Hall effect in the normal phase of the organic superconductor (TMTSF)2PF6

J. Moser; J.R. Cooper; D. Jerome; B. Alavi; S.E. Brown; K. Bechgaard

doi:10.1103/PhysRevLett.84.2674

Hall effect in the normal phase of the organic superconductor (TMTSF)₂PF₆

J. Moser
, J.R. Cooper
, D. Jerome
, B. Alavi
, S.E. Brown
, K. Bechgaard

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

Abstract

We report accurate Hall effect measurements performed in the normal phase of the quasi-one-dimensional organic conductor (TMTSF)(2)PF(6) at ambient pressure. The Hall coefficient is found to be strongly temperature dependent all the way from 300 K down to the spin density wave onset arising around 12 K. These new results emphasize the existence of a high temperature regime above 130 K where the Fermi liquid model is not satisfactory.

Original language	English
Journal	Physical Review Letters
Volume	84
Issue number	12
Pages (from-to)	2674-2677
ISSN	0031-9007
DOIs	https://doi.org/10.1103/PhysRevLett.84.2674
Publication status	Published - 2000

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abstract = "We report accurate Hall effect measurements performed in the normal phase of the quasi-one-dimensional organic conductor (TMTSF)(2)PF(6) at ambient pressure. The Hall coefficient is found to be strongly temperature dependent all the way from 300 K down to the spin density wave onset arising around 12 K. These new results emphasize the existence of a high temperature regime above 130 K where the Fermi liquid model is not satisfactory. ",

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AU - Alavi, B.

AU - Brown, S.E.

AU - Bechgaard, K.

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AB - We report accurate Hall effect measurements performed in the normal phase of the quasi-one-dimensional organic conductor (TMTSF)(2)PF(6) at ambient pressure. The Hall coefficient is found to be strongly temperature dependent all the way from 300 K down to the spin density wave onset arising around 12 K. These new results emphasize the existence of a high temperature regime above 130 K where the Fermi liquid model is not satisfactory.

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U2 - 10.1103/PhysRevLett.84.2674

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