TY - JOUR
T1 - Variation of temperature-linear specific heat with doping in (La1-xSrx)2CuO4
AU - Kato, M.
AU - Maeno, Y.
AU - Fujita, T.
N1 - Funding Information:
The authors would like to thank Dr. P. Lederer and Dr. K. Kumagai for stimulating discussions and comments. They are also very grateful to Y. Inaba for her important technical assistance, and to Y. Aoki for his contribution in determining the phase diagram. This work is supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Science and Culture of Japan.
PY - 1988/3/1
Y1 - 1988/3/1
N2 - Low-temperature specific heat of (La1-xSrx)2CuO4 has been studied between 2 and 20 K by systematically varying the Sr concentration x, in order to clarify the origin of non-zero γ, the temperature-linear specific-heat coefficient, frequently observed in high-Tc superconducting oxides. Identical procedure is used to prepare samples for the specific-heat measurement and for the determination of the structural, magnetic and superconductive phase-transition temperatures as a function of x. The value of γ is nearly zero in the antiferromagnetic ordering region, but increase abruptly with x to about 4 mJ/K2 mol in the insulating, but not antiferromagnetic region. By increasing x further into the superconductive region, γ tends to be smaller: 1.6 mJ/K2mol for x = 0.075. We argue that the non-zero γ is not due to inhomogeneity of the samples, but due to electronic origin intrinsic to this system.
AB - Low-temperature specific heat of (La1-xSrx)2CuO4 has been studied between 2 and 20 K by systematically varying the Sr concentration x, in order to clarify the origin of non-zero γ, the temperature-linear specific-heat coefficient, frequently observed in high-Tc superconducting oxides. Identical procedure is used to prepare samples for the specific-heat measurement and for the determination of the structural, magnetic and superconductive phase-transition temperatures as a function of x. The value of γ is nearly zero in the antiferromagnetic ordering region, but increase abruptly with x to about 4 mJ/K2 mol in the insulating, but not antiferromagnetic region. By increasing x further into the superconductive region, γ tends to be smaller: 1.6 mJ/K2mol for x = 0.075. We argue that the non-zero γ is not due to inhomogeneity of the samples, but due to electronic origin intrinsic to this system.
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U2 - 10.1016/0921-4534(88)90080-9
DO - 10.1016/0921-4534(88)90080-9
M3 - Article
AN - SCOPUS:0039584407
SN - 0921-4534
VL - 152
SP - 116
EP - 120
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 1
ER -