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Second magnetization peak, anomalous field penetration, and Josephson vortices in KCa[Formula: see text]Fe[Formula: see text]As[Formula: see text]F[Formula: see text] bilayer pnictide superconductor.
Lopes, P V; Sundar, Shyam; Salem-Sugui, S; Hong, Wenshan; Luo, Huiqian; Ghivelder, L.
Afiliação
  • Lopes PV; Instituto de Fisica, Universidade Federal do Rio de Janeiro, Rio de Janeiro, RJ, 21941-972, Brazil.
  • Sundar S; Instituto de Fisica, Universidade Federal do Rio de Janeiro, Rio de Janeiro, RJ, 21941-972, Brazil. shyam.phy@gmail.com.
  • Salem-Sugui S; School of Physics and Astronomy, University of St. Andrews, St Andrews, KY16 9SS, UK. shyam.phy@gmail.com.
  • Hong W; Instituto de Fisica, Universidade Federal do Rio de Janeiro, Rio de Janeiro, RJ, 21941-972, Brazil. said@if.ufrj.br.
  • Luo H; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Ghivelder L; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100190, China.
Sci Rep ; 12(1): 20359, 2022 Nov 27.
Article em En | MEDLINE | ID: mdl-36437284
ABSTRACT
We performed magnetization measurements in a single crystal of the anisotropic bilayer pnictide superconductor KCa[Formula see text]Fe[Formula see text]As[Formula see text]F[Formula see text], with [Formula see text] [Formula see text] 34 K, for [Formula see text] [Formula see text] [Formula see text]-axis and [Formula see text] [Formula see text] [Formula see text]-planes. A second magnetization peak (SMP) was observed in the isothermal M(H) curves measured below 16 K for [Formula see text] [Formula see text] [Formula see text]-planes. A peak in the temperature variation of the critical current density, [Formula see text](T), at 16 K, strongly suggests the emergence of Josephson vortices at lower temperatures, which leads to the SMP in the sample. In addition, it is noticed that the appearance of Josephson vortices below 16 K renders easy magnetic flux penetration. A detailed vortex dynamics study suggests that the SMP can be explained in terms of elastic pinning to plastic pinning crossover. Furthermore, contrary to the common understanding, the temperature variation of the first peak field, [Formula see text], below and above 16 K, behaves non-monotonically. A highly disordered vortex phase, governed by plastic pinning, has been observed between 17 and 23 K, within a field region around an extremely large first peak field. Pinning force scaling suggests that the point defects are the dominant source of pinning for H [Formula see text] [Formula see text]-planes, whereas, for H [Formula see text] [Formula see text]-axis, point defects in addition to surface defects are at play. Such disorder contributes to the pinning due to the variation in charge carrier mean free path, [Formula see text] -pinning. Moreover, the large [Formula see text] observed in our study is consistent with the literature, which advocates this material for high magnetic field applications.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Sci Rep Ano de publicação: 2022 Tipo de documento: Article País de afiliação: Brasil

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Sci Rep Ano de publicação: 2022 Tipo de documento: Article País de afiliação: Brasil
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