Mott transition in quasi-one-dimensional electron systems at quarter filling

被引:2
|
作者
Yonemitsu, K
机构
关键词
many-body and quasiparticle theories; metal-insulator phase transitions; magnetic phase transitions;
D O I
10.1016/S0379-6779(97)80379-7
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Renormalization-group equations are derived and numerically solved for one-dimensional, quarter-filled electron systems with a backward scattering, the Umklapp process, and couplings with 0, 2k(F), 4k(F) phonons. A charge gap opens when the Umklapp process becomes relevant through constructive interference with the coupling with 4k(F) phonons, though the Umklapp process itself is weak. Meanwhile, a spin gap opens when the coupling with 2k(F) phonons is strong enough. consider three-dimensionality by cutting off the logarithmic divergence in the Cooper or 2k(F) electron-hole channel. The former case may explain a qualitative difference between the resistivity of (DMe-DCNQI)(2)Ag and that of (DI-DCNQI)(2)Ag.
引用
收藏
页码:1635 / 1636
页数:2
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