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Thermally activated flux motion in optimally electron-doped (Ca0.85La0.15)(10)(Pt3As8)(Fe2As2)(5) and Ca-10(Pt3As8)((Fe0.92Pt0.08)(2)As-2)(5) single crystals
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Title
Thermally activated flux motion in optimally electron-doped (Ca0.85La0.15)(10)(Pt3As8)(Fe2As2)(5) and Ca-10(Pt3As8)((Fe0.92Pt0.08)(2)As-2)(5) single crystals
Issued Date
2020-12
Citation
Choi, Woojae. (2020-12). Thermally activated flux motion in optimally electron-doped (Ca0.85La0.15)(10)(Pt3As8)(Fe2As2)(5) and Ca-10(Pt3As8)((Fe0.92Pt0.08)(2)As-2)(5) single crystals. Results in Physics, 19, 103430. doi: 10.1016/j.rinp.2020.103430
Type
Article
Author Keywords
Vortex dynamicsVortex phase diagramThermally activated flux motionVortex glassCritical regionVortex dimensional crossover
Keywords
VORTEX-LIQUIDSUPERCONDUCTIVITYENERGYDEPENDENCETRANSITIONFIELDFLOWTC
ISSN
2211-3797
Abstract
The temperature dependence of the electric resistivity measured in various magnetic fields was analyzed by the vortex glass theory and the thermally activated flux motion (TAFM) theory. The vortex glass-to-vortex liquid (GTL) transition Tg obtained from the analysis shows a temperature dependence of BgT=B01-T/Tcm. The vortex liquid region is divided into the critical region existing in a finite temperature region just above Tg and the TAFM region present in the finite temperature region above it. In the critical region, the activation energy is expressed as Ueff=kBTTc-T/(Tc-Tg), whereas in the TAFM region, the activity energy is expressed as temperature-nonlinear UT,B=U0B1-tq. In the GTL transition, (Ca0.85La0.15)10(Pt3As8)(Fe2As2)5 maintains the 3D vortex structure without exhibiting dimension crossover of the vortex, but Ca10(Pt3As8)((Fe0.92Pt0.08)2As2)5 exhibits the dimension crossover from the 3D vortex glass to the 2D vortex liquid. © 2020 The Author(s)
URI
http://hdl.handle.net/20.500.11750/12622
DOI
10.1016/j.rinp.2020.103430
Publisher
Elsevier BV
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권용성
Kwon, Yong Seung권용성

Department of Physics and Chemistry

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