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Anisotropic thermopower of the organic superconductor κ-(BEDT-TTF)2Cu[N(CN)2]Br

R. C. Yu, J. M. Williams, H. H. Wang, J. E. Thompson, A. M. Kini, K. D. Carlson, J. Ren, M.-H. Whangbo, P. M. Chaikin

DOI 10.1103/PhysRevB.44.6932 · Physical Review B

T1

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Abstract

The thermopower of the organic superconductor κ-(BEDT-TTF)2Cu[N(CN)2]Br single crystals has been measured in two crystallographic directions a and c within the most conducting organic donor molecule plane. [Here BEDT-TTF represents bis(ethylenethio)-tetrathiafulvalene.] While the thermopower in the a direction is positive, the thermopower in the c direction is negative. The drastic anisotropy in thermopower reveals that the carriers in the a direction are holelike, whereas the carriers in the c direction are electronlike. A calculation based on the tight-binding electronic band structure is able to describe the temperature dependence of the anisotropic thermopower, but with a much reduced band dispersion.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
(BEDT-TTF)2Cu[N(CN)2]Br

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

11.6Pressure not reportedunknown
(BEDT-TTF)2Cu[N(CN)2]Br

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

11.4Pressure not reportedmidpoint
(BEDT-TTF)2Cu[N(CN)2]Br

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

10.7Pressure not reportedonset
(BEDT-TTF)2Cu(SCN)2

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10.4Pressure not reportedunknown
(BEDT-TTF)2Cu[N(CN)2]Cl

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

12.8Pressure not reportedunknown

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