Disordered Type-II Superconductors: A Universal Phase Diagram for Low-T Systems
arXiv:cond-mat/0007451 · doi:10.1016/S0921-4534(00)01767-6
Abstract
A universal phase diagram for weakly pinned low-T type-II superconductors is revisited and extended with new proposals. The low-temperature ``Bragg glass'' phase is argued to transform first into a disordered, glassy phase upon heating. This glassy phase, a continuation of the high-field equilibrium vortex glass phase, then melts at higher temperatures into a liquid. This proposal provides an explanation for the anomalies observed in the peak effect regime of 2H-NbSe and several other low-T materials which is independent of the microscopic mechanisms of superconductivity in these systems.
23 pages, 9 figures
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- Phase Behavior of Type-II Superconductors with Quenched Point Pinning Disorder: A Phenomenological Proposal
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- Driven Disordered Polymorphic Solids: Phases and Phase Transitions, Dynamical Coexistence and Peak Effect Anomalies
- Real-space vortex glass imaging and the vortex phase diagram of SnMo6S8
- Relaxation and Glassy Dynamics in Disordered Type-II Superconductors
- Exploring metastability via the third harmonic measurements in single crystals of - showing anomalous Peak effect
- Relaxation dynamics in type-II superconductors with point-like and correlated disorder
- Flux jumps, Second Magnetization Peak anomaly and the Peak Effect phenomenon in single crystals of and
- Melting and structure of the vortex solid in strongly anisotropic layered superconductors with random columnar pins
- Crossover from paramagnetic compressed flux regime to diamagnetic pinned vortex lattice in a single crystal of cubic Ca(3)Rh(4)Sn(13)
- Evolution in the split-peak structure across the Peak Effect region in single crystals of -NbSe
- Dual role of an ac driving force and the underlying two distinct order-disorder transitions in the vortex phase diagram of Ca3Ir4Sn13
- Vortex Phase Diagram of Layered Superconductor Cu0.03TaS2 for H || c
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