<p>We have studied non-equilibrium states in NbTi films deposited on fused silica under different surrounding conditions using electrical current pulses. When the applied current exceeds the depairing current <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(I_{c}\)</EquationSource> </InlineEquation>, a voltage response is observed after a characteristic delay time <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(t_{d}\)</EquationSource> </InlineEquation>. Although the sample dimensions are much larger than the coherence length <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\xi\)</EquationSource> </InlineEquation>, the localized micro-metric region formed corresponds to a hotspot. The delay times are quantitatively described using the Time-Dependent Ginzburg–Landau (TDGL) theory of M.&#xa0;Tinkham, enabling the determination of filament cooling times for the same sample in both liquid helium and vacuum. We find cooling times of about <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\tau _{d} = 6.0 \pm 0.5\)</EquationSource> </InlineEquation>&#xa0;ns in vacuum and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(5.3 \pm 0.5\)</EquationSource> </InlineEquation>&#xa0;ns in liquid helium. These results demonstrate that liquid helium has only a minor effect on the film cooling time, with most of the heat being transferred into the substrate via phonons. </p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Dynamic Study of the Environmental Impact on Gap Relaxation Time in NbTi Superconducting Wire

  • K. Harrabi

摘要

We have studied non-equilibrium states in NbTi films deposited on fused silica under different surrounding conditions using electrical current pulses. When the applied current exceeds the depairing current \(I_{c}\) , a voltage response is observed after a characteristic delay time \(t_{d}\) . Although the sample dimensions are much larger than the coherence length \(\xi\) , the localized micro-metric region formed corresponds to a hotspot. The delay times are quantitatively described using the Time-Dependent Ginzburg–Landau (TDGL) theory of M. Tinkham, enabling the determination of filament cooling times for the same sample in both liquid helium and vacuum. We find cooling times of about \(\tau _{d} = 6.0 \pm 0.5\)  ns in vacuum and \(5.3 \pm 0.5\)  ns in liquid helium. These results demonstrate that liquid helium has only a minor effect on the film cooling time, with most of the heat being transferred into the substrate via phonons.