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Volumn 6, Issue 12, 1996, Pages 1527-1553

Electronic structure of the α-(BEDT-TTF)2MHg(XCN)4 (M = Tl, K, NH4; X = S, Se) and related phases. Synthesis and crystal structure of the new stable organic metal α-(BEDT-TTF)2TlHg(Se1-xSxCN)4 (x = 0.125)

Author keywords

[No Author keywords available]

Indexed keywords

BAND STRUCTURE; CHARGE CARRIERS; CRYSTAL STRUCTURE; ELECTRIC CONDUCTIVITY OF SOLIDS; ELECTRONIC STRUCTURE; FERMI SURFACE; MOLECULAR CRYSTALS; ORGANOMETALLICS; PHASE TRANSITIONS; SALTS; SYNTHESIS (CHEMICAL);

EID: 0030394640     PISSN: 11554304     EISSN: None     Source Type: Journal    
DOI: 10.1051/jp1:1996172     Document Type: Article
Times cited : (81)

References (50)
  • 39
    • 33748827274 scopus 로고    scopus 로고
    • 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
    • 33748822083 scopus 로고    scopus 로고
    • note
    • 2 in reference [14] is interchanged with respect to that used in reference [2] as well as in the present work.
  • 41
    • 33748828791 scopus 로고    scopus 로고
    • note
    • 4).
  • 42
    • 0022685399 scopus 로고
    • 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.
    • (1987) Synth. Met. , vol.19 , pp. 327
    • Ducasse, L.1    Abderrabba, M.2    Gallois, B.3    Chasseau, D.4
  • 45
    • 33748809964 scopus 로고    scopus 로고
    • note
    • 4).
  • 46
    • 33748839299 scopus 로고    scopus 로고
    • note
    • 2 increases the band gap by about 60%.
  • 49
    • 33748827275 scopus 로고    scopus 로고
    • note
    • 6.
  • 50
    • 0000689361 scopus 로고    scopus 로고
    • 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.
    • (1996) Phys. Rev. B , vol.53 , pp. 12725
    • Campos, C.S.1    Sandhu, P.S.2    Brooks, J.S.3    Ziman, T.4


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.