Abstract

We study the dissipative conductivity $\sigma_1$ of a dirty superconductor with a finite Dynes parameter $\Gamma$ under a dc-biased weak time-dependent field. The Usadel equation for the current-carrying state is solved to calculate the pair potential, penetration depth, supercurrent density, and quasiparticle spectrum. It is shown that, while the depairing current density $j_d$ for $\Gamma=0$ is coincident with the Kupriyanov-Lukichev theory, a finite $\Gamma$ decreases the superfluid density, resulting in a reduction of $j_d$. The broadening of the peaks of the quasiparticle density of states induced by a combination of a finite $\Gamma$ and a dc bias can reduce $\sigma_1$ below that for the ideal dirty BCS superconductor with $\Gamma=0$, while subgap states at Fermi level proportional to $\Gamma$ results in a residual conductivity at $T\to 0$. We find the optimum combination of $\Gamma$ and the dc bias to minimize $\sigma_1$ by scanning all $\Gamma$ and all currents up to $j_d$. By using the results, it is possible to improve $j_d$ and reduce electromagnetic dissipation in various superconducting quantum devices.

Highlights

  • Electromagnetic properties of superconductors have been actively studied in many fields of fundamental and applied physics, including applications to superconducting radiofrequency (SRF) cavities for particle accelerators [1,2], microresonators for kinetic inductance detectors [3] and quantum computations [4], and single-photon detectors [5]

  • The dissipative conductivity σ1 is the real part of complex conductivity, which is sensitive to the details of the quasiparticle spectrum

  • II, we briefly review the quasiclassical theory for a dirty superconductor

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Summary

INTRODUCTION

Electromagnetic properties of superconductors have been actively studied in many fields of fundamental and applied physics, including applications to superconducting radiofrequency (SRF) cavities for particle accelerators [1,2], microresonators for kinetic inductance detectors [3] and quantum computations [4], and single-photon detectors [5]. Pair-breaking effects due to realistic materials features including magnetic impurities, Dynes parameters, and a proximity-coupled normal layer at the surface can reduce Rs via the broadening of the DOS peaks [26]. Sparse magnetic impurities can reduce Rs by ≈50% for the weak rf field It was shown [27] that a combination of such pair-breaking effects in materials and the pair-breaking current can shift the minimum in nonlinear Rs(Hrf ), consistent with the experimental observations that the. To study a superconductor under a dc bias and to find the optimum dc bias that minimizes electromagnetic dissipation would attract attention in superconducting device communities From fundamental perspectives, this system offers a stage for direct observations of the effects of the broadening of the DOS peaks on σ1 [23,36,37].

THEORY
ZERO-CURRENT STATE
CURRENT-CARRYING STATE
Depairing current density
Density of states
Dissipative conductivity σ1 under a dc bias
Zero-current state
Current-carrying state
Temperature and frequency dependences
Deparing current density
CONCLUSION

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