# Measurements of microwave vortex response in dc magnetic fields in Tl$_2$Ba$_2$CaCu$_2$O$_{8+x}$ films

## TL;DR

This study investigates the microwave vortex response of Tl$_2$Ba$_2$CaCu$_2$O$_{8+x}$ superconducting films in magnetic fields, revealing complex vortex dynamics, high depinning frequencies, and significant dissipation affecting potential applications.

## Contribution

It provides the first detailed measurement of the millimeter-wave vortex response in Tl$_2$Ba$_2$CaCu$_2$O$_{8+x}$ films and analyzes the underlying vortex dynamics and dissipation mechanisms.

## Key findings

- Multiple contributions to surface impedance change depending on temperature and field.
- High vortex motion depinning frequencies were observed.
- Small vortex viscosity indicates large dissipation and limits applications.

## Abstract

There is a renewed interest in superconductors for high-frequency applications, leading to a reconsideration of already known low-$T_c$ and high-$T_c$ materials. In this view, we present an experimental investigation of the millimeter-wave response in moderate magnetic fields of Tl$_2$Ba$_2$CaCu$_2$O$_{8+x}$ superconducting films with the aim of identifying the mechanisms of the vortex-motion-induced response. We measure the dc magnetic-field-dependent change of the surface impedance, $\Delta Z_s(H) = \Delta R_s(H) + i\Delta X_s(H)$ at 48 GHz by means of the dielectric resonator method. We find that the overall response is made up of several contributions, with different weights depending on the temperature and field: a possible contribution from Josephson or Abrikosov-Josephson fluxons at low fields; a seemingly conventional vortex dynamics at higher fields; a significant pair breaking in the temperature region close to $T_c$. We extract the vortex motion depinning frequency $f_p$, which attains surprisingly high values. However, by exploiting the generalized model for relaxational dynamics we show that this result come from a combination of a pinning constant $k_p$ arising from moderate pinning, and a vortex viscosity $\eta$ with anomalously small values. This latter fact, implying large dissipation, is likely a result from a peculiar microscopic structure and thus poses severe limits to the application of Tl$_2$Ba$_2$CaCu$_2$O$_{8+x}$ in a magnetic field.