Modeling-based prediction of current oscillation with the Josephson frequency in voltage-biased phase-slip center filaments

Abstract In this article, we demonstrate that the voltage-biased phase-slip center (PSC) can act as a direct equivalent (not merely an analogy) of the Josephson effect in Josephson junctions (JJs). We analyze the behavior of PSCs in the case when a constant voltage V is applied to the superconducting filament. The analysis is performed using finite element modeling on the basis of time-dependent Ginzburg–Landau (TDGL) equations. It reveals that the current in the filament oscillates with the Josephson frequency $$\omega =2eV/\hbar $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>ω</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> <mml:mi>e</mml:mi> <mml:mi>V</mml:mi> <mml:mo>/</mml:mo> <mml:mi>ħ</mml:mi> </mml:mrow> </mml:math> . This fact may have important corollaries in practice.

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Publication Details

Journal
Quantum Studies Mathematics and Foundations
Published
2025-09-25
DOI
https://doi.org/10.1007/s40509-025-00374-7
Primary Topic
Semiconductor Quantum Structures and Devices
Type
article
Field-Weighted Citation Impact
0.00

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article

Modeling-based prediction of current oscillation with the Josephson frequency in voltage-biased phase-slip center filaments

Armen Gulian
Quantum Studies Mathematics and Foundations
Semiconductor Quantum Structures and Devices
article

Modeling-based prediction of current oscillation with the Josephson frequency in voltage-biased phase-slip center filaments

Armen Gulian
article en

Abstract

Abstract In this article, we demonstrate that the voltage-biased phase-slip center (PSC) can act as a direct equivalent (not merely an analogy) of the Josephson effect in Josephson junctions (JJs). We analyze the behavior of PSCs in the case when a constant voltage V is applied to the superconducting filament. The analysis is performed using finite element modeling on the basis of time-dependent Ginzburg–Landau (TDGL) equations. It reveals that the current in the filament oscillates with the Josephson frequency $$\omega =2eV/\hbar $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>ω</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> <mml:mi>e</mml:mi> <mml:mi>V</mml:mi> <mml:mo>/</mml:mo> <mml:mi>ħ</mml:mi> </mml:mrow> </mml:math> . This fact may have important corollaries in practice.

Quantum Studies Mathematics and FoundationsVol. 12(3)
Quantum Devices (United States) (US)
Office of Naval Research
Openalex Percentile: Top 79%
Semiconductor Quantum Structures and Devices
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