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Valence effective Hamiltonian

The systems discussed in this chapter give some examples using different theoretical models for the interpretation of, primarily, UPS valence band data, both for pristine and doped systems as well as for the initial stages of interface formation between metals and conjugated systems. Among the various methods used in the examples are the following semiempirical Hartree-Fock methods such as the Modified Neglect of Diatomic Overlap (MNDO) [31, 32) and Austin Model 1 (AMI) [33] the non-empirical Valence Effective Hamiltonian (VEH) pseudopotential method [3, 34J and ab initio Hartree-Fock techniques. [Pg.74]

By adopting the no-pair approximation, a natural and straightforward extension of the nonrelativistic open-shell CC theory emerges. The multireference valence-universal Fock-space coupled-cluster approach is employed [25], which defines and calculates an effective Hamiltonian in a low-dimensional model (or P) space, with eigenvalues approximating some desirable eigenvalues of the physical Hamiltonian. The effective Hamiltonian has the form [26]... [Pg.164]

Molecular orbital calculations have been performed on compounds 19 and 20 . The calculated PM3 equilibrium geometric structures show that these compounds are severely distorted from planarity in accordance with X-ray structural analysis (see Section 8.I2.3.I). On the other hand, PM3 calculations performed on both neutral and oxidized/reduced compounds show that oxidation and reduction induce a clear gain of aromaticity. Predictions using the nonempirical valence effective Hamiltonian (VEH) method have shown that the electronic charge density in the highest occupied molecular orbital (HOMO) is localized on the benzodithiin 19 or benzoxathiin 20 rings. [Pg.860]

However, this is definitely the technique for future calculations involving a large number of metal atoms. Furthermore, the idea behind the pseudopotential method is also applied in other types of Hamiltonians described below, e.g., valence effective Hamiltonian and semi-empirical methods. [Pg.17]

Polymers treated with the valence effective Hamiltonian... [Pg.20]

Some of the theoretical models used vary in each of the studies reported. These models were discussed in chapter 2, and the results are presented in each individual case below. In some cases, however, a detailed interpretation of the experimental UPS spectra requires the support of calculated density-of-valence-states (DOVS) curves. For that purpose, the valence effective Hamiltonian (VEH) method, which has been shown to provide accurate distributions of valence states for polymers and molecules, is used12-14. Even though it cannot be used for metal-containing systems (since the VEH potentials are not defined for metal atoms), the VEH approach is nevertheless of interest to determine the nature of the electronic wavefunctions (molecular orbitals) associated with a given UPS feature in the pristine polymer. [Pg.89]

The measurements were carried out using polarized-light from synchrotron radiation. The angle-resolved UPS spectra were recorded for specific directions of photon incidence, photon polarization, and electron exit, chosen in order to resolve the momentum dependence of the 7t-electron energy bands which could be observed in this experiment. Details are available elsewhere63. The UPS results are analysed not only with the help of the valence effective Hamiltonian (VEH) method, but also with the help of new quantum-chemical calculations based upon the excitation model method64. The full VEH band structure is shown in Fig. 7.32. [Pg.127]

The increase of second-order hyperpolarizabilities upon backbone elongation has also been evaluated by quantum chemical means by the Bredas group [74]. With a valence effective Hamiltonian approach (VEH/SOS) the parameters in the sum-over-states expression are evaluated leading to the second-order hyperpolarizabilities yof the molecules. With the VEH/SOS approach the description of larger molecules is feasible, which means in the case of PTA molecules longer than the tetramer. [Pg.177]

Most calculations on CPs have used semiempirical methods. The Hiickel method yields useful results and many properties can be qualitatively understood [188,190], but numbers are not quite reliable. The valence effective Hamiltonian (VEH) method [191] has been applied successfully to CPs [187,192]. It uses atomic potentials parametrized on the results of ab initio HF-SCF calculations on small molecules, and not on experimental data in that sense, it is a purely theoretical method. [Pg.592]

We have employed the recently developed Valence Effective Hamiltonian technique (16) and MNDO calculations (22) to study the influence of strain in TKe sidegroups on the geometry of the backbone and the resulting polymer band structure, bandgap, and ionization potential. The molecule used in our simulation of strain... [Pg.144]

Shuai, Z., Bredas, J.L. Electronic structure and nonlinear optical properties of fullerenes C q and C70 A valence-effective-Hamiltonian study. Phys. Rev. B 46, 16135-16141 (1992)... [Pg.149]

Valence Effective Hamiltonian X-ray photoelectron spectroscopy X-Ray Diffraction... [Pg.656]

The electrochemical properties of conductive polymer systems are important with regard to understanding the electrochemical doping process and in applications of conductive polymers as battery electrodes. We have developed a computational method, based on the Valence Effective Hamiltonian technique, which is remarkably effective in the computation of oxidation and reduction potentials of a variety of conjugated polymers (polyacetylene, polyphenylene, polythiophene, polypyrrole) and their oligomers. [Pg.433]

The direct mapping of the electronic structure of the conjugated polymers is possible in photoelectron spectroscopy of thin films. The valence band, which is available from ultraviolet photoelectron spectroscopy, clearly shows shifts as well as a reduction of photoelectron peaks coming from the frontier k orbitals [31—33]. This is consistent with predictions from calculations using a Valence Effective Hamiltonian using a model of conformational twists separating every dimer on the chain. [Pg.787]


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See also in sourсe #XX -- [ Pg.211 ]




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