HUFFLE-type circuits,
are passed to the 300 K environment using a high density (40
channel) flexible coplanar waveguide assembly. AC-coupled, 2-3
stage microwave Si-bipolar amps, and Emitter-Coupled-Logic
(ECL) buffers accomplish voltage level translation to the
standard ECL levels, Using this technique, data rates in
excess of 1 Gb/s per channel can be achieved at low cost per
channel,. |
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Ultrafast,
integrable, optics-based interface between superconducting and
room-temperature
electronics Chia-Chi Wang, M.
Currie and T.Y. Hsiang
Summary: An ultrafast
optical interface between superconducting and room-temperature
electronics is proposed to take full advantage of high-speed
superconducting circuits. We report on the computed and
experimental studies of an optical receiving and modulating
system that is compatible in processing with the prevailing
integrated-superconducting-circuit technology. Planar
interdigitated Nb/Si/Nb metal-semiconductor-metal (MSM)
photodiodes are demonstrated as optical receivers with
resolvable bit-rate as high as 38 Gb/s, and the response of
MSM diode was shaped to be a single-flux-quantum pulse to
drive Josephson-junction-based circuits. A similar
interdigitated structure on a silicon waveguide is proposed to
be an ultrafast light-intensity modulator, with its operation
based on carrier-density modulation of the optical index of
refraction. This field-effect device has insignificant power
dissipation, in addition to high speed. A sample modulator
with 5-V bias is shown to have a modulation depth of 40% and a
bandwidth over 70 GHz. |
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Multi-chip
packaging for high speed superconducting
circuits R.D. Sandell, G.
Akerling and A.D. Smith
Summary: We report
the development of a multi-chip module (MCM) technology using
Nb metallization and benzocyclobutene (BCB) polymer
dielectric. The Nb/BCB structure displays very low loss, has
low processing temperature, and forms a wide range of
microstrip transmission line impedances. We are developing
flip chip, solder attachment for die mounting. We also report
the electrical characterization of Nb/BCB/Nb for both
microstrip resonators, delay lines, and bandpass
filters. |
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A
superconductive ring-pipelined network
system S. Tahara, S. Yorozu and
H. Matsuoka
Summary: A superconductive
ring-pipelined network system is proposed to improve
performance of multi-processor systems, and a prototype chip
is designed. A throughput of a data exchange between processor
elements limits the effective performance of the
multi-processor systems. The features of the superconductive
ring-pipelined network system are a high-clock-frequency
operation by using high-speed Josephson gates and wide band
superconductive transmission lines, and a high-density package
because of its low power consumption. These advantages
significantly reduce pipeline loss and improve flexibility in
data exchange. Therefore, this network system is capable of
improving the overall effective performance of multiprocessor
systems. The prototype chip consists of three Josephson ring
interface circuits and superconductive interconnections
positioned in between these interface circuits. There are a
total 1,130 gates. The prototype chip is designed to be
operated up to a clock frequency of 10 GHz. Therefore, the
total system throughput is estimated to be 60
Gbps. |
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Superconducting
neural circuits using SQUIDs Y.
Mizugaki, K. Nakajima, Y. Sawada and T.
Yamashita
Summary: Superconducting
implementation of neural circuits is presented. A neuron
element is composed of a coupled-SQUID, which is a combination
of a single-junction SQUID and a double-junction SQUID. A
synapse element is composed of multiple double-junction
SQUIDs. To demonstrate the abilities of these circuits
experimentally, a 8-bit neural-based A/D converter, which
contains three neurons and three synapses, has been fabricated
using a niobium integration technology. This is the first
successful implementation of both neuron and active synapse
elements into a superconducting neural network. |
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A
Josephson-junction-bridge track-and-hold
circuit K.Y. Tam and J.P.
Sage
Summary: This paper describes the design
and test of a high-speed monolithic track-and-hold circuit
(T/H) consisting of a Josephson-junction-bridge current switch
and a superconducting storage inductor. The bridge, under the
control of a common-mode clock current, switches a balanced,
differential input current. The T/H was fabricated using a
5-/spl mu/m, 1000 A/cm/sup 2/ niobium trilayer process.
Calculations and simulations of the T/H predict 5-bit dynamic
range, 4.6-bit effective dc resolution, 750 MHz analog
bandwidth, 725 ps acquisition time, 700 MS/s peak sampling
rate, and an unlimited hold time. Measurements on the
fabricated T/H verify the proper qualitative behavior of the
T/H and show that it has 5-bit dynamic range, 4.5-bit
effective dc resolution, 900 MHz analog bandwidth, and a 550
ps acquisition time, commensurate with a 900 MS/s sampling
rate. |
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Operation
of SAIL HTS digital circuits near 1
GHz S.M. Schwarzbek, K.E.
Yokoyama, D.J. Durand and R.A. Davidheiser
Summary:
Using Series Array Interferometer Logic (SAIL)
components, we have demonstrated an HTS gate driving an
exclusive OR, whose second input is being driven at 1 GHz.
This digital technique serves as an output interface: data is
placed on an rf carrier as phase information (Phase Shift
Keying). Low voltage, baseband, differential data can be
amplified by low noise, narrow bandwidth, single-ended
amplifiers. A simple demodulator completes the connection to
standard semiconductor electronics. |
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Optimization
of NbN MVTL logic gates for 10 K
operation M. Leung, D.J. Durand,
L.A. Abelson, L.R. Eaton and J.W. Spargo
Summary:
We have systematically studies designs for Modified
Variable Threshold Logic Gates (MVTL) in NbN within the
framework of factorial analysis. Our goal is to attain
optimized margin and fanout for 10 K operation. Significant
parasitic inductances, associated with current crowding at
junction vias, were measured and are found to affect the
operating margin. We report the progression of designs, margin
measurements and yield data for our 10 K
circuits. |
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Application
of superconducting electrodes to resonant-type LiNbO/sub 3/
optical modulator K. Yoshida, A.
Nomura, K. Komura and Y. Kanda
Summary: A
study has been made of a resonant type LiNbO/sub 3/ optical
modulator employing superconducting electrodes. Numerical
calculations of the modulation depth of the optical modulator
show that the driving power of the optical modulator using
superconducting electrodes can be much smaller than that using
normal metals. Experiments to demonstrate the operations of
the optical modulator with Pb-In electrodes resonant at 14.8
GHz have been successfully made at 4.2 K. An excellent
agreement between theory and experiments is obtained. It is
shown that the modulation power in the superconducting state
was estimated to be as small as 140 mW compared with 400 mW in
the normal state. The present results demonstrate the possible
application of superconducting electrodes to high performance
LMbO/sub 3/ optical modulators. |
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Microwave
losses of interferometers with many Josephson junctions versus
DC magnetic field R. Lochschmied,
W. Benzing and W. Jutzi
Summary: The average
microwave losses of interferometers with two and four strongly
damped Josephson junctions biased by a microwave current
source at 10 GHz much below the plasma frequency have been
simulated as a function of an external magnetic field.
