Quantum Resistive Behaviors in the Vortex Liquid Regimes at Finite Temperatures

Details Quantum Resistive Behaviors in the Vortex Liquid Regimes at Finite Temperatures Quantum Resistive Behaviors in the Vortex Liquid Regimes at Finite Temperatures

2002-10-29

arxiv.org/abs/cond-mat/0210626v5

J.Phys.Soc.Jpn. 72, 2930 (2003)

Physics

Condensed Matter

Superconductivity

14 pages, 21 figures. To appear in J. Phys. Soc. Jpn. Vol.72, No.11 (Nov., 2003)

Scientific paper

10.1143/JPSJ.72.2930

Motivated by a {\it mean field-like} resistive behavior in magnetic fields commonly seen in various superconducting (SC) cuprates and organics with strong fluctuation, {\it quantum} SC fluctuation effects on resistive behaviors are reexamined by putting emphasis on their roles in the so-called {\it thermal} vortex liquid regime. By incorporating the quantum fluctuation and a vortex pinning effect in the GL fluctuation theory, it is found that the resistivity curve shows not a fan-shaped broadening but a sharp drop at a 3d vortex-glass transition point far below an apparent upper critical field H_{c2}^*(T) as a result of a quantm fluctuation enhanced by an adequately small condensation energy or by a strong field. Fittings to data of cuprate and organic superconductors are performed by including effects of SC pseudogap region. It is argued on the cuprate materials that, irrespective of the presence of fluctuations of competing non-SC orders, the in-plane coherence length of hole-doped cuprates decreases on approaching the underdoped limit and that the condensation energy density to be measured from the heat capacity data is maximum near the optimal doping. The case of disordered quasi 2d s-wave films showing the field-tuned superconductor-insulator transition (FSIT) behavior is also studied for comparison, and an agreement with available data is found.

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