TY - JOUR
T1 - Low-temperature vortex liquid in La 2-x Sr x CuO 4
AU - Li, Lu
AU - Checkelsky, J. G.
AU - Komiya, Seiki
AU - Ando, Yoichi
AU - Ong, N. P.
PY - 2007/5
Y1 - 2007/5
N2 - In copper oxide superconductors, the lightly doped (small dopant concentration, x) region is of major interest because superconductivity, antiferromagnetism and the pseudogap state come together near a critical doping value, x c . But the way in which superconductivity is destroyed as x is decreased at very low temperatures, T, is not clear. Does the pair condensate vanish abruptly at a critical value, x c ? Or is phase coherence of the condensate destroyed by spontaneous vortices-as is the case at elevated T (refs-8, 9, 10)? So far, magnetization data at low T are very sparse in this region of the phase diagram. Here, we report torque magnetometry measurements on La 2x Sr x CuO 4 , which show that, in zero magnetic field, quantum phase fluctuations destroy superconductivity at x c ≈ 0.055. The phase-disordered condensate survives to x=0.03. In finite field H, the vortex solid-to-liquid transition occurs at H lower than the depairing field, H c2 . The resulting phase diagram reveals the large fraction of the x-H plane occupied by the quantum vortex liquid.
AB - In copper oxide superconductors, the lightly doped (small dopant concentration, x) region is of major interest because superconductivity, antiferromagnetism and the pseudogap state come together near a critical doping value, x c . But the way in which superconductivity is destroyed as x is decreased at very low temperatures, T, is not clear. Does the pair condensate vanish abruptly at a critical value, x c ? Or is phase coherence of the condensate destroyed by spontaneous vortices-as is the case at elevated T (refs-8, 9, 10)? So far, magnetization data at low T are very sparse in this region of the phase diagram. Here, we report torque magnetometry measurements on La 2x Sr x CuO 4 , which show that, in zero magnetic field, quantum phase fluctuations destroy superconductivity at x c ≈ 0.055. The phase-disordered condensate survives to x=0.03. In finite field H, the vortex solid-to-liquid transition occurs at H lower than the depairing field, H c2 . The resulting phase diagram reveals the large fraction of the x-H plane occupied by the quantum vortex liquid.
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U2 - 10.1038/nphys563
DO - 10.1038/nphys563
M3 - Article
AN - SCOPUS:34247892179
SN - 1745-2473
VL - 3
SP - 311
EP - 314
JO - Nature Physics
JF - Nature Physics
IS - 5
ER -