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39
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33748827274
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note
-
Although the global topology of these Fermi surfaces is not strongly dependent on the computational aspects, fine details like the area or the warping of the 1D portion can depend. For instance the area does not only depend on the crystal structure but also on the radial extension of the Slater orbitals (see also Ref. [14]) as well as, even if to alesser extent, on the mesh of k-points used to sample the Brillouin zone. The calculated areas of our Fermi surfaces are smaller than those obtained from magnetoresistance experiments (i.e., 9-12% vs. 16% for the (S) salts). These values could have been easily adjusted to match the magnetoresistance results by slightly changing the Slater orbitals in our calculations. Nevertheless, since our interest is on the comparison between the different salts and for reasons which will become clear later, we preferred to use exactly the same Slater orbitals as in all other studies of BEDT-TTF charge transfer salts previously performed in our group.
-
-
-
-
40
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33748822083
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-
note
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2 in reference [14] is interchanged with respect to that used in reference [2] as well as in the present work.
-
-
-
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41
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33748828791
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note
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4).
-
-
-
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42
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0022685399
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Because of the similarity in the donor⋯donor interactions (i.e., transfer integrals) the Fermi surfaces of the K(S) and K(Se) will be artificially similar if different HOMO energies (i.e., site energies) for the I, II and III donors are not used in the model tight binding calculations. Although small differences in the HOMO levels usually do not lead to serious problems, one needs to be careful when the differences are not so small. This fact has already been recognized for a number of organic charge transfer salts. See for instance: Ducasse L., Abderrabba M., Gallois B. and Chasseau D., Synth. Met. 19 (1987) 327.
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43
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0028381774
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45
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33748809964
-
-
note
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4).
-
-
-
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46
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33748839299
-
-
note
-
2 increases the band gap by about 60%.
-
-
-
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47
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0042962574
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Endres H., Keller H.J., Swietlik R., Schweitzer D., Angermund K. and Krüger C., Z. Naturforsch. 41a (1986) 1319.
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Krüger, C.6
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49
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33748827275
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note
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6.
-
-
-
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50
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0000689361
-
-
4) salt under pressure has appeared: Campos C.S., Sandhu P.S., Brooks J.S. and Ziman T., Phys. Rev. B 53 (1996) 12725. Although the approaches in the two papers are slightly different, the main results concerning the effect of pressure on the area of the closed part of the Fermi surface are similar.
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Campos, C.S.1
Sandhu, P.S.2
Brooks, J.S.3
Ziman, T.4
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