Microwave losses appear periodically within distinct ranges of
the magnetic field, with microwave amplitudes below and above
threshold currents. The main period corresponds to one flux
quantum in every interferometer loop. The absorption rate
increases with the microwave amplitude in qualitative
agreement with measurements. |
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HTS/ferroelectric
thin films for tunable microwave
components F.A. Miranda, C.H.
Mueller, C.D. Cubbage, K.B. Bhasin, R.K. Singh and S.D.
Harkness
Summary: We report on the electrical
characterization of Ba/sub 0.5/Sr/sub 0.5/TiO/sub 3//YBa/sub
2/Cu/sub 3/O/sub 7-/spl delta///LaAlO/sub 3/ multilayer
structure. This structure was fabricated using a pulsed laser
deposition technique yielding film thicknesses of 300 nm and
800 nm for the YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// (YBCO)
and the Ba/sub 0.5/Sr/sub 0.5/TiO/sub 3/ (BST) films,
respectively, A transition temperature T/sub c/=91.5 K was
measured for the YBCO film in this structure after deposition
of the BST layer. The structure was patterned into parallel
plate capacitors with 400/spl times/400 /spl mu/m gold
contacts and YBCO electrodes on top and underneath the BST,
respectively. A relative dielectric constant (/spl epsiv//sub
r/)/spl sim/425 and a loss tangent (tan/spl delta/)=0.010 were
measured at 1.0 MHz at 298 K and zero dc voltage (V/sub dc/=0
volts). At 77 K, the dielectric data showed 320/spl les//spl
epsiv//sub r//spl les/360 and tan/spl delta/=0.036 at V/sub
dc/=0 volts. For 5.0/spl ges/V/sub dc//spl ges/-3.0 volts /spl
epsiv//sub r/ could be varied from 180 to 370. For -5.0/spl
les/V/sub dc//spl les/-3.0 volts, /spl epsiv//sub r/ decreased
rapidly with little change in tan/spl delta/. The /spl
epsiv//sub r/ versus V/sub dc/ data suggest that changes in
/spl epsiv//sub r/ were affected by electrode space charge
layers. |
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RF
coupling to single crystal BSCCO under c-axis
bias G.K.G. Hohenwarter, A.W.
Laundrie, J.U. Lee, J.B. Beyer and J.E.
Nordman
Summary: We have explored rf coupling
to BSCCO single crystals with c-axis bias currents over a wide
range of frequencies. A structure was developed that afforded
the necessary impedance transformations at several frequencies
from dc to 35 GHz. At low frequencies, connections were made
to a coaxial cable. At X-band, the sample was placed in front
of a short section of waveguide, forming a resonator. Above 12
GHz, the sample mount formed a coplanar resonator. At 35 GHz
it was used as the end plate of a cylindrical cavity with
degenerate mode spoilers and a loaded Q-factor of 3800 at 38.3
GHz. Fabricated BSCCO samples showed evidence of hysteretic
Josephson junction stack behavior at 77 K. Application of low
frequency rf signals caused steps to appear in the sample I-V.
At frequencies above 6.4 GHz only a reduction of critical
current was observed. |
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A
high gain YBCO antenna array with integrated feed and
balun L.P. Ivrissimtzis, M.J.
Lancaster and N.McN. Alford
Summary: A
supergain antenna array of closely spaced printed dipoles made
of thick film YBCO was designed and experimentally tested. An
optimization of the directive gain with respect to
interelement spacing, dipole length, and other circuit
parameters, subject to constraints in array size, was
performed by combining the spectral domain method of moments
and transmission line theory. The design procedure accounts
far losses associated with the strip material, both at the
feed and the radiating dipoles, and power dissipation in the
substrate. A practical design of a sixteen element array is
demonstrated, with an integrated feeding network and a balun,
also made of high-T/sub c/ superconductors (HTS). Performance
is compared against simulated data. The superconducting array
has gain significantly higher than that of a similar
supercooled silver array albeit at the expense of transmission
bandwidth. It is shown that supergain is practically
achievable by miniature, printed HTS dipole
arrays. |
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The
ARPA high temperature superconductivity
program F.W. Patten and S.A.
Wolf
Summary: This paper presents an overview
of the Advanced Research Projects Agency (ARPA) program on
high temperature superconductivity (HTS). This
multidisciplinary effort has, since 1987, spent about
$220,000,000 on promoting the science and technology of these
materials. Support of many aspects of R and D has been
provided to universities, national laboratories and an
emerging industrial base. The current program is focused on
several promising applications: (1) the development of RF and
microwave passive components and subsystems for radar, EW,
wireless communications and medical instrumentation; (2)
developing digital applications of cryogenic technology both
utilizing superconductors as well as semiconductors; (3)
contributing to the development of a conductor for power
applications, and (4) developing a variety of low-cost
reliable cryocoolers that will be the enabler for many
aforementioned applications. |
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Cryogenic
electronics in advanced sensor
systems M.M.
Fitelson
Summary: Cryogenic Electronics
technologies are discussed from the standpoint of meeting
sensor performance requirements. Capabilities that are
provided by cryogenic electronics are described. Radar and
Electronic Warfare (EW) Systems requirements are based on the
need to detect and track targets in the presence of clutter
and jamming signals. Radars must transmit high fidelity
signals, and receive returns with high fidelity and wide
dynamic range for Doppler Processing, to discriminate targets
from clutter and jamming. Requirements are translated into
radar specifications: transmitter, receiver, antenna array,
and other components must produce low phase noise. The
receiver and analog to digital converter (ADC) need wide
linear dynamic range. HTS technology provides key devices to
achieve phase noise supression and large signal dynamic range.
Examples include: HTS resonators generate stable reference
signals in the radar; switchable preselectors remove out of
band jamming; HTS circuits enable digital to analog converters
(DACs) and ADCs to provide direct synthesis of complex
waveforms and digitization of received signals. EW System
requirements are high dynamic range reception, and real-time
signal processing; they must be wide-band and recognize a
diverse set of waveforms. An HTS switchable preselector and
delay line provide the front end for an advanced EW receiver
and processor. The application of HTS technology to Radar and
EW Systems will be addressed, and progress to date in
development of analog and digital HTS devices will be
described. |
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Improved
design of an optically switched inductance modulation circuit
for noise reduction in SQUID
systems G.S. Park, Sae Woo Nam,
B. Cabrera and M.E. Huber
Summary: We have
modeled and optimized the design of an optically driven
inductance modulation circuit, for use as part of a 1/f noise
reduction scheme for SQUID magnetometers. We modulate the
effective inductance of a photolithographically patterned coil
via its mutual inductance with three concentric
superconducting washers directly above the coil. The
superconducting loops formed by each of these washers can be
broken by sending laser light onto a constricted meander
section of each of these washers. With the laser off, the
superconducting washer loops diamagnetically shield the coil,
and the coil has a low effective inductance. With the laser
on, the meanders are driven normal and the superconducting
washer loops are open, greatly reducing the shielding. The
coil then has a high effective inductance. In a series of
computational runs, we have optimized the design of this
circuit in terms of its inductance modulation depth and its
avoidance of flux jumping incidents. The free parameters in
this study were the inner diameter of the coil, the number of
loops in the coil, the dimensions of the three washers, and
the size of the overlaps between washers. |
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Use
of a DC SQUID receiver preamplifier in a low field MRI
system H.C. Seton, D.M. Bussell,
J.M.S. Hutchison and D.J. Lurie
Summary: We
have used tuned receiver coils coupled to a dc SQUID
preamplifier in a small scale magnetic resonance imaging (MRI)
system operating at 425 kHz (B/sub 0/=0.01 T). The coil and
SQUID are cooled to 4.2 K in a modified biomagnetic cryostat.
