TY - JOUR
T1 - Temperature and field dependence of the anisotropy parameter for the high-temperature superconductor HgBa 2CuO 4+δ
AU - Xia, D. D.
AU - Yu, G.
AU - Zhao, X.
AU - Li, B.
AU - Liu, X.
AU - Ji, L.
AU - Chan, M. K.
AU - Greven, M.
PY - 2012/11
Y1 - 2012/11
N2 - We investigate the magnetization of HgBa 2CuO 4+δ below the superconducting transition temperature (T c) using angle-dependent torque magnetometry. The anisotropy of the superconducting parameter γ is analyzed with the Kogan model. For underdoped samples, we observe significant temperature and field dependences in the temperature range of about 5-10K below T c. For an overdoped sample, the field and temperature dependences of γ are less significant. Our data at all doping levels are consistent with the possibility that, at fixed magnetic field strength, γ approaches a constant value at low temperature. The strong temperature dependence in the range 5-10K below T c in the underdoped samples might arise from enhanced fluctuations due to the much larger anisotropy than in the overdoped case. At temperatures close to T c, γ is dramatically reduced due to the breakdown of the Kogan model as a result of critical fluctuations combined with the non-zero superconducting transition width of the samples.
AB - We investigate the magnetization of HgBa 2CuO 4+δ below the superconducting transition temperature (T c) using angle-dependent torque magnetometry. The anisotropy of the superconducting parameter γ is analyzed with the Kogan model. For underdoped samples, we observe significant temperature and field dependences in the temperature range of about 5-10K below T c. For an overdoped sample, the field and temperature dependences of γ are less significant. Our data at all doping levels are consistent with the possibility that, at fixed magnetic field strength, γ approaches a constant value at low temperature. The strong temperature dependence in the range 5-10K below T c in the underdoped samples might arise from enhanced fluctuations due to the much larger anisotropy than in the overdoped case. At temperatures close to T c, γ is dramatically reduced due to the breakdown of the Kogan model as a result of critical fluctuations combined with the non-zero superconducting transition width of the samples.
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U2 - 10.1088/0953-2048/25/11/115010
DO - 10.1088/0953-2048/25/11/115010
M3 - Article
AN - SCOPUS:84867314112
SN - 0953-2048
VL - 25
JO - Superconductor Science and Technology
JF - Superconductor Science and Technology
IS - 11
M1 - 115010
ER -