TY - JOUR

T1 - Spin-density-wave transition of (formula presented) at high magnetic fields

AU - Matsunaga, N.

AU - Yamashita, K.

AU - Kotani, H.

AU - Nomura, K.

AU - Sasaki, T.

AU - Hanajiri, T.

AU - Yamada, J.

AU - Nakatsuji, S.

AU - Anzai, H.

N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.

PY - 2001

Y1 - 2001

N2 - The transverse magnetoresistance of the Bechgaard salt (formula presented) has been measured for various pressures, with the field up to 24 T parallel to the lowest-conductivity direction (formula presented) A quadratic behavior is observed in the magnetic-field dependence of the spin-density-wave (SDW) transition temperature (formula presented) With increasing pressure, (formula presented) decreases and the coefficient of the quadratic term increases. These results are consistent with the prediction of the mean-field theory based on the nesting of the quasi-one-dimensional Fermi surface. Using a mean-field theory, (formula presented) for the perfect nesting case is estimated as about 16 K. This means that even at ambient pressure where (formula presented) is 12 K, the SDW phase of (formula presented) is substantially suppressed by the two dimensionality of the system.

AB - The transverse magnetoresistance of the Bechgaard salt (formula presented) has been measured for various pressures, with the field up to 24 T parallel to the lowest-conductivity direction (formula presented) A quadratic behavior is observed in the magnetic-field dependence of the spin-density-wave (SDW) transition temperature (formula presented) With increasing pressure, (formula presented) decreases and the coefficient of the quadratic term increases. These results are consistent with the prediction of the mean-field theory based on the nesting of the quasi-one-dimensional Fermi surface. Using a mean-field theory, (formula presented) for the perfect nesting case is estimated as about 16 K. This means that even at ambient pressure where (formula presented) is 12 K, the SDW phase of (formula presented) is substantially suppressed by the two dimensionality of the system.

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U2 - 10.1103/PhysRevB.64.052405

DO - 10.1103/PhysRevB.64.052405

M3 - Article

AN - SCOPUS:85038321312

VL - 64

JO - Physical Review B - Condensed Matter and Materials Physics

JF - Physical Review B - Condensed Matter and Materials Physics

SN - 0163-1829

IS - 5

ER -