57 research outputs found
Ultra-Low-Power Superconductor Logic
We have developed a new superconducting digital technology, Reciprocal
Quantum Logic, that uses AC power carried on a transmission line, which also
serves as a clock. Using simple experiments we have demonstrated zero static
power dissipation, thermally limited dynamic power dissipation, high clock
stability, high operating margins and low BER. These features indicate that the
technology is scalable to far more complex circuits at a significant level of
integration. On the system level, Reciprocal Quantum Logic combines the high
speed and low-power signal levels of Single-Flux- Quantum signals with the
design methodology of CMOS, including low static power dissipation, low latency
combinational logic, and efficient device count.Comment: 7 pages, 5 figure
Whispering Vortices
Experiments indicating the excitation of whispering gallery type
electromagnetic modes by a vortex moving in an annular Josephson junction are
reported. At relativistic velocities the Josephson vortex interacts with the
modes of the superconducting stripline resonator giving rise to novel
resonances on the current-voltage characteristic of the junction. The
experimental data are in good agreement with analysis and numerical
calculations based on the two-dimensional sine--Gordon model.Comment: 5 pages, 5 figures, text shortened to fit 4 pages, correction of
typo
Ferromagnetic Josephson switching device with high characteristic voltage
We develop a fast Magnetic Josephson Junction (MJJ) - a superconducting
ferromagnetic device for a scalable high-density cryogenic memory compatible in
speed and fabrication with energy-efficient Single Flux Quantum (SFQ) circuits.
We present experimental results for
Superconductor-Insulator-Ferromagnet-Superconductor (SIFS) MJJs with high
characteristic voltage IcRn of >700 uV proving their applicability for
superconducting circuits. By applying magnetic field pulses, the device can be
switched between MJJ logic states. The MJJ IcRn product is only ~30% lower than
that of conventional junction co-produced in the same process, allowing for
integration of MJJ-based and SIS-based ultra-fast digital SFQ circuits
operating at tens of gigahertz.Comment: 10 pages, 4 figure
Observation of progressive motion of ac-driven solitons
We report the first experimental observation of phase-locked motion of a
topological soliton at a nonzero average velocity in a periodically modulated
lossy medium, under the action of an ac force with no dc component [the effect
was predicted by G. Filatrella, B.A. Malomed, and R.D. Parmentier, Phys. Lett.
A 198, 43 (1995)]. The velocity is related by a resonant condition to the
driving frequency. The observation is made in terms of the current-voltage,
I(V), characteristics for a fluxon trapped in an annular Josephson junction
placed into dc magnetic field. Large zero-crossing constant-voltage steps,
exactly corresponding to the resonantly locked soliton motion at different
orders of the resonance, are found on the experimental I(V) curves. A measured
dependence of the size of the steps vs. the external magnetic field is in good
agreement with predictions of an analytical model based on the balance equation
for the fluxon's energy. The effect has a potential application as a
low-frequency voltage standard. The work was supported by a grant from the
German-Israeli Foundation.Comment: Physical Review B, in press (Rapid Communication
RF assisted switching in magnetic Josephson junctions
We test the effect of an external RF field on the switching processes of magnetic Josephson junctions (MJJs) suitable for the realization of fast, scalable cryogenic memories compatible with Single Flux Quantum logic. We show that the combined application of microwaves and magnetic field pulses can improve the performances of the device, increasing the separation between the critical current levels corresponding to logical "0" and "1." The enhancement of the current level separation can be as high as 80% using an optimal set of parameters. We demonstrate that external RF fields can be used as an additional tool to manipulate the memory states, and we expect that this approach may lead to the development of new methods of selecting MJJs and manipulating their states in memory arrays for various applications
High Density Fabrication Process for Single Flux Quantum Circuits
We implemented, optimized and fully tested over multiple runs a
superconducting Josephson junction fabrication process tailored for the
integrated digital circuits that are used for control and readout of
superconducting qubits operating at millikelvin temperatures. This process was
optimized for highly energy efficient single flux quantum (ERSFQ) circuits with
the critical currents reduced by factor of ~10 as compared to those operated at
4.2 K. Specifically, it implemented Josephson junctions with 10 uA unit
critical current fabricated with a 10 uA/um2 critical current density. In order
to circumvent the substantial size increase of the SFQ circuit inductors, we
employed a NbN high kinetic inductance layer (HKIL) with a 8.5 pH/sq sheet
inductance. Similarly, to maintain the small size of junction resistive shunts,
we used a non-superconducting PdAu alloy with a 4.0 ohm/sq sheet resistance.
