Plastic vortex creep and dimensional crossovers in the highly anisotropic superconductor HgBa\(_2\)CuO\(_{4+x}\)

In type-II superconductors exposed to magnetic fields between upper and lower critical values, \(H_{c1}\) and \(H_{c2}\), penetrating magnetic flux forms a lattice of vortices whose motion can induce dissipation. Consequently, the magnetization \(M\) of superconductors is typically progressively wea...

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Bibliographic Details
Published inarXiv.org
Main Authors Cole, Haley M, Venuti, Michael B, Gorman, Brian, Bauer, Eric D, Chan, Mun K, Eley, Serena
Format Paper
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 16.12.2021
Subjects
Creep (materials)
Crossovers
Crystal lattices
Cuprates
Fluid flow
Magnetic fields
Magnetic flux
Magnetic properties
Magnetism
Magnetization
Plastic flow
Superconductors
Temperature dependence
Vortices
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Summary:In type-II superconductors exposed to magnetic fields between upper and lower critical values, \(H_{c1}\) and \(H_{c2}\), penetrating magnetic flux forms a lattice of vortices whose motion can induce dissipation. Consequently, the magnetization \(M\) of superconductors is typically progressively weakened with increasing magnetic field \(B \propto n_v\) (for vortex density \(n_v\)). However, some materials exhibit a non-monotonic \(M(B)\), presenting a maximum in \(M\) at what is known as the second magnetization peak. This phenomenon appears in most classes of superconductors, including low \(T_c\) materials, iron-based, and cuprates, complicating pinpointing its origin and garnering intense interest. Here, we report on vortex dynamics in optimally doped and overdoped HgBa\(_2\)CuO\(_{4+x}\) crystals, with a focus on a regime in which plastic deformations of the vortex lattice govern magnetic properties. Specifically, we find that both crystals exhibit conspicuous second magnetization peaks and, from measurements of the field- and temperature- dependent vortex creep rates, identify and characterize phase boundaries between elastic and plastic vortex dynamics, as well as multiple previously unreported transitions within the plastic flow regime. We find that the second magnetization peak coincides with the elastic-to-plastic crossover for a very small range of high fields, and a sharp crossover within the plastic flow regime for a wider range of lower fields. We find evidence that this transition in the plastic flow regime is due to a dimensional crossover, specifically a transition from 3D to 2D plastic dynamics.
ISSN:2331-8422