Detection and communications device employing stochastic resonance

Claim 2

A detecting device employing the phenomenon of stochastic resonance to improve signal-to-noise ratio (SNR) and detector sensitivity, said device comprising: a stochastic resonance element comprising a superconducting loop having at least one Josephson junction, said loop having at least two stable states of internal magnetic flux and being transitionable from one state to another; means for applying noise to said loop; means for coupling a magnetic flux input to said loop of unknown and insufficient amplitude to cause said loop to change state, the noise and flux input together in said loop inducing said loop to transition stochastically from one state to another to produce an output signal; and means for detecting the output signal of said loop indicative of the internal magnetic flux state transitions of said loop, thereby determining the existence of and information about the input magnetic flux.

Claim 3

The device recited in claim 1, wherein said noise applying means comprises a noise source having an arbitrary frequency spectrum.

Claim 4

The device recited in claim 2, wherein said noise applying means further comprises means for converting the noise energy into a magnetic flux.

Claim 5

The device recited in claim 3, wherein said noise applying means further comprises means for coupling the magnetic flux form of the noise energy to said superconducting loop.

Claim 6

The device recited in claim 1, wherein said noise applying means further comprises means for varying the amplitude of the noise energy, which amplitude variations change the rate of transitions between magnetic flux states of said superconducting loop to achieve maximization of the SNR, thereby inducing the phenomenon of stochastic resonance in said superconducting loop.

Claim 7

The device recited in claim 1, wherein said superconducting loop has at least two Josephson junctions, said device further comprising means to apply a biasing current across said junctions to adjust the energy barrier between the internal flux states of said superconducting loop.

Claim 8

The device recited in claim 1, and further comprising means for applying a magnetic flux to said Josephson junction to adjust the energy barrier between the internal flux states of said superconducting loop.

Claim 9

The device recited in claim 7, whereby a dc magnetic flux is also added to the flux input to further affect the output SNR.

Claim 10

The device recited in claim 7, whereby a dc magnetic flux is also added to the noise to further affect the output SNR.

Claim 11

The device recited in claim 1, and further comprising means for recording the variations of the internal flux state of said superconducting loop as a function of time.

Claim 12

A detecting device employing the phenomenon of stochastic resonance to improve signal-to-noise ratio (SNR) and detector sensitivity, said device comprising: a plurality of stochastic resonance elements, each comprising a superconducting loop having at least one Josephson junction connected in an array, each said loop having at least two stable states of internal magnetic flux and being transitionable from one state to another; means for applying noise to each said loop; means for coupling a magnetic flux input to each said loop of unknown and insufficient amplitude to cause said loop to change state, the noise and flux input together in each said loop inducing each said loop to transition stochastically from one state to another to produce an output signal; and means for effectively combining the output signals of said loops and detecting the output signal of said array indicative of the combined internal magnetic flux state transitions of said array, thereby determining the existence of and information about the input magnetic flux.

Claim 13

A detecting device employing the phenomenon of stochastic resonance to improve signal-to-noise ratio (SNR) and detector sensitivity, said device comprising: a plurality of stochastic resonance elements, each comprising a superconducting loop having at least one Josephson junction connected in an array, each said loop having at least two stable states of internal magnetic flux and being transitionable from one state to another; means for applying noise to each said loop; means for coupling a magnetic flux input to each said loop of unknown and insufficient amplitude to cause said loop to change state, the noise and flux input together in each said loop inducing each said loop to transition stochastically from one state to another to produce an output signal; and means for effectively combining the output signals of said loops and detecting the output signal of said array indicative of the combined internal magnetic flux state transitions of said array, thereby determining the existence of and information about the input magnetic flux.

Claim 14

The device recited in claim 11, wherein said superconducting loops in said array are connected in parallel.

Claim 15

The device recited in claim 11, wherein said superconducting loops in said array are connected in series.

Claim 16

The device recited in claim 11, wherein said superconducting loops in said array are all connected to each other and the output of said array is an enhanced composite of all said superconducting loops in said array.

Claim 19

The device recited in claim 6, wherein said bias applying means further comprises means for varying the amplitude of the bias current, which amplitude variations change the rate of transitions between magnetic flux states of said superconducting loop to achieve maximization of the SNR, thereby inducing the phenomenon of stochastic resonance in said superconducting loop.

Claim 20

The device recited in claim 1, and further comprising means for applying a dc magnetic flux to the flux input to further affect the output SNR.

Claim 21

The device recited in claim 1, and further comprising means for applying a dc magnetic flux to the applied noise to further affect the output SNR.

Claim 22

The device recited in claim 6, and further comprising means for applying a dc magnetic flux to the flux input to further affect the output SNR.

Claim 23

The device recited in claim 6, and further comprising means for applying a dc magnetic flux to the applied noise to further affect the output SNR.

Claim 24

The device recited in claim 7, wherein said magnetic flux applying means comprises means for varying the amplitude of the applied magnetic flux, which amplitude variations adjusts the energy barrier to achieve maximization of SNR, thereby inducing the phenomenon of stochastic resonance in said superconducting loop.

Claim 25

The device recited in claim 8, whereby the dc magnetic flux added to the flux input is variable in amplitude, which amplitude variations adjusts the energy barrier to achieve maximization of SNR, thereby inducing the phenomenon of stochastic resonance in said superconducting loop.

Claim 26

The device recited in claim 9, wherein the dc magnetic flux added to applied noise is variable in amplitude, which amplitude variations adjusts the energy barrier to achieve maximization of SNR, thereby inducing the phenomenon of stochastic resonance in said superconducting loop.