The modifications provide transparency to rf signals
originating outside the cryostat while maintaining an
acceptably low liquid helium boiloff rate. By applying
negative feedback we have damped low loss, high Q-factor SQUID
input circuits to achieve a useful imaging bandwidth of over 2
kHz. |
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High
slew rate large bandwidth integrated dc SQUID magnetometer for
NMR applications S.L. Thomasson
and C.M. Gould
Summary: We have developed an
integrated dc SQUID magnetometer, with additional positive
feedback (APF) unmodulated SQUID electronics system for low
frequency true NMR applications. We constructed our SQUID
circuit using an 11-layer Nb/Al/AlO/sub x//Nb process. Our
design modifies previous APF approaches by incorporating
selectable, high resolution on-chip feedback resistance. The
on-chip resistance selection allows us to maximize the SQUID
gain, dV/d/spl Phi/, at the operating point. With the use of
APF we have achieved a slew rate greater than 10/sup 6/ /spl
Phi//sub 0//s, and a bandwidth of approximately 300 kHz, which
is suitable for sensitive NMR measurements. |
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Integrated
rf amplifier based on dc
SQUID M.A. Tarasov, G.V.
Prokopenko, V.P. Koshelets, I.L. Lapitskaya and L.V.
Filippenko
Summary: Integrated
radio-frequency amplifiers comprising a 4-loop dc SQUID,
seriesly connected input coil turns, a resonant capacitor
parallel to the input coil, series capacitors at the input and
output ports and bias resistors have been designed, fabricated
and experimentally studied. A multiloop dc SQUID with parallel
loops and seriesly connected single-turn input coils placed
inside each loop and integration with the input resonant
matching circuit elements and with elements of dc bias circuit
allows one to increase signal frequency and reduce the
influence of external noise. The amplifiers with three
different capacitors have resonant frequencies 560, 656, 758
MHz and bandwidth about 50 MHz. The noise temperature of such
amplifiers below 1.5 K has been measured using cold attenuator
and room-temperature noise sources. The layout comprising
three pairs of such amplifiers placed on the same 15/spl
times/24 mm substrate was designed to increase the bandwidth
over the bandwidth of the individual amplifiers. |
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White
noise performance of integrated DC SQUID susceptometers in
high magnetic fields K.G.
Stawiasz, M.B. Ketchen and L.R. Narasimhan
Summary:
We have characterized the white noise performance of
integrated DC SQUID susceptometers in magnetic fields up to
400 G. The field is applied in the plane of the tunnel
junctions and pickup loops. For 1 /spl mu/m diameter
junctions, the noise does not increase significantly as the
field is increased to 125 G. Further increase of the applied
field results in higher noise until approximately 200 G where
the critical current of the junctions is at a minimum. The
noise then improves to approximately 4 times the zero field
value at the maximum of the first lobe of the single junction
interference pattern. We have also measured the noise of a
SQUID with 0.6 /spl mu/m junctions and found no increase up to
250 G. |
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Using
a scanning SQUID to determine the symmetry of the order
parameter in YBCO A. Mathai, Y.
Gim, R.C. Black, A. Amar and F.C. Wellstood
Summary:
We have determined the time and spatial symmetry of the
superconducting order parameter in YBa/sub 2/Cu/sub 3/O/sub 7/
(YBCO) by using a Scanning SQUID Microscope to perform a
time-reversal invariance test. We find the order parameter in
YBCO has a time-reversal invariant d(x/sup 2/-y/sup 2/)
symmetric component. In addition, we find that the amplitude
of any imaginary isotropic s-wave symmetric component must be
less than 6% and any real isotropic s-wave component less than
89%. |
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Multi-loop
self-shielded dc-SQUID with meander-shaped input
coil V.V. Masalov, A.N. Samoos,
A.N. Matlashov, V.Y. Slobodchikov and Y.V.
Maslennikov
Summary: A multi-loop design
insensitive to external uniform magnetic fields is suggested
for a dc SQUID. The SQUID has a meander-shaped coupling coil,
which show promise both for LTc and HTc biomagnetic measuring
systems. The 16- and 32-loop versions of the SQUID were
manufactured using niobium technology and were tested
experimentally. On the basis of the experimental data it was
shown that the use of LTc multi-loop SQUIDs makes it possible
to develop biomagnetic measuring gradiometers with a
resolution of the order of 3-4 fT/spl radic/Hz. A multiloop
SQUID may be used with a flux transformer in the form of a
first-order gradiometer free from conductor crossings. Such a
gradiometer has a single-layer design and can be easily
fabricated from HTc materials. |
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A
double dc SQUID based
magnetometer Yu.V. Maslennikov,
A.V. Baljaev, O.V. Snigirev, O.V. Kaplunenko and R.
Mezzena
Summary: We have developed a double
dc SQUID based magnetometer with a direct read-out circuit and
measured its signal and noise characteristics. The inductances
of the input SQUID and SQUID-preamplifier were 120 and 250 pH.
Thin-film flux transformers on the separate substrates had an
inductance of the order of 1 /spl mu/H each and a current
sensitivity of 0.54 and 0.32 /spl mu/A//spl Phi//sub 0/ for
the first and the second SQUIDs, respectively. The intrinsic
energy resolution of the fabricated magnetometer for an
optimal gain of 58 for the first stage was close to 1.6/spl
times/10/sup -32/ J/Hz. The dynamic range and the slew rate
were about 126 dB and 4/spl times/10/sup 4/ /spl Phi//sub
0//s. |
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Thin-film
resistive SQUIDS G.S. Krivoy and
H. Koch
Summary: Different all thin-film
partly resistive superconducting quantum interference devices
(RSQUIDs) for noise thermometry in the liquid helium
temperature range were designed and investigated. Three
different types of RSQUID were realised: (i) dc RSQUID, (ii)
rf RSQUID, and (iii) RSQUID with two quantization loops
(double RSQUID). Shunted tunnel junctions were used as weak
links. The resistive parts have been made as a Cu thin film
combined with Nb thin films either as a sandwich or a planar
element. The devices using a rf pump have integrated rf
coupling coils. Resistances of the resistive parts in the
range from 2.69 /spl mu//spl Omega/ to 246 /spl mu//spl Omega/
were obtained. The output signal was /spl ap/50 /spl mu/V for
the dc RSQUIDs, up to 80 /spl mu/V for the rf RSQUIDs, and up
to 1.2 mV for the double RSQUIDs. The linear dependences of
the output signal frequency versus a dc current passed through
the resistive part were observed up to 40 MHz. The double
RSQUIDS described have a clear advantage in the output signal
compared to the other RSQUIDs. |
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Dc
SQUID based on unshunted Josephson junctions: experimental
results H. Seppa, M. Kiviranta
and L. Gronberg
Summary: It has been proposed
that a new SQUID type be constructed by using unshunted
Josephson junctions instead of resistively shunted junctions.
