Phase-fluctuating superconductivity in overdoped La 2-x Sr x CuO 4

被引:0
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作者
Rourke P.M.C. [1 ]
Mouzopoulou I. [1 ]
Xu X. [2 ,3 ]
Panagopoulos C. [2 ,4 ]
Wang Y. [5 ]
Vignolle B. [6 ]
Proust C. [6 ]
Kurganova E.V. [7 ]
Zeitler U. [7 ]
Tanabe Y. [8 ]
Adachi T. [8 ]
Koike Y. [8 ]
Hussey N.E. [1 ]
机构
[1] H. H. Wills Physics Laboratory, University of Bristol, Bristol, BS8 1TL, Tyndall Avenue
[2] Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University
[3] Department of Physics, Hangzhou Normal University
[4] Department of Physics, University of Crete and FORTH
[5] State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University
[6] Laboratoire National des Champs Magnetiques Intenses, CNRS INSA, UJF, UPS
[7] High Field Magnet Laboratory, Institute for Molecules and Materials, Radboud University Nijmegen, 6525 ED Nijmegen
[8] Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki, Aoba-ku, Sendai 980-8579
基金
英国工程与自然科学研究理事会;
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D O I
10.1038/nphys1945
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学科分类号
摘要
In underdoped cuprate superconductors, phase stiffness is low and long-range superconducting order is destroyed readily by thermally generated vortices (and anti-vortices), giving rise to a broad temperature regime above the zero-resistive state in which the superconducting phase is incoherent 1-4 . It has often been suggested that these vortex-like excitations are related to the normal-state pseudogap or some interaction between the pseudogap state and the superconducting state 5-10 . However, to elucidate the precise relationship between the pseudogap and superconductivity, it is important to establish whether this broad phase-fluctuation regime vanishes, along with the pseudogap 11 , in the slightly overdoped region of the phase diagram where the superfluid pair density and correlation energy are both maximal 12 . Here we show, by tracking the restoration of the normal-state magnetoresistance in overdoped La 2-x Sr x CuO 4 , that the phase-fluctuation regime remains broad across the entire superconducting composition range. The universal low phase stiffness is shown to be correlated with a low superfluid density 1 , a characteristic of both underdoped and overdoped cuprates 12-14 . The formation of the pseudogap, by inference, is therefore both independent of and distinct from superconductivity. © 2011 Macmillan Publishers Limited. All rights reserved.
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页码:455 / 458
页数:3
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