TY - JOUR
T1 - Maki parameter and upper critical field of the heavy-fermion superconductor UBe13
AU - Shimizu, Yusei
AU - Ikeda, Yoichi
AU - Wakabayashi, Takumi
AU - Haga, Yoshinori
AU - Tenya, Kenichi
AU - Hidaka, Hiroyuki
AU - Yanagisawa, Tatsuya
AU - Amitsuka, Hiroshi
PY - 2011/9
Y1 - 2011/9
N2 - We have performed low-temperature specific-heat measurements in magnetic fields for a single crystal UBe13. It has been observed that our sample exhibits a superconducting transition at an intermediate temperature (Tc ∼ 0.81 K) between previously reported values for two variant samples called H type and L type. The specific heat C(T) of our sample shows a T3 behavior below ∼0.7 Tc, which is similar to the behavior of the H-type sample, suggesting the existence of point nodes in the superconducting gap function. We have obtained the upper-critical-field curves Hc2 for the (001), (111), and (110) crystal axes, which show no anisotropy at least down to the lowest measured temperature of 0.5 K. We have also derived the Maki parameter k2, and it has been revealed that the k2 steeply decreases isotropically upon cooling just below T c. Paramagnetic effects and the symmetry of Cooper pairing of UBe13 are discussed.
AB - We have performed low-temperature specific-heat measurements in magnetic fields for a single crystal UBe13. It has been observed that our sample exhibits a superconducting transition at an intermediate temperature (Tc ∼ 0.81 K) between previously reported values for two variant samples called H type and L type. The specific heat C(T) of our sample shows a T3 behavior below ∼0.7 Tc, which is similar to the behavior of the H-type sample, suggesting the existence of point nodes in the superconducting gap function. We have obtained the upper-critical-field curves Hc2 for the (001), (111), and (110) crystal axes, which show no anisotropy at least down to the lowest measured temperature of 0.5 K. We have also derived the Maki parameter k2, and it has been revealed that the k2 steeply decreases isotropically upon cooling just below T c. Paramagnetic effects and the symmetry of Cooper pairing of UBe13 are discussed.
KW - Heavy fermion
KW - Paramagnetic effect
KW - Unconventional superconductor
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U2 - 10.1143/JPSJ.80.093701
DO - 10.1143/JPSJ.80.093701
M3 - Article
AN - SCOPUS:80052420498
SN - 0031-9015
VL - 80
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 9
M1 - 093701
ER -