Theory of magnetic field-induced charge-density-wave phases

JETP Letters

Volumn 78, Issue 3, 2003, Pages 138-142

  Lebed, A G ^a,b  

^a BOSTON COLLEGE   (United States)

^b LANDAU INSTITUTE FOR THEORETICAL PHYSICS   (Russian Federation)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0347228251     PISSN: 00213640     EISSN: None     Source Type: Journal    
DOI: 10.1134/1.1618879     Document Type: Article

References (29)

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22. 4, in addition to the Q1D sheets of the FS, also have Q2D parts of the FS. The influence of the Q2D electron orbits on the physical properties of the FICDW phases will be studied elsewere. As shown in [7], from a phenomenological point of view, the FICDW phase is mixed with the component of the FISDW state characterized by zero projection of the total spin on the magnetic field direction. Nevertheless, the CDW-FICDW scenario (see [8, 9, 12]) considered in this paper is based on the suggestion that the SDW instability is a secondary phenomenon comparable with the CDW one. In other words, we assume that a bare coupling constant for the CDW instability is significantly bigger than a bare coupling constant for the SDW instability (see for discussions in [8, 9, 12]).
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