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Stochastic resonance in superconducting loops containing Josephson junctions. Numerical simulation
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10.1063/1.2400686
/content/aip/journal/ltp/32/12/10.1063/1.2400686
http://aip.metastore.ingenta.com/content/aip/journal/ltp/32/12/10.1063/1.2400686
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Potential function of a superconducting loop containing a Josephson junction. The hysteresis parameter , the external magnetic flux . Inset: scheme of the rf SQUID ring; is the inductance of the ring, is the magnetic flux through the ring, and and are the critical current and the capacitance of the Josephson junction, respectively.

Image of FIG. 2.
FIG. 2.

Symmetric bistable potential of the rf SQUID ring for and ; the values of the flux corresponding to the minima of the potential , the middle of the barrier , and the potential barrier height (a). A diagram of the transition of the system from one stable state to another upon the warping of the potential by an external magnetic flux (b).

Image of FIG. 3.
FIG. 3.

Time series of a periodic input signal (white curves), the signal with noise, (black), and the output signal (gray) (a); the Fourier spectra of the output signal at different noise levels (b).

Image of FIG. 4.
FIG. 4.

Dependence of the flux gain and signal-to-noise ratio on the noise level in a one-ring rf SQUID. Parameter , input signal amplitude , signal frequency , noise cutoff frequency , and number of points in the time series 32768. The curve of the SNR does not appear smooth because of the scatter in the determination of the position of the noise shelf.

Image of FIG. 5.
FIG. 5.

Even and odd harmonics in the Fourier spectrum of the output signal at different levels of the constant bias flux. The noise intensity is equal to that value at which the maximum stochastic amplification of the signal is observed.

Image of FIG. 6.
FIG. 6.

Values of the first three harmonics of the main signal in the output Fourier spectrum as a function of the input bias flux ; . The noise intensity is equal to that value at which the maximum stochastic amplification of the signal is observed.

Image of FIG. 7.
FIG. 7.

Potential surface for two coupled rf SQUID rings in the absence of additional bias, input signal, and noise at the following parameter values: , (a); , , (b), , (c); , (d), and with biasing by an external signal for , , (e); , , (f).

Image of FIG. 8.
FIG. 8.

Flux gain as a function of the noise level and coupling coefficient for identical rings (a) and different rings (b). Signal amplitude , signal frequency , hysteresis parameters (a); , (b).

Image of FIG. 9.
FIG. 9.

Potential of a 4-terminal SQUID for , , .

Image of FIG. 10.
FIG. 10.

Flux gain as a function of the noise level in the ring of a 4-terminal SQUID. Parameters: , , .

Image of FIG. 11.
FIG. 11.

Possible configurations of stochastic antennas for receiving weak quasi-harmonic signals with the use of SQUIDs: a,b—antennas for SQUID microscopes, c—antennas for low-frequency radar, geophysical magnetometry, and biomagnetic measurements.

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/content/aip/journal/ltp/32/12/10.1063/1.2400686
2006-12-01
2014-04-24
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Stochastic resonance in superconducting loops containing Josephson junctions. Numerical simulation
http://aip.metastore.ingenta.com/content/aip/journal/ltp/32/12/10.1063/1.2400686
10.1063/1.2400686
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