# Local flux-flow instability in superconducting films near Tc

## TL;DR

This paper develops a theory of local flux-flow instability in superconducting films near Tc, explaining abrupt voltage jumps in current-voltage characteristics and aligning with experimental data, with implications for fast photon detection.

## Contribution

It introduces a novel local instability model for flux flow in superconducting films, differing from traditional global models, and applies it to experimental observations.

## Key findings

- Theory predicts local flux-flow instability occurs in narrow film strips.
- Model agrees with Nb film experiments on voltage jumps.
- Implications for superconducting photon detectors.

## Abstract

Larkin and Ovchinnikov established that the viscous flow of magnetic flux quanta in current-biased superconductor films placed in a perpendicular magnetic field can lose stability due to a decrease in the vortex viscosity coefficient $\eta$ with increasing velocity of the vortices $v$. The dependence of $\eta$ on $v$ leads to a $nonlinear$ section in the current-voltage ($I$-$V$) curve which ends at the flux-flow instability point with a voltage jump to a highly resistive state. At the same time, in contradistinction with the nonlinear conductivity regime, instability jumps often occur in $linear$ $I$-$V$ sections. Here, for the elucidation of such jumps we develop a theory of local instability of the magnetic flux flow occurring not in the entire film but in a narrow strip across the film width in which vortices move much faster than outside it. The predictions of the developed theory are in agreement with experiments on Nb films for which the heat removal coefficients and the inelastic scattering times of quasiparticles are deduced. The presented model of local instability is also relevant for the characterization of superconducting thin films whose performance is examined for fast single-photon detection.