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Molecular orbital theory tight-binding approximation

Electronic band structures were calculated for several polymeric chains structurally analogous to polyacetylene (-CH-CH) and carbyne (-CbC). Ihe present calculations use the Extended Huckel molecular orbital theory within the tight binding approximation, and values of the calculated band gaps E and band widths BW were used to assess the potential applic ilitf of these materials as electrical semiconductors. Substitution of F or Cl atoms for H atoms in polyacetylene tended to decrease both the E and BW values (relative to that for polyacetylene). Rotation about rhe backbone bonds in the chains away from the planar conformations led to sharp increases in E and decreases in BW. Substitution of -SiH or -Si(CH,) groups for H in polyacetylene invaribly led to an increase in E and a decrease in BW, as was generally the case for insertion of Y ... [Pg.600]

In Eq. (10.9), is the overlap energy and S the corresponding overlap between adsorbate and surface atomic orbitals. Approximate Eq. (10.9) applies when ad molecule orbitals are s-symmetric and the metal electrons are also described by s-atomic orbital. Equation (10.9) is a familiar expression within molecular orbital theory and is deduced from tight binding theory including overlap of the atomic orbitals as in extended Hiickel theory (Hoffmann) is used [9]. [Pg.289]

Sometimes the estimation of the electronic structures of polymer chains necessitates the inclusion of long-range interactions and intermolecular interactions in the chemical shift calculations. To do so, it is necessary to use a sophisticated theoretical method which can take account of the characteristics of polymers. In this context, the tight-binding molecular orbital(TB MO) theory from the field of solid state physics is used, in the same sense in which it is employed in the LCAO approximation in molecular quantum chemistry to describe the electronic structures of infinite polymers with a periodical structure -11,36). In a polymer chain with linearly bonded monomer units, the potential energy if an electron varies periodically along the chain. In such a system, the wave function vj/ (k) for electrons at a position r can be obtained from Bloch s theorem as follows(36,37) ... [Pg.35]


See other pages where Molecular orbital theory tight-binding approximation is mentioned: [Pg.30]    [Pg.10]    [Pg.70]    [Pg.287]    [Pg.440]    [Pg.18]    [Pg.100]    [Pg.370]    [Pg.25]    [Pg.283]    [Pg.525]    [Pg.2]    [Pg.231]    [Pg.218]    [Pg.5]    [Pg.84]    [Pg.109]    [Pg.288]    [Pg.133]    [Pg.1562]   
See also in sourсe #XX -- [ Pg.3 ]




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