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Annalen der Physik

Nonlinear dynamics in a high‐gain amplifier: the dc SQUID

Adi R. Bulsara, Kurt A. Wiesenfeld, Mario E. Inchiosa

Published Sep 25, 2000• 0 citations
Publisher

Abstract

Abstract We study the detection of very weak time‐periodic magnetic signals via a double‐junction (dc) Superconducting Quantum Interference Device (SQUID). The device, represented by two coupled nonlinear differential equations for the quantum mechanical junction phase differences, admits long‐time static or oscillatory solutions, the transition between them being easily controlled by experimentally accessible parameters. Gain is maximal when the device is tuned to the onset of the oscillatory solutions; i.e., when the minima in the 2D potential function disappear. We concentrate on the SQUID dynamics near this critical point and compute the oscillation frequency via a center manifold reduction of the full 2D dynamics. Knowing this frequency permits its exploitation as a detection/classification tool in magnetic remote sensing applications.

DOI
10.1002/andp.200051209-1003

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Nonlinear dynamics in a high-gain amplifier: the dc SQUID

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We study the detection of very weak time-periodic magnetic signals via a double-junction (dc) Superconducting Quantum Interference Device (SQUID). The device, represented by two coupled nonlinear differential equations for the quantum mechanical junction phase differences, admits long-time static or oscillatory solutions, the transition between them being easily controlled by experimentally accessible parameters. Gain is maximal when the device is tuned to the onset of the oscillatory solutions; i.e., when the minima in the 2D potential function disappear. We concentrate on the SQUID dynamics near this critical point and compute the oscillation frequency via a center manifold reduction of the full 2D dynamics. Knowing this frequency permits its exploitation as a detection/classification tool in magnetic remote sensing applications.

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Conventional rf SQUIDs (superconducting quantum interference devices) consist of a superconducting loop interrupted by one weak link, and when read out via a tank circuit they produce output signals in the order of a few tens of microvolts. When the single weak link is replaced by a dc SQUID (a superconducting loop with two junctions) a so-called double quantization loop SQUID is formed. In this paper it is shown theoretically, and supported experimentally with thin-film devices of three different designs, that the general behaviour can be explained by a simplified picture of the fixed critical current of the single junction of the rf SQUID being replaced by an effective critical current of a dc SQUID loop that is varied by the applied magnetic flux (i.e., we have a rf SQUID with a variable β parameter). A more detailed analysis of the experimental data and the theory of this novel device reveals its interesting nonlinear character and shows the deviations from this simple picture. It is demonstrated experimentally that output signals in the order of ≥1 mV can be obtained with a suitable read-out mode for the tank circuit, a clear advantage when compared to conventional rf SQUIDs. With respect to dc SQUIDs, the coupling to integrated planar input coils will be unproblematic since no microwave resonances should occur in the structures.

