TY - JOUR
T1 - Phase-fluctuating superconductivity in overdoped La 2-x Sr x CuO 4
AU - Rourke, Patrick M.C.
AU - Mouzopoulou, Ioanna
AU - Xu, Xiaofeng
AU - Panagopoulos, Christos
AU - Wang, Yue
AU - Vignolle, Baptiste
AU - Proust, Cyril
AU - Kurganova, Evgenia V.
AU - Zeitler, Uli
AU - Tanabe, Yoichi
AU - Adachi, Tadashi
AU - Koike, Yoji
AU - Hussey, Nigel E.
PY - 2011/6
Y1 - 2011/6
N2 - 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.
AB - 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.
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U2 - 10.1038/nphys1945
DO - 10.1038/nphys1945
M3 - Article
AN - SCOPUS:79958015016
VL - 7
SP - 455
EP - 458
JO - Nature Physics
JF - Nature Physics
SN - 1745-2473
IS - 6
ER -