TY - JOUR
T1 - Role of spin-orbit coupling on the spin triplet pairing in Na xCoO2·yH2O II
T2 - Multiple phase diagram under the magnetic field
AU - Yanase, Youichi
AU - Mochizuki, Masahito
AU - Ogata, Masao
N1 - Copyright:
Copyright 2005 Elsevier B.V., All rights reserved.
PY - 2005/12
Y1 - 2005/12
N2 - The possibility of multiple phase diagram in the novel superconductor NaxCoO2·yH2O is analyzed on the basis of the multi-orbital Hubbard model including the atomic spin-orbit coupling. We have shown that the spin triplet pairing state is stable in this model. The p-wave (f-wave) state is stabilized when the Hund's rule coupling is large (small). In the precedent paper, we have determined the direction of d-vector at T = Tc and H = 0 within the linearized Dyson-Gorkov equation. In this paper, the pairing state below Tc and under the magnetic field is determined within the weak coupling approximation including the paramagnetic effect. We find that the p + f coexistent state is stabilized at low temperatures in a part of parameter range. We point out that the phase diagram in the H-T plane is quite different between the p-wave, f-wave and p + f -wave superconductivities. The characteristics of each phase are clarified by showing the magnetic susceptibility and specific heat. We discuss the comparison with experimental results and suggest some future experiments to detect the multiple phase transition.
AB - The possibility of multiple phase diagram in the novel superconductor NaxCoO2·yH2O is analyzed on the basis of the multi-orbital Hubbard model including the atomic spin-orbit coupling. We have shown that the spin triplet pairing state is stable in this model. The p-wave (f-wave) state is stabilized when the Hund's rule coupling is large (small). In the precedent paper, we have determined the direction of d-vector at T = Tc and H = 0 within the linearized Dyson-Gorkov equation. In this paper, the pairing state below Tc and under the magnetic field is determined within the weak coupling approximation including the paramagnetic effect. We find that the p + f coexistent state is stabilized at low temperatures in a part of parameter range. We point out that the phase diagram in the H-T plane is quite different between the p-wave, f-wave and p + f -wave superconductivities. The characteristics of each phase are clarified by showing the magnetic susceptibility and specific heat. We discuss the comparison with experimental results and suggest some future experiments to detect the multiple phase transition.
KW - Multi-orbital model
KW - Multiple phase diagram
KW - NaCoOHO
KW - Spin triplet superconductivity
KW - d-vector
UR - http://www.scopus.com/inward/record.url?scp=29244431668&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=29244431668&partnerID=8YFLogxK
U2 - 10.1143/JPSJ.74.3351
DO - 10.1143/JPSJ.74.3351
M3 - Article
AN - SCOPUS:29244431668
SN - 0031-9015
VL - 74
SP - 3351
EP - 3364
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 12
ER -