Third angular effect of magnetoresistance and dimensionality of Q1D organic conductors

H. Yoshino; A. Oda; T. Sasaki; T. Hanajiri; J. Yamada; S. Nakatsuji; H. Anzai; Keizo Murata

doi:10.1016/S0379-6779(98)00948-5

Third angular effect of magnetoresistance and dimensionality of Q1D organic conductors

H. Yoshino, A. Oda, T. Sasaki, T. Hanajiri, J. Yamada, S. Nakatsuji, H. Anzai, Keizo Murata

IMR - Materials Property Division

Research output: Contribution to journal › Conference article › peer-review

2 Citations (Scopus)

Abstract

Magnetoresistance of (TMTSF)₂ClO₄ was investigated in the anion ordered state (R-state). The angular dependence of magnetoresistance was measured for I ∥ c^* and B ∥ ab up to 24 T at 0.5 K. The third angular effect of magnetoresistance of quasi-one-dimensional (Q1D) metal was observed as the hump of the magnetoresistance. Semiclassical calculation of the angular dependence of the magnetoresistance was carried out based on a model Q1D conductor with two pairs of Q1D Fermi surfaces as expected for (TMTSF)₂ClO₄ in the R-state.

Original language	English
Pages (from-to)	2251
Number of pages	1
Journal	Synthetic Metals
Volume	103
Issue number	1-3
DOIs	https://doi.org/10.1016/S0379-6779(98)00948-5
Publication status	Published - 1999 Jun 24
Event	Proceedings of the 1998 International Conference on Science and Technology of Synthetic Metals (ICSM-98) - Montpellier Duration: 1998 Jul 12 → 1998 Jul 18

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title = "Third angular effect of magnetoresistance and dimensionality of Q1D organic conductors",

abstract = "Magnetoresistance of (TMTSF)2ClO4 was investigated in the anion ordered state (R-state). The angular dependence of magnetoresistance was measured for I ∥ c* and B ∥ ab up to 24 T at 0.5 K. The third angular effect of magnetoresistance of quasi-one-dimensional (Q1D) metal was observed as the hump of the magnetoresistance. Semiclassical calculation of the angular dependence of the magnetoresistance was carried out based on a model Q1D conductor with two pairs of Q1D Fermi surfaces as expected for (TMTSF)2ClO4 in the R-state.",

author = "H. Yoshino and A. Oda and T. Sasaki and T. Hanajiri and J. Yamada and S. Nakatsuji and H. Anzai and Keizo Murata",

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T1 - Third angular effect of magnetoresistance and dimensionality of Q1D organic conductors

AU - Yoshino, H.

AU - Oda, A.

AU - Sasaki, T.

AU - Hanajiri, T.

AU - Yamada, J.

AU - Nakatsuji, S.

AU - Anzai, H.

AU - Murata, Keizo

PY - 1999/6/24

Y1 - 1999/6/24

N2 - Magnetoresistance of (TMTSF)2ClO4 was investigated in the anion ordered state (R-state). The angular dependence of magnetoresistance was measured for I ∥ c* and B ∥ ab up to 24 T at 0.5 K. The third angular effect of magnetoresistance of quasi-one-dimensional (Q1D) metal was observed as the hump of the magnetoresistance. Semiclassical calculation of the angular dependence of the magnetoresistance was carried out based on a model Q1D conductor with two pairs of Q1D Fermi surfaces as expected for (TMTSF)2ClO4 in the R-state.

AB - Magnetoresistance of (TMTSF)2ClO4 was investigated in the anion ordered state (R-state). The angular dependence of magnetoresistance was measured for I ∥ c* and B ∥ ab up to 24 T at 0.5 K. The third angular effect of magnetoresistance of quasi-one-dimensional (Q1D) metal was observed as the hump of the magnetoresistance. Semiclassical calculation of the angular dependence of the magnetoresistance was carried out based on a model Q1D conductor with two pairs of Q1D Fermi surfaces as expected for (TMTSF)2ClO4 in the R-state.

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DO - 10.1016/S0379-6779(98)00948-5

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JO - Synthetic Metals

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T2 - Proceedings of the 1998 International Conference on Science and Technology of Synthetic Metals (ICSM-98)

Y2 - 12 July 1998 through 18 July 1998

ER -

Third angular effect of magnetoresistance and dimensionality of Q1D organic conductors

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