For integration with quantum circuits in a multi-chip module, 5 and 10 um
height bump processes were also optimized. To keep the fabrication process in
check, we developed and thoroughly tested a comprehensive Process Control
Monitor chip set.Comment: 10 pages, 5 figures, 1 tabl
Resonant flux motion and I-V -characteristics in frustrated Josephson junctions
We describe the dynamics of fluxons moving in a frustrated Josephson junction
with p, d, and f-wave symmetry and calculate the I-V characteristics. The
behavior of fluxons is quite distinct in the long and short length junction
limit. For long junctions the intrinsic flux is bound at the center and the
moving integer fluxon or antifluxon interacts with it only when it approaches
the junction's center. For small junctions the intrinsic flux can move as a
bunched type fluxon introducing additional steps in the I-V characteristics.
Possible realization in quantum computation is presented.Comment: 21 pages, 8 figure
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ ΠΎΡΠ²Π΅ΡΠ΅Π½ΠΈΡ Π½Π° ΠΏΡΠΎΡΠ°ΡΠΈΠ²Π°Π½ΠΈΠ΅ ΡΠ΅ΠΌΡΠ½ ΠΊΠ°ΠΏΡΡΡΡ ΠΊΠΈΡΠ°ΠΉΡΠΊΠΎΠΉ ΠΈ Π±ΡΠΎΠΊΠΊΠΎΠ»ΠΈ ΠΈ Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠ½ΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΌΠΈΠΊΡΠΎΠ·Π΅Π»Π΅Π½ΠΈ Π² Π·Π°ΠΊΡΡΡΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠ΅ ΡΠΈΠ½Π΅ΡΠ³ΠΎΡΡΠΎΠ½Π° ΠΠ‘Π 1.01
Relevance. Growing plants in artificial conditions (closed agroecosystems) requires precise regulation of plant growth factors, starting from the first stages of ontogenesis. One of the parameters is the presence or absence of light in the period of seed germination. For most types of cabbage the standard method is germination in the dark, but for freshly harvested seeds (at rest) light exposure is necessary. According to the literature, the mechanisms of the effect of light on seed germination are complex and ambiguous, so the issue needs detailed research.Methods. Therefore, the purpose of this work was to study the germination of seeds of broccoli (Brassica oleracea var. italica Plenck) and Chinese cabbage (Brassica