Using this approach we are able to present a SQUID having a
high output dynamic resistance and a device characterized by a
negative output resistance and an extremely low noise. The
first mentioned is called a high-gain SQUID, the latter an
unshunted SQUID. This article describes preliminary
experiments obtained from the SQUIDs based on this concept.
The iv characteristics are shown to resemble the theoretically
predicted characteristics but the noise performance was higher
than expected. Most likely the reason for the high noise was
the imperfect damping of the SQUID in the frequencies near 1
GHz. |
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Effects
of high energy proton bombardment (50-280 MeV) on dc
SQUIDS B. Muhlfelder, G.M. Gutt,
J.M. Lockhart, P. Carelli, A. Zehnder, F. Mattenberger, W.
Hajdas, P. Lerch and R. Henneck
Summary:
Three thin film dc SQUIDs of varied construction were
bombarded with energetic protons in the energy range of 50 to
280 MeV. Measurements of the voltage output of the dc SQUIDs
were taken in open loop, as well as flux locked mode, in an
environment of proton flux that was varied from 10/sup 4/ to
10/sup 7/ protons/cm/sup 2//s. Discrete voltage jumps
corresponding to 0.01 to 0.001 flux quanta were observed in
two of the three SQUIDs in the flux locked mode; discrete
changes in the open loop SQUID output voltage were also
observed. Some data appear to be consistent with
proton-induced flux motion in the body of the SQUID
loop. |
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Measurement
and simulation of the voltage-flux transfer function of SQUID
arrays Kin Li and S.P.
Hubbell
Summary: We measured the V-/spl Phi/
of 100-element SQUID arrays and compared them to simulations.
Two SQUID inductances, 13 pH and 5 pH were studied. The change
of voltage modulation depth per /spl Phi//sub 0/ in a 5 pH
SQUID array was faster than that in a 13 pH SQUID array due to
larger effective area variations. The effect of magnetic field
uniformity on the SQUID arrays output was also studied. We
found that a non-uniform magnetic field had the effect of
reducing the output voltage and periodicity in V-/spl Phi/ for
a SQUID array with high flux bias. |
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A
novel method of realizing two-dimensional array systems of
high-T/sub c/ step-edge Josephson
junctions C.D.
Reintsema
Summary: We have developed a unique
substrate terracing process to achieve two-dimensional arrays
of high-T/sub c/ step-edge superconductor-normal
metal-superconductor Josephson junctions. This process has
been used to realize 3/spl times/3 and 3/spl times/6 antenna
coupled arrays for direct detection of emission. An
enhancement to this process incorporating a YBa/sub 2/Cu/sub
3/O/sub 7-/spl delta// base layer and a Nb/PdAu ground plane
is described. This modification enabled the fabrication of
arrays capacitively coupled to detector junctions for
detection of emission at frequencies beyond 300 GHz. This
report details the motivation, design, fabrication process,
and preliminary results of several array
experiments. |
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Properties
of YBaCuO step-edge Josephson junction series
arrays J. Konopka, I. Wolff, S.
Beuven, M. Siegel and A.I. Braginski
Summary:
YBa/sub 2/Cu/sub 3/O/sub 7/ (YBCO) structures composed
of 10 and 100 step-edge Josephson junction series arrays
incorporated into two-arm logarithmic spiral or bow-tie type
were designed, fabricated by pulsed-laser deposition on
structured LaAlO/sub 3/ substrates and measured in the
temperature range 12 to 70 K at frequencies up to 150 GHz. At
18 K the I/sub c/R/sub N/ product of 10 junction arrays was up
to 0.8 mV. Wide Shapiro steps at voltages corresponding to the
multiple frequency of irradiation of 100 and 150 GHz were
measured, as well as the emitted power and the linewidth at 12
GHz. In some arrays, 30 to 40% of the junctions were phase
locked. This indicated that the spread of critical parameters
of that fraction of the total junction population did not
exceed 10%. |
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Microwave
response of intrinsic Josephson junctions in BSCCO single
crystals A. Irie and G.
Oya
Summary: We have studied the microwave
response of an array of intrinsic Josephson junctions in the
c-axis direction in large Bi/sub 2/Sr/sub 2/CaCu/sub 2/O/sub
7/ (BSCCO) single crystals indicating multiple resistive
branches on the I-V characteristics. Under the 8-10 GHz
microwave irradiation, they showed three types of responses
depending on its power P. For relatively low P, the Shapiro
steps were observed, whose voltage separations were two order
magnitude larger than that calculated from /spl Delta/V=hf/2e,
indicating that about one hundred intrinsic junctions in the
crystal are phase-locked. For high P, two types of RF-induced
steps were observed. In the case of resonance mode, the I-V
curve showed the pronounced constant voltage step together
with subharmonic ones. On the other hand, for off-resonance
mode the broad step was observed. The voltages of these steps
increased lineally with p/sup 1/2/. These results suggest that
the fluxon motions in intrinsic Josephson junctions interact
with external RF field. |
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Intrinsic
Josephson junctions in high-T/sub c/ superconductors as high
frequency sources K. Schlenga, G.
Hechtfischer, W. Walkenhorst, P. Muller, F.X. Regi, H. Savary,
J. Schneck, M. Veith, W. Brodkorb and E.
Steinbeiss
Summary: We report on microwave
emission experiments of Bi/sub 2/Sr/sub 2/CaCu/sub 2/O/sub
8+y/-single crystals at frequencies between 12 GHz and 95 GHz.
Due to the intrinsic Josephson effect these samples form
series connections of typically 2000 contacts. For the first
time we observed phase-locking of more than 1000 junctions at
93.7 GHz in Bi/sub 1.8/Pb/sub 0.2/Sr/sub 2/CaCu/sub 2/O/sub
8+y/ single crystals. Concerning the development of high
frequency sources we report on first experiments on vertically
structured thin films of Tl/sub 2/Ba/sub 2/Ca/sub 2/Cu/sub
3/O/sub 10/. |
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Integrated
High-T/sub c/ oscillator array and high resistance detector
junction J. Edstam, G. Brorsson,
E.A. Stepantsov and H.K. Olsson
Summary: We
have integrated an array of five High-T/sub c/ Josephson
junction oscillators with a Josephson detector junction of
high resistance, e.g. 25 /spl Omega/. High impedance detectors
are suitable in integrated superconducting receivers. We find
the output power to be sufficient to modulate the detector
junction with large Shapiro steps in the frequency range
200-700 GHz. The oscillator junctions were dc-biased in
parallel and integrated in an inductive high frequency
coupling circuit to oscillate coherently in-phase. The high
frequency coupling circuit is evaluated through its influence
on the current-voltage characteristic of the Josephson
junctions. |
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Broadband
detection properties of EuBa/sub 2/Cu/sub 3/O/sub 7-/spl
delta// array junctions K. Tsuru,
M. Suzuki and O. Michikami
Summary: We have
fabricated EuBa/sub 2/Cu/sub 3/O/sub 7-/spl delta// Josephson
junction arrays of two different sizes to improve detection
output and microwave coupling between junctions and an rf
source. The arrays contain three weak link grain boundary
junctions made on an MgO bicrystal substrate. It is
demonstrated that both the junction array configuration and
smaller junction size are effective in improving microwave
coupling and hence in increasing the responsivity. The best
responsivity obtained is 1085 V/W for broadband detection at
11.9 GHz. |
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Stacked
series arrays of high-T/sub c/ trilayer Josephson
junctions J.N. Eckstein, I.
