TY - JOUR
T1 - Superconducting transition in κ-(BEDT-TTF)2Cu[N(CN)2]Br under magnetic field
AU - Ito, Hiroshi
AU - Watanabe, Masashi
AU - Nogami, Yoshio
AU - Ishiguro, Takehiko
AU - Komatsu, Tokutaro
AU - Saito, Gunzi
AU - Hosoito, Nobuyoshi
N1 - Funding Information:
poorer than that for parallel case. As a cause of the noticiable discrepancy, we remined of the contribution from the vortex motion to the magneto-conductivity: for this salt flux melting has been claimed. 6 The details Of the fitting of the resistive transition data will be presented elsewhere. We thank Dr. R. Ikeda for handing refs. 1 and 2 prior to publication and useful discussion. This work was partly supported by the Grant-in-Aid for Scientific Research from Ministry of Education, Science and Culture, Japan.
PY - 1991/12/1
Y1 - 1991/12/1
N2 - Interlayer and intralayer coherence lengths of κ-(BEDT-TTF)2Cu[N(CN)2]Br are derived as ξb(0)=6±2 A ̊, ξac(0)=24±5 A ̊, respectively, by magnetic measurement. The renormalized theory of the order parameter fluctuation near the superconducting transition region was employed for the analysis. The broad resistive transitions under magnetic field are discussed on the same footing.
AB - Interlayer and intralayer coherence lengths of κ-(BEDT-TTF)2Cu[N(CN)2]Br are derived as ξb(0)=6±2 A ̊, ξac(0)=24±5 A ̊, respectively, by magnetic measurement. The renormalized theory of the order parameter fluctuation near the superconducting transition region was employed for the analysis. The broad resistive transitions under magnetic field are discussed on the same footing.
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U2 - 10.1016/0921-4534(91)91451-9
DO - 10.1016/0921-4534(91)91451-9
M3 - Article
AN - SCOPUS:0026383414
SN - 0921-4534
VL - 185-189
SP - 2659
EP - 2660
JO - Physica C: Superconductivity and its applications
JF - Physica C: Superconductivity and its applications
IS - PART 4
ER -