The angular and magnetic field dependence of a critical current parallel to the layers in the layered superconductors is studied. The critical current value is found for a superconductor with strong pinning centers. Quantum flux creep in sufficiently perfect layered high-To superconductors is discus
Pinning and creep in layered superconductors
โ Scribed by M.V. Feigel'man; V.B. Geshkenbein; A.I. Larkin
- Book ID
- 103942514
- Publisher
- Elsevier Science
- Year
- 1990
- Tongue
- English
- Weight
- 1010 KB
- Volume
- 167
- Category
- Article
- ISSN
- 0921-4534
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โฆ Synopsis
The thermal-and disorder-induced effects in the mixed state of a layered high-T, superconductor (in a field Hllc) are studied. The flux line lattice is of a quasi-2D type at sufftciently high field H2 Ho where H,, is proportional to the mass anisotropy m/M and estimated to be around 3 T for the Bi-and Tl-based superconductors. At H > H,, the FLL melts at a temperature T,,, close to the temperature of 2D dislocation-mediated melting. At T> T,,, the system is in the normal state. At low temperatures T< Ts= T,,,/ ln(H/H,) the system is in the vortex glass state with zero linear resistivity: aV/aj-0 as j-0. In the intermediate temperature range T,-c T< T,,, the energy barriers for the plastic motion ofvortices are finite and thermally activated flux flow (TAFF) occurs. In the vortex glass state, different regimes of flux pinning and creep are identified and the behaviour of the critical current j, as a function of temperature and magnetic field is estimated. Power-law behaviour of the effective pinning energy U(j) at ja: j, is obtained for the case of 2D collective creep.
๐ SIMILAR VOLUMES
We study a flux creep when the magnetic field is parallel to the layers (the Cu-O planes) and vortices move across them. The pinning of vortices results from their interaction with the layered structure of the superconductor. where Mis the effective mass and q is the wavevector along the z-axis, s