rapa var. chinensis), taking into account the light factor and the simultaneous analysis of antioxidant activity as a marker of changes in metabolic processes.Results. The experiment has revealed a significant increase in the antioxidant activity of the microgreens during germination in the dark compared to germination in the light (in broccoli by 5.5 times, in Chinese cabbage by 4.8 times). Later on, after the seedlings are moved to the light, the differences between the light and dark versions practically disappear. After germination in the light, the antioxidant activity of microgreens in comparison with the original (dry seeds) decreased by 3-3.5 times, while in the dark β on the contrary, increased by 1.5-1.6 times. The final results of germination (germination energy and seed germination) practically do not differ in the versions. In the case of dark germination, the height of microgreens is greater (due to etiolation and stretching in the absence of light), however, later on, the differences in the versions are smoothed out. The biomass of microgreens in the version of light germination on the 4th day after sowing seeds in broccoli is by 9.1% higher, in Chinese cabbage β by 10.5%. In case of Chinese cabbage, differences remained until the end of the experiment (on the 18th day from sowing seeds), in case of broccoli they were smoothed out. Comparison of two kinds of cabbage has showen that broccoli in the closed system of the synergotron forms a much higher aboveground biomass than Chinese cabbage (on the 4th day after sowing β by 37%, on the 18th day β by 75.4% in the dark version).ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ. ΠΡΠΈ Π²ΡΡΠ°ΡΠΈΠ²Π°Π½ΠΈΠΈ ΡΠ°ΡΡΠ΅Π½ΠΈΠΉ Π² ΠΈΡΠΊΡΡΡΡΠ²Π΅Π½Π½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
(Π·Π°ΠΊΡΡΡΡΠ΅ Π°Π³ΡΠΎΡΠΊΠΎΡΠΈΡΡΠ΅ΠΌΡ) ΡΡΠ΅Π±ΡΠ΅ΡΡΡ ΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ΅Π³ΡΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ°ΠΊΡΠΎΡΠΎΠ² ΡΠΎΡΡΠ° ΡΠ°ΡΡΠ΅Π½ΠΈΠΉ, Π½Π°ΡΠΈΠ½Π°Ρ Ρ ΠΏΠ΅ΡΠ²ΡΡ
