Angular dependent magnetotransport and electronic structure in quasione-dimensional organic conductor (TMTSF)2ClO4

Kaya Kobayashi; Toshihito Osada

doi:10.1016/S0379-6779(00)01095-X

Angular dependent magnetotransport and electronic structure in quasione-dimensional organic conductor (TMTSF)₂ClO₄

Kaya Kobayashi, Toshihito Osada

Research output: Contribution to journal › Article › peer-review

2 Citations (Scopus)

Abstract

Anisotropic magnetotransport in a quasi-one-dimensional (Q1D) organic conductor (TMTSF)₂ClO₄ are discussed relating to its electronic structure. (1) The Lebed resonance is semiclassically considered for general field orientations. The Danner-Chaikin oscillation is not an independent phenomenon, but it is regarded as the oscillation of Lebed resonance amplitude. (2) In (TMTSF)₂ClO₄, the Lebed resonance position reflects the anion ordering (AO) superlattice. Using this fact, the lower limit of AO gap is estimated. (3) The magnetoresistance angular effects under d.c. electric fields are numerically studied. The angular effect structures doubly split and shift under electric fields along the stacking axis. This effect can be explained by the fact that electrons on each Fermi sheet feel different effective magnetic fields.

Original language	English
Pages (from-to)	1029-1030
Number of pages	2
Journal	Synthetic Metals
Volume	120
Issue number	1-3
DOIs	https://doi.org/10.1016/S0379-6779(00)01095-X
Publication status	Published - Mar 15 2001
Externally published	Yes

Keywords

Magnetotransport
Organic conductors based on radical cation and/or anion salts

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics
Mechanics of Materials
Mechanical Engineering
Metals and Alloys
Materials Chemistry

Access to Document

10.1016/S0379-6779(00)01095-X

Cite this

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title = "Angular dependent magnetotransport and electronic structure in quasione-dimensional organic conductor (TMTSF)2ClO4",

abstract = "Anisotropic magnetotransport in a quasi-one-dimensional (Q1D) organic conductor (TMTSF)2ClO4 are discussed relating to its electronic structure. (1) The Lebed resonance is semiclassically considered for general field orientations. The Danner-Chaikin oscillation is not an independent phenomenon, but it is regarded as the oscillation of Lebed resonance amplitude. (2) In (TMTSF)2ClO4, the Lebed resonance position reflects the anion ordering (AO) superlattice. Using this fact, the lower limit of AO gap is estimated. (3) The magnetoresistance angular effects under d.c. electric fields are numerically studied. The angular effect structures doubly split and shift under electric fields along the stacking axis. This effect can be explained by the fact that electrons on each Fermi sheet feel different effective magnetic fields.",

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AU - Osada, Toshihito

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N2 - Anisotropic magnetotransport in a quasi-one-dimensional (Q1D) organic conductor (TMTSF)2ClO4 are discussed relating to its electronic structure. (1) The Lebed resonance is semiclassically considered for general field orientations. The Danner-Chaikin oscillation is not an independent phenomenon, but it is regarded as the oscillation of Lebed resonance amplitude. (2) In (TMTSF)2ClO4, the Lebed resonance position reflects the anion ordering (AO) superlattice. Using this fact, the lower limit of AO gap is estimated. (3) The magnetoresistance angular effects under d.c. electric fields are numerically studied. The angular effect structures doubly split and shift under electric fields along the stacking axis. This effect can be explained by the fact that electrons on each Fermi sheet feel different effective magnetic fields.

AB - Anisotropic magnetotransport in a quasi-one-dimensional (Q1D) organic conductor (TMTSF)2ClO4 are discussed relating to its electronic structure. (1) The Lebed resonance is semiclassically considered for general field orientations. The Danner-Chaikin oscillation is not an independent phenomenon, but it is regarded as the oscillation of Lebed resonance amplitude. (2) In (TMTSF)2ClO4, the Lebed resonance position reflects the anion ordering (AO) superlattice. Using this fact, the lower limit of AO gap is estimated. (3) The magnetoresistance angular effects under d.c. electric fields are numerically studied. The angular effect structures doubly split and shift under electric fields along the stacking axis. This effect can be explained by the fact that electrons on each Fermi sheet feel different effective magnetic fields.

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