Bozovic, G.F. Virshup, R.H. Ono and S.P.
Benz
Summary: We report on the properties of
stacked series arrays of trilayer Josephson junctions grown by
atomic layer-by-layer molecular beam epitaxy. Trilayer
Josephson junctions oriented so that the current travels in
the c-axis direction have been described previously. Series
arrays are made by placing more than one barrier layer in the
Ba/sub 2/Sr/sub 2/CaCu/sub 2/O/sub 8/-based, (2212), epitaxial
structure. Single molecular layers of 2212 doped with Dy to
reduce the local carrier concentration are used as barriers,
and are placed very close to each other, e.g., separated by
only a few molecular layers of the superconducting phase.
Phase locking of a.c. Josephson currents has been observed.
The critical current density of such junctions has been
observed to be very uniform on wafers that are free of second
phase defects, and operation up to 60 K has been
obtained. |
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Phase
locking of HTS Josephson junctions closed into a
superconducting loop S. Beuven,
M. Darula, J. Schubert, W. Zander, M. Siegel and P.
Seidel
Summary: We investigated the mutual
interaction of four high-T/sub c/ Josephson junctions which
were closed into a superconducting loop. Phase locking of all
four junctions was demonstrated in the temperature range from
4.2 K to 48 K. Locking intervals of 18% of the critical
current were obtained up to voltages corresponding to a
frequency of 180 GHz, according to the second Josephson
relation. By comparing our data with numerical simulations, we
could show that the junctions were locked in the in-phase
state and that the circuit can act as a source of coherent
radiation which can deliver power to a load. |
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Josephson
vortex-flow transistors based on parallel arrays of YBa/sub
2/Cu/sub 3/O/sub 7-/spl delta// bicrystal grain boundary
junctions R. Gerdemann, L. Alff,
A. Beck, O.M. Froehlich, B. Mayer and R.
Gross
Summary: Three-terminal electronic
devices based on flux-flow phenomena have attracted
considerable interest due to their potential application in
the interface between superconducting and semiconducting
electronics. We have fabricated Josephson vortex flow
transistors based on parallel arrays of YBa/sub 2/Cu/sub
3/O/sub 7-/spl delta// (YBCO) bicrystal Grain Boundary
Junctions (GBJs). The array critical current I/sub c/ has been
measured as a function of an external magnetic field B or the
magnetic field of the current I/sub ctrl/ that is fed through
the control line coupled inductively to the array. By varying
the device geometry we have studied the influence of the
coupling of the magnetic control and the array parameters such
as the number N of discrete Josephson elements and the
screening parameter /spl beta//sub L/ on the I/sub c/(B)
dependences of the arrays. Going from /spl beta//sub L//spl
Lt/1 to /spl beta//sub L//spl Gt/1 the measured I/sub c/(B)
curves changed from a dependence similar to the diffraction
pattern of a grid to a dependence dominated by the parameters
of a single array cell. The impact on the available current
gain is discussed. |
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Applications
of mm-wave SIS mixers to middle atmosphere monitoring
systems H. Suzuki, T. Imamura, N.
Yokoyama, M. Suzuki, H. Ogawa, K. Kawabata and Y.
Fukui
Summary: We have already developed a
low-noise 100 GHz band (98-115 GHz) SIS mixer using Nb/AlOx/Nb
junction technology. The mixer has a noise temperature of 17 K
when used as a double sideband (DSB) heterodyne receiver. The
SIS receiver has been in use in the 4 m radio telescope at
Nagoya University for five years. As a further application of
the SIS mixer, we developed middle-atmosphere ozone monitoring
system using an SIS mixer for the first time. The system can
measure ozone mixing ratio every 5 minutes. The integration
time is less than 1/10 of the time needed in a conventional
system using Schottky barrier diode (SBD) mixers. We have also
begun developing developing a 200 GHz band (210-280 GHz) SIS
mixer for radio astronomy and for monitoring other minor
constituents such as ClO. The preliminary experiment showed
that the mixer has a rather low noise temperature of 60 K
(DSB). |
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Mixer
of short weak link using a resonance effect due to multiple
Andreev reflections at subgap
voltages T. Matsui and H.
Ohta
Summary: Short metallic weak links of Nb
are used for millimeter-wave mixer experiments at 100-110 GHz.
When the weak links are connected to a voltage bias circuit
with zero output impedance, subharmonic gap structures are
observed as a large dynamic resistance region or a negative
differential resistance region at voltages V/sub u/=2/spl
Delta//ne on the I-V curve, where n=1, 2, 3, ... . These
strong structures are caused by a resonance effect between the
energy gap and the multiple Andreev reflections that are
present whenever there is a spatial inhomogeneity of the pair
potential. Enhancement of IF signal peaks is observed at the
subgap voltages. These experimental results suggest the
appearance of the density of states predicted theoretically by
R. Kummel et al. The subharmonic gap structure and details of
the SNS mixer experiment will be described. |
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Four
photons sensitivity heterodyne detection of submillimeter
radiation with superconducting tunnel
junctions A. Karpov, J. Blondel,
M. Voss and K.H. Gundlach
Summary: An ultra
low noise SIS receiver has been prepared for radio astronomy.
The minimum double sideband receiver noise temperature is
about 30 K which corresponds to 2 /spl planck//spl omega//k or
an equivalent number of 4 photons of noise. The minimum
measured double sideband mixer noise temperature is about 10 K
which corresponds to 0.6 /spl planck//spl omega//k or
approximately to 1 photon of noise. The fixed tuned SIS mixer
operates in the 290-370 GHz frequency range. The submicron
niobium junctions mere fabricated using photoresist lines for
junction definition. The receiver has been used at the 30 m
IRAM radio telescope in Spain in winter 1994. Telescope system
noise temperature of 500 K single sideband has been achieved
when the sky opacity was about 0.17. |
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Shot
noise and photon-induced correlations in 500 GHz SIS
detectors N.B. Dubash, M.J.
Wengler and J. Zmuidzinas
Summary:
Photon-induced current correlations in SIS detectors
can result in an output noise that is greater or less than
shot noise. Evidence of these correlations had been observed
for 100 GHz rf by accurate noise measurements as reported in
our previous work. We now present a detailed analysis of these
current correlations for frequencies between 100 and 500 GHz.
We also report new measurements of photon-induced noise in a
490 GHz SIS mixer, and discuss the Gaussian beam techniques
used to eliminate the thermal background radiation. For small
490 GHz rf power, the output noise is equal to shot noise. The
results of the 100 and 490 GHz photon noise measurement are
summarized in context to shot noise and the effect of the
current correlations predicted by the theoretical
model. |
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Measurement
of the noise contributions to SIS heterodyne
receivers D.P.
