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Journal Article

Pressure effect on the magnetic susceptibility of low dimensional organic conductors ∝, β- (BEDT-TTF)2I3 and (TMTSF)2X (X = ClO4, PF6, ReO4)

MPS-Authors
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Weger,  M.
Department of Molecular Physics, Max Planck Institute for Medical Research, Max Planck Society;

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Schweitzer,  D.
Department of Molecular Physics, Max Planck Institute for Medical Research, Max Planck Society;

/persons/resource/persons232300

Keller,  H.J.
Department of Molecular Physics, Max Planck Institute for Medical Research, Max Planck Society;

External Resource

https://www.sciencedirect.com/science/article/pii/0379677987903778/pdf?md5=7498a9220497f9590108d77b3c8452fb&pid=1-s2.0-0379677987903778-main.pdf
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https://doi.org/10.1016/0379-6779(87)90377-8
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Citation

Forro, L., Cooper, R., Rothaemel, B., Schilling, J., Weger, M., Schweitzer, D., et al. (1987). Pressure effect on the magnetic susceptibility of low dimensional organic conductors ∝, β- (BEDT-TTF)2I3 and (TMTSF)2X (X = ClO4, PF6, ReO4). Synthetic Metals, 19(1-3), 339-346. doi:10.1016/0379-6779(87)90377-8.


Cite as: https://hdl.handle.net/21.11116/0000-0008-1DEA-1
Abstract
The pressure dependence of the static susceptibility of the α and β phases of (BEDT-TTF)2I3 and of (TMTSF)2X for X = ClO4−, PF6−, ReO4− was measured using a Faraday balance up to a pressure of 10 kbar. The fractional pressure dependence δ 1nξs/δP is -2.0%/kbar and −3.3%/kbar for the α- and β-(BEDT-TTF)2I3 respectively and it is temperature independent. For (TMTSF)2X δ1nξs/δP is about −3.0%/kbar at room temperature and increases to −4.8%/kbar on cooling. Both the magnitude and temperature dependence of the fractional pressure dependence in those two families are in contrast with the behaviour in TTF-TCNQ, where the magnitude is −8.%/kbar and decreases with decreasing temperature.