Memory effects and peak effect in type II superconductors

A large amount of experimental and theoretical work has been devoted to understand memory effects (ME) in the solid vortex lattice (VL) but has remained, however, controversial until now. In the vicinity of the anomaly known as the peak effect (PE) both the VL mobility and the measured critical curr...

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Autores principales: Pasquini, G., Luna, D., Eismann, B., Bettachini, V., Bekeris, V.
Formato: JOUR
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_09214526_v398_n2_p420_Pasquini
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spelling todo:paper_09214526_v398_n2_p420_Pasquini2023-10-03T15:45:19Z Memory effects and peak effect in type II superconductors Pasquini, G. Luna, D. Eismann, B. Bettachini, V. Bekeris, V. High and low Tc superconductors vortex lattice Memory effects Peak effect Vortex lattice Labusch constant Memory effects Peak effect Vortex lattice Critical current density (superconductivity) Crystal lattices Nonlinear analysis Superconducting materials A large amount of experimental and theoretical work has been devoted to understand memory effects (ME) in the solid vortex lattice (VL) but has remained, however, controversial until now. In the vicinity of the anomaly known as the peak effect (PE) both the VL mobility and the measured critical current density are found to be dependent of the dynamical history of the sample, in both low Tc (LTS) and high Tc (HTS) superconductors. Experiments in YBa2Cu3O7 (YBCO) crystals have shown that the mobility of the VL increases after assisting the system with a symmetric AC field (or current) of moderated amplitude. On the other hand, after an asymmetric AC field assists vortices, the VL becomes less mobile. These features indicate that ME in these samples cannot be ascribed to an equilibration process, but probably are related to the organization of the lattice after nearest neighbor re-accommodation or induced plastic VL deformation. Recently, we have shown evidence that in YBCO the PE is a dynamic anomaly observed in the non-linear response, and is absent in the Labusch constant derived from the linear Campbell regime. However, this behavior seems not to be extensive to other systems as the traditional LTS NbSe2. In this work, the AC response in the PE region of NbSe2 and YBCO samples are presented and compared. Very salient differences both in the linear and non-linear response as well as in the ME characteristics indicate that a different physics governs the PE phenomena in each case. © 2007 Elsevier B.V. All rights reserved. Fil:Pasquini, G. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Bekeris, V. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_09214526_v398_n2_p420_Pasquini
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic High and low Tc superconductors vortex lattice
Memory effects
Peak effect
Vortex lattice
Labusch constant
Memory effects
Peak effect
Vortex lattice
Critical current density (superconductivity)
Crystal lattices
Nonlinear analysis
Superconducting materials
spellingShingle High and low Tc superconductors vortex lattice
Memory effects
Peak effect
Vortex lattice
Labusch constant
Memory effects
Peak effect
Vortex lattice
Critical current density (superconductivity)
Crystal lattices
Nonlinear analysis
Superconducting materials
Pasquini, G.
Luna, D.
Eismann, B.
Bettachini, V.
Bekeris, V.
Memory effects and peak effect in type II superconductors
topic_facet High and low Tc superconductors vortex lattice
Memory effects
Peak effect
Vortex lattice
Labusch constant
Memory effects
Peak effect
Vortex lattice
Critical current density (superconductivity)
Crystal lattices
Nonlinear analysis
Superconducting materials
description A large amount of experimental and theoretical work has been devoted to understand memory effects (ME) in the solid vortex lattice (VL) but has remained, however, controversial until now. In the vicinity of the anomaly known as the peak effect (PE) both the VL mobility and the measured critical current density are found to be dependent of the dynamical history of the sample, in both low Tc (LTS) and high Tc (HTS) superconductors. Experiments in YBa2Cu3O7 (YBCO) crystals have shown that the mobility of the VL increases after assisting the system with a symmetric AC field (or current) of moderated amplitude. On the other hand, after an asymmetric AC field assists vortices, the VL becomes less mobile. These features indicate that ME in these samples cannot be ascribed to an equilibration process, but probably are related to the organization of the lattice after nearest neighbor re-accommodation or induced plastic VL deformation. Recently, we have shown evidence that in YBCO the PE is a dynamic anomaly observed in the non-linear response, and is absent in the Labusch constant derived from the linear Campbell regime. However, this behavior seems not to be extensive to other systems as the traditional LTS NbSe2. In this work, the AC response in the PE region of NbSe2 and YBCO samples are presented and compared. Very salient differences both in the linear and non-linear response as well as in the ME characteristics indicate that a different physics governs the PE phenomena in each case. © 2007 Elsevier B.V. All rights reserved.
format JOUR
author Pasquini, G.
Luna, D.
Eismann, B.
Bettachini, V.
Bekeris, V.
author_facet Pasquini, G.
Luna, D.
Eismann, B.
Bettachini, V.
Bekeris, V.
author_sort Pasquini, G.
title Memory effects and peak effect in type II superconductors
title_short Memory effects and peak effect in type II superconductors
title_full Memory effects and peak effect in type II superconductors
title_fullStr Memory effects and peak effect in type II superconductors
title_full_unstemmed Memory effects and peak effect in type II superconductors
title_sort memory effects and peak effect in type ii superconductors
url http://hdl.handle.net/20.500.12110/paper_09214526_v398_n2_p420_Pasquini
work_keys_str_mv AT pasquinig memoryeffectsandpeakeffectintypeiisuperconductors
AT lunad memoryeffectsandpeakeffectintypeiisuperconductors
AT eismannb memoryeffectsandpeakeffectintypeiisuperconductors
AT bettachiniv memoryeffectsandpeakeffectintypeiisuperconductors
AT bekerisv memoryeffectsandpeakeffectintypeiisuperconductors
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