Woody
Summary: The development of quantum
limited heterodyne receivers requires that you understand and
are able to measure the major sources of noise in the receiver
system. The major sources of noise in millimeter- and
submillimeter-wave SIS heterodyne receivers are the optical
front end losses, vacuum fluctuation noise associated with the
RF coupling efficiency to the SIS tunnel junction and IF
amplifier noise. Although there are several methods for
estimating the optical losses and IF amplifier noise, the RF
coupling efficiency or quantum efficiency has been much more
difficult to ascertain. This paper describes in situ
techniques for measuring all three noise contributions in a
standard receiver used for astronomical observations. Results
are presented for the receivers operating in the Owens Valley
Millimeter Interferometer Array. |
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Superconducting
packet switch M. Hosoya, T.
Nishino, W. Hioe, S. Kominami and K. Takagi
Summary:
Very broad band throughputs greater than 1T bit/sec are
desired in heavily loaded communication systems. Using the
merits of superconducting devices, a superconducting network
system is expected to improve the throughputs of such
communication bottleneck systems. The paper describes a
superconducting packet switch which is indispensable to a
proposed superconducting network system. Considering the
characteristics of various switch architectures, the
space-division Banyan type architecture is adopted for a
superconducting packet switch proto-type. The complete design
of the proto-type is performed and the total operation is
numerically simulated and confirmed. A 2/spl times/2 switching
element which controls the paths of two packets is a key
component of the proto-type. The basic switching element with
one-bit data width is fabricated and the correct operation is
completely confirmed. |
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A
clock distribution scheme for large RSFQ
circuits K. Gaj, E.G. Friedman,
M.J. Feldman and A. Krasniewski
Summary: A
primary issue in maximizing the performance of large scale
synchronous digital systems is the clock distribution scheme.
We present novel clocking scheme, developed specifically for
RSFQ logic, which is based on the concurrent flow of the clock
and data signals. The scheme permits the circuit throughput to
be independent of inter-cell connection delays and
significantly reduces the dependence of the throughput on the
clock-to-output delay of the cells. Concurrent flow clocking
is particularly well for structured architectures. The
simulated maximum clock frequency of an RSFQ decimation
digital filter currently under development at the University
of Rochester can be as much as seven times higher using
concurrent-flow clocking rather than conventional
(counterflow) clocking. This advantage, however, is reduced to
a factor of two due to fabrication parameter variations in
present day superconductive technologies. |
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Design
of an RSFQ microprocessor P.
Bunyk and V.K. Semenov
Summary: We are
discussing a general-purpose microprocessor architecture that
is suitable for implementation using the Rapid
Single-Flux-Quantum (RSFQ) family of logic-memory circuits.
While the microprocessor provides a functionally complete RISC
instruction set with 16-bit words, a bit-serial self-timed
approach makes it simple enough to be fabricated using the
current Josephson junction technology. Our plans are to
design, fabricate and test a completely operational prototype
of this system. |
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A
novel Josephson cellular array M.
Morisue and Fu-Qiang Li
Summary: This paper
describes a novel Josephson combinational logic cellular array
which can perform any function of n-variable. The basic logic
functions such as AND, OR, NOT and Exclusive-OR can be easily
achieved by the proposed cellular array. In this paper the
principle to construct the cellular array by using SQUID gate
is described in detail. In order to verify the operation of
the cellular array, simulations have been made for basic logic
circuits and a full adder with a satisfactory reliability and
high speed operation. |
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One-dimensional
parallel Josephson-junction arrays as a tool for circuit
diagnostics H.S.J. van der Zant,
T.P. Orlando and A.W. Kleinsasser
Summary: We
propose and demonstrate the use of underdamped,
one-dimensional parallel arrays of Josephson junctions as a
tool for circuit diagnostics. By measuring the Fiske modes and
the critical current in a magnetic field, we determined the
self and nearest neighbor inductances as well as the
capacitances of single junctions. We have used this technique
to find the capacitance of Nb-Al/sub 2/O/sub x/-Nb junctions
for critical current densities of 0.3-20 kA/cm/sup 2/. We find
that the specific capacitance increases by about a factor of 2
over this range. This increase has important consequences for
the design of single-flux-quantum circuits and SQUIDs.
Measurement of the junction capacitance for critical current
densities of 100 kA/cm/sup 2/ is possible, but requires
submicron junctions with dimensions of the order of 0.3 /spl
mu/m. |
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Multiparameter
optimization of RSFQ circuits using the method of inscribed
hyperspheres Q.P. Kerr and M.J.
Feldman
Summary: Rapid Single Flux Quantum
(RSFQ) circuits must be designed with large operating margins
because of variations in the fabrication process. We describe
a routine to optimize the yield, rather than the critical
margin, of RSFQ circuits, based on the method of inscribed
hyperspheres. The operating region is mapped out with a
minimum of circuit simulations taking into account the
relative size of the process variations. The method is
effective for as many as nine parameters. We show that the
standard optimization of critical margin will often give a
seriously wrong result for multidimensional parameter
space. |
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A
computer-aided design framework for superconductor
circuits M. Khalaf, S. Whiteley
and T. Van Duzer
Summary: This report
describes a Computer-Aided Design (CAD) framework for
superconducting digital circuits that will automatically
transform a high-level combinational circuit description to a
gate-level netlist. The framework involves enhancing the
current semiconductor logic synthesis CAD tools developed at
UC Berkeley (SIS) for application to superconductor digital
circuits. The issues specific to superconducting circuits at
the synthesis level include the use of multi-phase ac clocking
for combinational logic, latching behavior with resetting time
constraints, and dual-rail noninverting logic. |
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Design
tools for parameter determination and simulation of integrated
Josephson structures H. Topfer,
H. Uhlmann, M. Knoll, H. Thiele and M.
Selent
Summary: The recent development of
integrated Josephson circuits with increased complexity-e.g.
RSFQ devices-invokes the need of a comprehensive
computer-aided design support. The derivation of circuit
parameters from layout data as well as an efficient and
versatile simulation technique are essential means in the
design and dimensioning of complex integrated structures. We
present a comprehensive solution for calculating circuit
parameters and simulating the device dynamics. The calculation
of inductances and capacitances is performed by
three-dimensional field computation using special developed
programs which have been proven in high-T/sub c/ SQUID design.
They can process layout information in standard graphic
interchange formats (e.g. DXF). The netlists for device
simulation can be generated automatically from the equivalent
circuit schematic. Additionally, a technique for distributed
simulation, which allows performing
margins-and-yields-analyses in an efficient manner, was
elaborated. The performance of the whole design tool set is
demonstrated using basic RSFQ circuits. |
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Series
Josephson junction arrays as a high output voltage
amplifier E. Terzioglu and M.R.
