TY - JOUR
T1 - Single Crystal Growth and Superconductivity in La7Ni3 without Inversion Symmetry in the Crystal Structure
AU - Nakamura, Ai
AU - Honda, Fuminori
AU - Homma, Yoshiya
AU - Li, Dexin
AU - Nishimura, Kengo
AU - Kakihana, Masashi
AU - Hedo, Masato
AU - Nakama, Takao
AU - O'Nuki, Yoshichika
AU - Aoki, Dai
N1 - Funding Information:
This work was supported by JSPS KAKENHI Grant Numbers 25247055, 15K05156, 15H05884, 15H05882, and 16H04006 and start-up research costs from the Project to Promote Gender Equality and Support Female Researchers from Tohoku University.
PY - 2017/4/6
Y1 - 2017/4/6
N2 - We succeeded in growing single crystals of La7Ni3 with the non-centrosymmetric hexagonal structure by the Bridgman method, and measured the electrical resistivity and specific heat under magnetic fields. The superconducting transition temperature Tsc is 2.4 K. The electronic specific heat coefficient γ is 44 mJ/(K2-f.u.-mol). Correspondingly, the upper critical field Hc2(0) in superconductivity is large, Hc2 = 27 kOe. The electronic specific heat shows the jump at Tsc = 2.4 K, indicating the bulk superconductivity with ΔCe/γTc = 1.2, which is close to the weak coupling BCS value of 1.43. Although the temperature dependence of specific heat and some parameters of superconductivity are well explained by the conventional BCS model, the temperature dependence of Hc2 is not consistent with the simple BCS model.
AB - We succeeded in growing single crystals of La7Ni3 with the non-centrosymmetric hexagonal structure by the Bridgman method, and measured the electrical resistivity and specific heat under magnetic fields. The superconducting transition temperature Tsc is 2.4 K. The electronic specific heat coefficient γ is 44 mJ/(K2-f.u.-mol). Correspondingly, the upper critical field Hc2(0) in superconductivity is large, Hc2 = 27 kOe. The electronic specific heat shows the jump at Tsc = 2.4 K, indicating the bulk superconductivity with ΔCe/γTc = 1.2, which is close to the weak coupling BCS value of 1.43. Although the temperature dependence of specific heat and some parameters of superconductivity are well explained by the conventional BCS model, the temperature dependence of Hc2 is not consistent with the simple BCS model.
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U2 - 10.1088/1742-6596/807/5/052012
DO - 10.1088/1742-6596/807/5/052012
M3 - Conference article
AN - SCOPUS:85018302487
SN - 1742-6588
VL - 807
JO - Journal of Physics: Conference Series
JF - Journal of Physics: Conference Series
IS - 5
M1 - 052012
T2 - 18th International Conference on Strongly Correlated Electron Systems, SCES 2016
Y2 - 9 May 2016 through 13 May 2016
ER -