Numéro |
J. Phys. I France
Volume 6, Numéro 12, December 1996
|
|
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Page(s) | 1597 - 1608 | |
DOI | https://doi.org/10.1051/jp1:1996177 |
J. Phys. I France 6 (1996) 1597-1608
The Fermi Surfaces of
-(BEDT-TTF)
X
J. Wosnitza1, G. Goll1, 2, D. Beckmann1, S. Wanka1, D. Schweitzer3 and W. Strunz4
1 Physikalisches Institut, Universität Karlsruhe, 76128 Karlsruhe, Germany
2 Grenoble High Magnetic Field Laboratory, Max-Planck-Institut für Festkörperforschung and Centre National de la Recherche Scientifique, BP 166, 38042 Grenoble, France
3 Physikalisches Institut, Universität Stuttgart, 70550 Stuttgart, Germany
4 Anorganisch-chemisches Institut, Universität Heidelberg, 69120 Heidelberg, Germany
(Received 24 april 1996, received in final form 27 June 1996, accepted 1 July 1996)
Abstract
We present de Haas-van Alphen (dHvA) measurements of the isostructural quasi two-dimensional (quasi-2D) organic superconductors
-(BEDT-TTF)
2IBr
2 and
-(BEDT-TTF)
2I
3 with superconducting transition temperatures of
K and
7 K, respectively. For both salts almost the same dHvA frequency and a beating behavior of the dHvA signal are found which
reflect the similarity of the Fermi surface (FS) topology in both materials. The FS can be well described by a slightly corrugated
quasi-2D cylinder. the corresponding overlap integral
between the highly conducting organic layers could be determined with high precision
is larger for
-(BEDT-TTF)
2I
3 although this salt has the larger interlayer distance. The effective cyclotron masses are very similar in both materials
. On the other hand the observed spin-splitting zeros suggest a rather large difference and large absolute values of the conduction
electron
g-factor which seems to reflect the importance of electron-electron interactions in the
-phase salts.
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