Beasley
Summary: We are investigating the
potential of series arrays of nonhysteretic Josephson
Junctions as high output voltage amplifiers. Such amplifiers
may be useful in Josephson Junction-to-CMOS drivers in
Superconductor/Semiconductor hybrid systems. The I-V curves of
these arrays are sensitive to the nature and degree of
coupling between the junctions in the array. The coupling is
determined by the type and the value of the load as well as
the junction capacitance (i.e. /spl beta//sub c/) Depending on
the nature of the load, the junctions may lock in phase
("in-phase state") or couple such that the fundamental of the
Josephson oscillations cancel ("anti-phase state"),
suppressing the high frequency Josephson oscillations in the
load. Using numerical simulations, we studied the stability of
such states to various loads of interest and under static and
dynamic drive conditions. |
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Circuit
design for a high-T/sub c/ Josephson
sampler M. Hidaka and J.S.
Tsai
Summary: We propose a high-speed and
high-sensitivity sampler circuit using high T/sub c/
superconducting (HTS) Josephson junctions. This circuit
consists of five non-latching junctions, superconducting lines
and a superconducting ground-plane. A main feature of this
circuit is a non-latching comparator junction whose switching
generates a circulating current in a superconducting loop.
Computer simulation and prototype layout were performed to
study its ability and feasibility. |
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Discrete
underdamped vortex flow
devices A.E. Duwel, H.S.J. van
der Zant and T.P. Orlando
Summary: Vortex
flow devices consisting of discrete arrays of underdamped
Josephson junctions have been fabricated and measured. These
devices and their long, continuous junction counterparts are
based on the ability to magnetically control the Eck voltage
in an underdamped system. We find that both transistor and
oscillator parameters are improved by placing the arrays above
a superconducting ground plane and by connecting two arrays in
series. We developed models for the device behavior which
numerically account for the measured parameters. Our models
also suggest that junctions with smaller capacitances will
further improve the device parameters. |
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Generation
of single vortices and local detection by integrated dc
SQUIDs F. Peter, M. Grimm, M.
Muck and C. Heiden
Summary: A test circuit
for the local generation and detection of single vortices has
been fabricated, based on a multilayer structure with
low-pinning e-beam evaporated Nb and high-pinning reactively
sputtered NbN films. The generation of vortices is performed
by a current through a control line perpendicular to a
low-pinning channel. For the detection and determination of
the position of generated vortices, several dc SQUIDs were
located around the low-pinning channel and the control line.
The presence of single vortices in the channel lead to a shift
in the dc SQUID flux-to-voltage transfer function. By computer
simulations of the flux that a single vortex generates at the
position of the SQUIDs, the number and location of generated
vortices could be determined. The spatial resolution of this
procedure was determined to be about /spl plusmn/1 /spl mu/m
normal to and /spl plusmn/2 /spl mu/m along the
channel. |
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Gain
limitations in narrow width Josephson junction vortex flow
transistors M.A. Ketkar, J.B.
Beyer and J.E. Nordman
Summary: The number of
devices required to achieve a practical gain from a Josephson
junction vortex flow transistor (JVFT) distributed amplifier
is inversely proportional to the gain or the transresistance,
r/sub m/ of each active device. A large number of devices
means longer transmission line lengths associated with
increased loss and size. Reducing the junction width results
in increased r/sub m/, however there is a fundamental limit
for achievable r/sub m/. This is basically due to two reasons,
increased fringing field effects and edge penetration at
smaller aspect ratios. Field analyses made on devices with
various dimensions show this limitation in the magnitude of
r/sub m/ for narrower junctions. The analysis also provides
valuable information on parasitic elements in the circuit
model for a JVFT. Results of the analyses on devices having
different geometries suitable for high frequency operation are
presented. |
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Mechanisms
for conduction via low-frequency noise measurements of
high-T/sub c/ thin-film
microbridges T. Nguyen, J.M.
O'Callaghan, B.A. Davidson, R.D. Redwing, G.K.G. Hohenwarter,
J.E. Nordman and J.B. Beyer
Summary: We have
investigated possible mechanisms for conduction in high-T/sub
c/ thin-film microbridges biased into the voltage state via
the low-frequency noise properties. Measurements on thinned
YBCO microbridges indicate that the voltage noise power
spectral density S/sub V/(f) is proportional to the DC voltage
. |
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Discrete
models of Abrikosov vortex flow
transistors A. Davidson and N.F.
Pedersen
Summary: Electronic devices based on
flux flow phenomena in oxide superconductors have been under
development, and are potentially important for applications,
particularly in the interface between RSFQ circuits and
silicon based room temperature electronics. Models for these
flux flow transistors (FFTs) usually have been based on
discrete Josephson elements, ignoring the physics of fluxoid
nucleation. We have explored a numerical simulation of flux
flow also using discrete Josephson elements, but at the level
of the Abrikosov vortex, so that nucleation at the film edge
becomes part of the model. Our results imply that the
inhomogeneous coupling of the magnetic control is important
for a saturated transfer function, rather than a periodic one,
and that there is no advantage in putting flux flow strips in
parallel, separated by open gaps. Furthermore, gain may be
increased by arranging the bias to separately optimize
nucleation and transfer to the load. |
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Computer
simulations of dynamics of vortex lines in superconducting
flux flow transistors H. Andoh,
M. Kusunoki, A. Fujimaki and H. Hayakawa
Summary:
We study the dynamics of vortex lines in
superconducting flux flow transistors (SFFTs) made of High
T/sub c/ superconductors, YBa/sub 2/Cu/sub 3/O/sub x/. By
computer simulations we have found that the density of vortex
lines in SFFTs has close relation to device I-V
characteristics rather than the velocity of vortex lines and
that we have to increase the density of vortex lines to get
ones with available gain. To be more concrete, in order to
increase the density of vortex lines we have to lower surface
barriers at the edge of weak-links and heighten the magnetic
field near the edge of weak links. Especially, it is very
important to heighten the magnetic field at the both sides of
a link in a SFFT. Under the control of the control current,
vortex lines in a SFFT are driven by the transport current
(the bias current) mainly, but it is important to think of the
other forces such as the force by screening current, the force
induced by the other vortices and the force induced by the
image vortices. Based on the local stochastic equation of
motion for vortex lines, computer simulations for some
conditions are performed to discuss the dynamic behavior of
vortex lines in a SFFT. We report the effect of the external
magnetic field induced by the control current on the motion of
vortex lines in SFFTs. |
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Characteristics
of high-T/sub c/ superconducting flux flow transistors with
submicron channels K. Miyahara,
K. Tsuru, S. Kubo and M. Suzuki
Summary:
High-T/sub c/ superconducting flux flow transistors
were fabricated by focused ion-beam irradiation with thin
films of co-evaporated YBaCuO. The line-shaped vortex flow
channels (0.8 /spl mu/m in width) were constructed by scanning
a focused Ga ion-beam (500 nm in diameter) to reduce the
critical super-current of the film. The three terminal
characteristics of the device were successfully measured. The
flux flow characteristics and the transresistance of the
submicron channel were measured and compared with those of an
ordinary device with a channel wider than 2 /spl mu/m. The
measured flow voltage, transresistance and current gain are
discussed in relation to the parallel flow of the vortices in
the wide channel. |
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RF
characterization of Josephson flux-flow transistors: design,
modeling, and on-wafer
measurement Y.M. Zhang, E.
Carlsson, D. Winkler, G. Brorsson, H. Zirath and E.
