TY - JOUR
T1 - Irreversibility line of the HgBa2CaCu2O6+δ high-temperature superconductors
AU - Huang, Z. J.
AU - Xue, Y. Y.
AU - Meng, R. L.
AU - Chu, C. W.
N1 - Copyright:
Copyright 2015 Elsevier B.V., All rights reserved.
PY - 1994
Y1 - 1994
N2 - Reversible and irreversible magnetizations (M) have been measured on a polycrystalline sample of HgBa2CaCu2O6+δ (Hg 1:2:1:2) before and after oxygenation. For the preoxygenated sample, the superconducting transition temperature (Tc) is ∼114 K with a transition width of ∼2 K. The irreversibility line (Hirr) is approximated by a power law Hirr∼(1-Tirr/Tc)n with n∼5/2 between 0.1 and 5.5 T. For the oxygenated sample, Tc is ∼120 K with a width ∼4 K and the n for Hirr is almost the same. The values of n, which are ∼3/2 for Y 1:2:3:, ∼5/2 for Hg 1:2:1:2, and ∼11/2 for the Bi and Tl families, seem to correlate well with the distance between adjacent CuO2 blocks. A scaling law M[1-(T/T*)2]F(H), is observed for reversible M up to a few degrees below Tc with a T*∼112 K before oxygenation. This suggests that Hg 1:2:1:2 is a quasi-two-dimensional system, where the effects of thermal fluctuations have been previously demonstrated.
AB - Reversible and irreversible magnetizations (M) have been measured on a polycrystalline sample of HgBa2CaCu2O6+δ (Hg 1:2:1:2) before and after oxygenation. For the preoxygenated sample, the superconducting transition temperature (Tc) is ∼114 K with a transition width of ∼2 K. The irreversibility line (Hirr) is approximated by a power law Hirr∼(1-Tirr/Tc)n with n∼5/2 between 0.1 and 5.5 T. For the oxygenated sample, Tc is ∼120 K with a width ∼4 K and the n for Hirr is almost the same. The values of n, which are ∼3/2 for Y 1:2:3:, ∼5/2 for Hg 1:2:1:2, and ∼11/2 for the Bi and Tl families, seem to correlate well with the distance between adjacent CuO2 blocks. A scaling law M[1-(T/T*)2]F(H), is observed for reversible M up to a few degrees below Tc with a T*∼112 K before oxygenation. This suggests that Hg 1:2:1:2 is a quasi-two-dimensional system, where the effects of thermal fluctuations have been previously demonstrated.
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U2 - 10.1103/PhysRevB.49.4218
DO - 10.1103/PhysRevB.49.4218
M3 - Article
AN - SCOPUS:35949006857
VL - 49
SP - 4218
EP - 4221
JO - Physical Review B
JF - Physical Review B
SN - 0163-1829
IS - 6
ER -