ΡΡΠ°ΠΏΠΎΠ² ΠΎΠ½ΡΠΎΠ³Π΅Π½Π΅Π·Π°. ΠΠ΄Π½ΠΈΠΌ ΠΈΠ· Π²Π°ΠΆΠ½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ²Π»ΡΠ΅ΡΡΡ Π½Π°Π»ΠΈΡΠΈΠ΅ ΠΈΠ»ΠΈ ΠΎΡΡΡΡΡΡΠ²ΠΈΠ΅ ΡΠ²Π΅ΡΠ° Π² ΠΏΠ΅ΡΠΈΠΎΠ΄ ΠΏΡΠΎΡΠ°ΡΡΠ°Π½ΠΈΡ ΡΠ΅ΠΌΡΠ½. ΠΠ»Ρ Π±ΠΎΠ»ΡΡΠΈΠ½ΡΡΠ²Π° ΡΠ°Π·Π½ΠΎΠ²ΠΈΠ΄Π½ΠΎΡΡΠ΅ΠΉ ΠΊΠ°ΠΏΡΡΡΡ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΏΡΠΎΡΠ°ΡΠΈΠ²Π°Π½ΠΈΠ΅ Π² ΡΠ΅ΠΌΠ½ΠΎΡΠ΅, ΠΎΠ΄Π½Π°ΠΊΠΎ Π΄Π»Ρ ΡΠ²Π΅ΠΆΠ΅ΡΠ±ΡΠ°Π½Π½ΡΡ
ΡΠ΅ΠΌΡΠ½ (Π² ΡΠΎΡΡΠΎΡΠ½ΠΈΠΈ ΠΏΠΎΠΊΠΎΡ) Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΡΠ²Π΅ΡΠ°. ΠΠΎ Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ½ΡΠΌ Π΄Π°Π½Π½ΡΠΌ, ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΡ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΠ²Π΅ΡΠ° Π½Π° ΠΏΡΠΎΡΠ°ΡΡΠ°Π½ΠΈΠ΅ ΡΠ΅ΠΌΡΠ½ Π½ΠΎΡΡΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΡΠΉ, Π½Π΅ΠΎΠ΄Π½ΠΎΠ·Π½Π°ΡΠ½ΡΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅Ρ ΠΈ Π²ΠΎΠΏΡΠΎΡ Π½ΡΠΆΠ΄Π°Π΅ΡΡΡ Π² Π΄Π΅ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡΡ
.ΠΠ΅ΡΠΎΠ΄Ρ. Π¦Π΅Π»ΡΡ ΡΠ°Π±ΠΎΡΡ ΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΈΠ·ΡΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΡΠ°ΡΡΠ°Π½ΠΈΡ ΡΠ΅ΠΌΡΠ½ Π±ΡΠΎΠΊΠΊΠΎΠ»ΠΈ (Brassica oleracea var. italica Plenck) ΠΈ ΠΊΠ°ΠΏΡΡΡΡ ΠΊΠΈΡΠ°ΠΉΡΠΊΠΎΠΉ (Brassica rapa var. chinensis) Ρ ΡΡΠ΅ΡΠΎΠΌ ΡΠ²Π΅ΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠ°ΠΊΡΠΎΡΠ° ΠΈ ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠΌ Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠ½ΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΊΠ°ΠΊ ΠΌΠ°ΡΠΊΠ΅ΡΠ° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ².Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΡΠ²Π»Π΅Π½ΠΎ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠ½ΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΌΠΈΠΊΡΠΎΠ·Π΅Π»Π΅Π½ΠΈ ΠΏΡΠΈ ΠΏΡΠΎΡΠ°ΡΠΈΠ²Π°Π½ΠΈΠΈ Π² ΡΠ΅ΠΌΠ½ΠΎΡΠ΅ Π² ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ Ρ ΠΏΡΠΎΡΠ°ΡΠΈΠ²Π°Π½ΠΈΠ΅ΠΌ Π½Π° ΡΠ²Π΅ΡΡ (Ρ Π±ΡΠΎΠΊΠΊΠΎΠ»ΠΈ β Π² 5,5 ΡΠ°Π·, Ρ ΠΊΠ°ΠΏΡΡΡΡ ΠΊΠΈΡΠ°ΠΉΡΠΊΠΎΠΉ β Π² 4,8 ΡΠ°Π·Π°). ΠΠΎΡΠ»Π΅ ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΌΠΈΠΊΡΠΎΠ·Π΅Π»Π΅Π½ΠΈ Π½Π° ΡΠ²Π΅Ρ, ΡΠ°Π·Π»ΠΈΡΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠ²Π΅ΡΠΎΠ²ΡΠΌ ΠΈ ΡΠ΅ΠΌΠ½ΠΎΠ²ΡΠΌ Π²Π°ΡΠΈΠ°Π½ΡΠ°ΠΌΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ ΠΈΡΡΠ΅Π·Π°Π»ΠΈ. ΠΠΎΡΠ»Π΅ ΠΏΡΠΎΡΠ°ΡΡΠ°Π½ΠΈΡ Π½Π° ΡΠ²Π΅ΡΡ Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠ½Π°Ρ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΌΠΈΠΊΡΠΎΠ·Π΅Π»Π΅Π½ΠΈ Π² ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΉ (ΡΡΡ
ΠΈΡ
ΡΠ΅ΠΌΡΠ½) ΡΠ½ΠΈΠΆΠ°Π»Π°ΡΡ Π² 3-3,5 ΡΠ°Π·Π°, Π² ΡΠΎ Π²ΡΠ΅ΠΌΡ ΠΊΠ°ΠΊ Π² ΡΠ΅ΠΌΠ½ΠΎΡΠ΅ β Π½Π°ΠΎΠ±ΠΎΡΠΎΡ, ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π»Π°ΡΡ Π² 1,5-1,6 ΡΠ°Π·Π°. ΠΡΠΈ ΡΡΠΎΠΌ ΠΊΠΎΠ½Π΅ΡΠ½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΡΠΎΡΠ°ΡΠΈΠ²Π°Π½ΠΈΡ (ΡΠ½Π΅ΡΠ³ΠΈΡ ΠΏΡΠΎΡΠ°ΡΡΠ°Π½ΠΈΡ ΠΈ Π²ΡΡ
ΠΎΠΆΠ΅ΡΡΡ ΡΠ΅ΠΌΡΠ½) ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ ΡΠ°Π·Π»ΠΈΡΠ°Π»ΠΈΡΡ ΠΏΠΎ Π²Π°ΡΠΈΠ°Π½ΡΠ°ΠΌ. ΠΡΠΈ ΡΠ΅ΠΌΠ½ΠΎΠ²ΠΎΠΌ ΠΏΡΠΎΡΠ°ΡΠΈΠ²Π°Π½ΠΈΠΈ Π²ΡΡΠΎΡΠ° ΠΌΠΈΠΊΡΠΎΠ·Π΅Π»Π΅Π½ΠΈ Π±ΠΎΠ»ΡΡΠ΅ (Π·Π° ΡΡΠ΅Ρ ΡΡΠΈΠΎΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ Π²ΡΡΡΠ³ΠΈΠ²Π°Π½ΠΈΡ ΠΏΡΠΈ ΠΎΡΡΡΡΡΡΠ²ΠΈΠΈ ΡΠ²Π΅ΡΠ°), ΠΎΠ΄Π½Π°ΠΊΠΎ Π² Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΌ ΡΠ°Π·Π»ΠΈΡΠΈΡ ΠΏΠΎ Π²Π°ΡΠΈΠ°Π½ΡΠ°ΠΌ ΡΠ³Π»Π°ΠΆΠΈΠ²Π°ΡΡΡΡ. ΠΠΈΠΎΠΌΠ°ΡΡΠ° ΠΌΠΈΠΊΡΠΎΠ·Π΅Π»Π΅Π½ΠΈ Π½Π° ΡΠ²Π΅ΡΡ Π½Π° 4-Π΅ ΡΡΡΠΊΠΈ ΠΏΠΎΡΠ»Π΅ ΠΏΠΎΡΠ΅Π²Π° ΡΠ΅ΠΌΡΠ½ Ρ Π±ΡΠΎΠΊΠΊΠΎΠ»ΠΈ β Π²ΡΡΠ΅ Π½Π° 9,1%, Ρ ΠΊΠ°ΠΏΡΡΡΡ ΠΊΠΈΡΠ°ΠΉΡΠΊΠΎΠΉ β Π½Π° 10,5%. Π£ ΠΊΠ°ΠΏΡΡΡΡ ΠΊΠΈΡΠ°ΠΉΡΠΊΠΎΠΉ ΡΠ°Π·Π»ΠΈΡΠΈΡ ΡΠΎΡ
ΡΠ°Π½ΡΠ»ΠΈΡΡ Π΄ΠΎ Π·Π°Π²Π΅ΡΡΠ΅Π½ΠΈΡ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ° (Π½Π° 18-Π΅ ΡΡΡΠΊΠΈ ΠΎΡ ΠΏΠΎΡΠ΅Π²Π° ΡΠ΅ΠΌΡΠ½), Ρ Π±ΡΠΎΠΊΠΊΠΎΠ»ΠΈ β ΡΠ³Π»Π°ΠΆΠΈΠ²Π°Π»ΠΈΡΡ. Π‘ΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ Π΄Π²ΡΡ
ΡΠ°Π·Π½ΠΎΠ²ΠΈΠ΄Π½ΠΎΡΡΠ΅ΠΉ ΠΊΠ°ΠΏΡΡΡΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, ΡΡΠΎ Π±ΡΠΎΠΊΠΊΠΎΠ»ΠΈ Π² Π·Π°ΠΌΠΊΠ½ΡΡΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠ΅ ΡΠΈΠ½Π΅ΡΠ³ΠΎΡΡΠΎΠ½Π° ΡΠΎΡΠΌΠΈΡΡΠ΅Ρ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π±ΠΎΠ»ΡΡΡΡ Π½Π°Π΄Π·Π΅ΠΌΠ½ΡΡ Π±ΠΈΠΎΠΌΠ°ΡΡΡ, ΡΠ΅ΠΌ ΠΊΠ°ΠΏΡΡΡΠ° ΠΊΠΈΡΠ°ΠΉΡΠΊΠ°Ρ (Π½Π° 4-Π΅ ΡΡΡΠΊΠΈ ΠΏΠΎΡΠ»Π΅ ΠΏΠΎΡΠ΅Π²Π° β Π½Π° 37%, Π½Π° 18-Π΅ ΡΡΡΠΊΠΈ β Π½Π° 75,4% Π² ΡΠ΅ΠΌΠ½ΠΎΠ²ΠΎΠΌ Π²Π°ΡΠΈΠ°Π½ΡΠ΅).
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