Wikborg
Summary: Josephson flux-flow
transistors based on 0-32/spl deg/ [001]-tilt YBa/sub 2/Cu/sub
3/O/sub 7/ bicrystal junctions have been fabricated with Au
loops as the control current lines. In order to measure the
S-parameters of the transistors, no matching elements are
implemented and 50 Omega coplanar lines are used as the input
and output ends of the transistors. The rf properties of the
transistors have been modeled on an HP microwave CAD design
system, with the junction parameters taken from our dc
measurements. Simulations indicate that the transistors can
have a maximum stable gain of 20 dB at 7 GHz and 6 dB around
35 GHz under matched conditions. An 'on-wafer'
transmission-reflection-load (TRL) method is used for
calibrating the S-parameters of the transistor. A low
temperature microwave probe station has been built: a pair of
microwave probes inside a cryostat are moveable in the
xyz-directions. Together with a Wiltron 360B vector network
analyzer, this setup provides a convenient way for doing
on-wafer characterization of the transistors in the frequency
range from 40 MHz to 60 GHz, and in the temperature range from
20 to 80 K. |
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Superconducting
flux flow transistors with submicrometer
structures M. Kusunoki, H.
Akaike, A. Fujimaki and H. Hayakawa
Summary:
A miniaturization of high critical temperature (T/sub
c/) superconducting flux flow transistor (SFFT) was studied.
The weak link width in the direction of the vortex flow was
varied from 5 /spl mu/m to 10 /spl mu/m. The weak link length
in the direction of bias current flow was fixed to 5 /spl
mu/m. An increase in the gain was observed as the weak link
width decreased. A control line was placed close to the weak
link at a distance of 0.5 /spl mu/m to compensate for a
decrease of magnetic sensitivity due to the miniaturization.
We also improved the characteristics of the SFFT by forming a
corrugated structure, which is named corrugation flux flow
transistor (CFFT). A submicron patterning of YBa/sub 2/Cu/sub
3/O/sub y/ (YBCO) thin film was performed using focused ion
beam lithography. Furthermore, we demonstrated a micro flux
flow transistor (MFFT) consisting of a single bridge. The MFFT
also operated as well as the CFFT. |
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Superconducting
flux-flow transistors based upon YBa/sub 2/Cu/sub 3/O/sub 7/
nanobridges J. Schneider, A. v.d.
Hart and R. Wordenweber
Summary:
Superconducting flux-flow transistors were fabricated
from thin (50 nm) high temperature superconducting YBa/sub
2/Cu/sub 3/O/sub 7/ films. In order to determine whether the
suppression of the critical current by an applied control
current is caused by the magnetic induction or thermal heating
due to dissipation in the control line, two different device
geometries were developed. The first structure consists of a
parallel array of short nanobridges and one parallel control
line. In the second structure, a single 10 /spl mu/m long
nanobridge is arranged with two parallel long control lines
placed on both sides of the signal line. Our measurements
demonstrate that in both geometries the magnetic induction of
the control lines suppresses the transport properties of the
nanobridges. However, for control currents larger than the
critical current the transport properties of the bridge are
additionally strongly suppressed by thermal effects, which are
caused by heating of the current-biased control lines.
Furthermore, transistor structures with one long nanobridge
and two control lines react more sensitively to small control
currents than the device with a single and short control line.
They can operate at currents far below the critical current,
which leads testable transistor devices. |
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HTS
flux-flow channels on silicon
wafers D.B. Fenner, J.I. Budnick,
D.M. Potrepka, Q. Li, P.A. Rosenthal, J. Luo and W.D.
Hamblen
Summary: New process/structure
designs for the channel in the vortex flux-flow transistor
(VFFT) have been explored utilizing thin YBCO films on silicon
wafers. Two designs are reported: first, films on
micromachined Si(100) surfaces, and second, films ex-situ
annealed in bromine. Shallow trenches are anisotropically
etched into Si(100) wafers forming (111) facets, and films are
grown by pulsed laser deposition. Bromination processing of
YBCO is preceded by mild de-oxidation and followed by a
re-oxidation. Broad-area characterizations by R(T), dc
magnetometry, and ac susceptibility are given. On Si(100),
epitaxial YBCO films have sharp R(T) transitions and high
J/sub c/. Films on Si(111) and brominated films have a toe in
R(T) at T/sub co/, and lower J/sub c/ more easily reduced by
H. YBCO falling across the trenched surfaces or small
brominated regions have R(T), I-V, and I/sub c/ promising for
use as flux-flow channels in VFFT. |
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A
single flux quantum shift register operating at 65
K M.G. Forrester, J.X. Przybysz,
J. Talvacchio, J. Kang, A. Davidson and J.R.
Gavaler
Summary: We report the fabrication
and quasi-static testing of a two-stage, high-temperature
superconducting, Single Flux Quantum shift register. The
five-junction circuit was fabricated using a single YBCO film,
with step-edge grain boundary junctions. Storage of flux, and
its motion in response to LOAD and SHIFT signals, was
demonstrated at 65 K. |
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The
critical current and normal resistance of high-T/sub c/
step-edge SNS junctions C.D.
Reintsema, R.H. Ono, G. Barnes, L. Borcherdt, T.E. Harvey, G.
Kunkel, D.A. Rudman, L.R. Vale, N. Missert and P.A.
Rosenthal
Summary: We have fabricated
high-T/sub c/ superconductor-normal-superconductor Josephson
junctions with a variety of controlled geometries and measured
the resulting dependences of critical current and normal
resistance. These studies show that we can adjust our junction
parameters over orders of magnitude, thus allowing us to
tailor the junctions for a variety of
applications. |
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Electron
beam damaged high-T/sub c/ junctions-stability,
reproducibility and scaling
laws A.J. Pauza, D.F. Moore, A.M.
Campbell, A.N. Broerst and K. Char
Summary:
The problems of stability and reproducibility of the
electron beam irradiated high-T/sub c/ junctions have been
studied. It is found that with a overdamage-anneal protocol
that stable junctions can be obtained. While on chip
uniformity can be very good (1%), the chip to chip
reproducibility is not better than 20%. The annealing process
allows us to vary T/sub c/ of the junctions over a wide range,
making it possible to study the scaling behaviour of a single
junction. We find that in these junctions I/sub c/R/sub n//spl
prop/J/sub c//sup n/, with n=0.75-0.8 or, since the
quasiparticle and Cooper-pair cross sections appear to be
equivalent, I/sub c/R/sub n//spl prop//spl sigma//sub N//sup
p/ where p=3.0-3.7. |
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Electromagnetic
properties of YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//
thin-film grain-boundary weak
links B.H. Moeckly and R.A.
Buhrman
Summary: The I-V characteristics of
thin film microbridges containing 900 basal-plane-faced tilt
boundaries (TBs) exhibit pronounced resonant structure. This
structure is attributable to the presence of "beating modes"
previously studied in high Q DC SQUID structures having
substantial shunt capacitance and large inductance. Less
pronounced but clear resonant structure is also observable in
in-plane c-axis TBs. We discuss a model which accounts for
this behavior. |
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Author Index (1994 - Part
3) No author information
available
Summary: Not
available |
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