Journal of Applied Physics•Aug 15, 1993•16 citations
Abstract We study the detection of very weak time‐periodic magnetic signals via a double‐junction (dc) Superconducting Quantum Interference Device (SQUID). The device, represented by two coupled nonlinear differential equations for the quantum mechanical junction phase differences, admits long‐time static or oscillatory solutions, the transition between them being easily controlled by experimentally accessible parameters. Gain is maximal when the device is tuned to the onset of the oscillatory solutions; i.e., when the minima in the 2D potential function disappear. We concentrate on the SQUID dynamics near this critical point and compute the oscillation frequency via a center manifold reduction of the full 2D dynamics. Knowing this frequency permits its exploitation as a detection/classification tool in magnetic remote sensing applications.
We study the detection of very weak time-periodic magnetic signals via a double-junction (dc) Superconducting Quantum Interference Device (SQUID). The device, represented by two coupled nonlinear differential equations for the quantum mechanical junction phase differences, admits long-time static or oscillatory solutions, the transition between them being easily controlled by experimentally accessible parameters. Gain is maximal when the device is tuned to the onset of the oscillatory solutions; i.e., when the minima in the 2D potential function disappear. We concentrate on the SQUID dynamics near this critical point and compute the oscillation frequency via a center manifold reduction of the full 2D dynamics. Knowing this frequency permits its exploitation as a detection/classification tool in magnetic remote sensing applications.
We study the detection of very weak time-periodic magnetic signals via a double-junction (dc) Superconducting Quantum Interference Device (SQUID). The device, represented by two coupled nonlinear differential equations for the quantum mechanical junction phases, admits of long-time static or oscillatory solutions, the transition being controllable by experimental parameters. Signal detection is optimal when the device is “tuned” to the onset of the oscillatory solutions; i.e., when the minima in the 2D potential function disappear. Modeling the device via a derived input-output transfer characteristic yields a response (quantified via the signal-to-noise ratio at the signal frequency) in good agreement with recent experiments. We also present some preliminary results pertaining to coupled dc SQUIDs, taking into account the (incoherent) thermal noise sources in each of the Josephson junctions. As might be expected from previous work, coupling the SQUIDs and/or summing their outputs enhances the response to the external signal.
We describe a new dc-superconducting quantum interference device (SQUID) circuit of the FM type, which has a large coefficient for converting an applied magnetic flux into a frequency of MHz band or a lower band. The circuit consists of a SQUID amplifier composed of two stages, formed by a superconducting weak link and two dc-SQUID elements with nonhysteretic characteristics. In the first stage, the weak link and dc-SQUID elements are connected in parallel and operated by a common bias voltage. Since the respective elements oscillate with high frequencies by the ac Josephson effect, the two frequencies interact with each other, so that, the first stage generates a beat signal of a lower frequency. In the second stage, the other dc-SQUID element with a intrinsic flux gain enhances the beat signal generated during the first stage. A theoretical analysis of the circuit with computer simulation shows that the beat frequency is a periodical function of the magnetic flux, and the SQUID amplifier with two stages can improve the flux sensitivity.
We present a study of the controllable nonlinear dynamics of a micromechanical beam coupled to a dc-SQUID (superconducting quantum interference device). The coupling between these systems places the modes of the beam in a highly nonlinear potential, whose shape can be altered by varying the bias current and applied flux of the SQUID. We detect the position of the beam by placing it in an optical cavity, which sets free the SQUID to be used solely for actuation. This enables us to probe the previously unexplored full parameter space of this device. We measure the frequency response of the beam and find that it displays a Duffing oscillator behavior which is periodic in the applied magnetic flux. To account for this, we develop a model based on the standard theory for SQUID dynamics. In addition, with the aim of understanding if the device can reach nonlinearity at the single phonon level, we use this model to show that the responsivity of the current circulating in the SQUID to the position of the beam can become divergent, with its magnitude limited only by noise. This suggests a direction for the generation of macroscopically distinguishable superposition states of the beam.
We present a study of the controllable nonlinear dynamics of a micromechanical beam coupled to a dc-SQUID (superconducting quantum interference device). The coupling between these systems places the modes of the beam in a highly nonlinear potential, whose shape can be altered by varying the control parameters of the SQUID. We detect the position of the beam by placing it in an optical cavity, which frees the SQUID to be used solely for actuation. This enables us to probe the previously unexplored full parameter space of this device. We measure the frequency response of the beam and find that it displays a periodic dependence on applied magnetic flux. To account for this, we develop a model based on the standard theory for SQUID dynamics. In addition, with the aim of understanding if the device can reach nonlinearity at the single phonon level, we use this model to show that the responsivity of the current circulating in the SQUID to the position of the beam can become divergent, with its magnitude limited only by noise. This suggests a direction for the generation of macroscopically distinguishable superposition states of the beam.
Conventional rf SQUIDs (superconducting quantum interference devices) consist of a superconducting loop interrupted by one weak link, and when read out via a tank circuit they produce output signals in the order of a few tens of microvolts. When the single weak link is replaced by a dc SQUID (a superconducting loop with two junctions) a so-called double quantization loop SQUID is formed. In this paper it is shown theoretically, and supported experimentally with thin-film devices of three different designs, that the general behaviour can be explained by a simplified picture of the fixed critical current of the single junction of the rf SQUID being replaced by an effective critical current of a dc SQUID loop that is varied by the applied magnetic flux (i.e., we have a rf SQUID with a variable β parameter). A more detailed analysis of the experimental data and the theory of this novel device reveals its interesting nonlinear character and shows the deviations from this simple picture. It is demonstrated experimentally that output signals in the order of ≥1 mV can be obtained with a suitable read-out mode for the tank circuit, a clear advantage when compared to conventional rf SQUIDs. With respect to dc SQUIDs, the coupling to integrated planar input coils will be unproblematic since no microwave resonances should occur in the structures.