Coexistence of antiferromagnetism with superconductivity in CePt
In
; Microscopic phase diagram determined by
In NMR and NQR
CePt
In
における超伝導と反強磁性の共存;
In核-核磁気共鳴(NMR)法と核四重極共鳴(NQR)法によって決めた微視的相図
酒井 宏典
; 徳永 陽
; 神戸 振作
; Ronning, F.*; Bauer, E. D.*; Thompson, J. D.*
Sakai, Hironori; Tokunaga, Yo; Kambe, Shinsaku; Ronning, F.*; Bauer, E. D.*; Thompson, J. D.*
常圧で重い電子系反強磁性体であるCePt
In
(
=5.2K)の
In核-核磁気共鳴(NMR)及び核四重極共鳴(NQR)測定を圧力下において行った。Ce
電子の反強磁性状態は約2.4GPaのところで、局在的から遍歴的な性質を示すようになり、超伝導が観測されるようになる。さらに加圧すると、3.4GPaのところで、反強磁性秩序は完全に抑制され、NMR緩和率は超伝導転移温度において、通常よりも鋭く、一次転移的に減少を示した。
Single crystals of the heavy-fermion antiferromagnet CePt
In
with a N
el temperature (
) of 5.2 K at ambient pressure have been investigated by zero-field
In-nuclear magnetic/quadrupole resonance (NMR/NQR) measurements as a function of applied pressure. Within the antiferromagnetic state the character of Ce's
electron appears to change from localized to itinerant-like at
GPa, approximately the pressure where superconductivity first emerges. With increased pressure, the superconducting transition
reaches a maximum just at or slighty before antiferromagnetic order disappears, and not at the pressure
GPa where the steeply decreasing N
el boundary extrapolates to zero temperature. For
, the spin relaxation rate drops sharply by more than two orders of magnitude at
, suggestive of a first order transition.