TY - JOUR
T1 - Nickel-based phosphide superconductor with infinite-layer structure, BaNi2P2
AU - Mine, Takashi
AU - Yanagi, Hiroshi
AU - Kamiya, Toshio
AU - Kamihara, Yoichi
AU - Hirano, Masahiro
AU - Hosono, Hideo
N1 - Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2008/7
Y1 - 2008/7
N2 - Analogous to cuprate high-Tc superconductors, a NiP-based compound system has several crystals in which the Ni-P layers have different stacking structures. Herein, the properties of BaNi2P2 are reported. BaNi2P2 has an infinite-layer structure, and shows a superconducting transition at ∼3 K. Moreover, it exhibits metallic conduction and Pauli paramagnetism in the temperature range of 4-300 K. Below 3 K, the resistivity sharply drops to zero, and the magnetic susceptibility becomes negative, while the volume fraction of the superconducting phase estimated from the diamagnetic susceptibility reaches ∼100 vol.% at 1.9 K. These observations substantiate that BaNi2P2 is a bulk superconductor.
AB - Analogous to cuprate high-Tc superconductors, a NiP-based compound system has several crystals in which the Ni-P layers have different stacking structures. Herein, the properties of BaNi2P2 are reported. BaNi2P2 has an infinite-layer structure, and shows a superconducting transition at ∼3 K. Moreover, it exhibits metallic conduction and Pauli paramagnetism in the temperature range of 4-300 K. Below 3 K, the resistivity sharply drops to zero, and the magnetic susceptibility becomes negative, while the volume fraction of the superconducting phase estimated from the diamagnetic susceptibility reaches ∼100 vol.% at 1.9 K. These observations substantiate that BaNi2P2 is a bulk superconductor.
KW - A. Superconductor
KW - D. Electronic transport
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U2 - 10.1016/j.ssc.2008.05.010
DO - 10.1016/j.ssc.2008.05.010
M3 - Article
AN - SCOPUS:46549084993
SN - 0038-1098
VL - 147
SP - 111
EP - 113
JO - Solid State Communications
JF - Solid State Communications
IS - 3-4
ER -