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Potential functions evaluation

It follows from the above discussion and the relation (2.12) that one may call the energies B and A the bottom and the top, respectively, of the band. Similarly, the facts that the first moment of the canonical bands vanishes and that the potential function evaluated at D (C ) = - -l is zero lead us to call the centre of the band. Finally, we note that the energy V = B is the bottom of the s band. In the free-electron case all... [Pg.36]

In this chapter, we look at the techniques known as direct, or on-the-fly, molecular dynamics and their application to non-adiabatic processes in photochemistry. In contrast to standard techniques that require a predefined potential energy surface (PES) over which the nuclei move, the PES is provided here by explicit evaluation of the electronic wave function for the states of interest. This makes the method very general and powerful, particularly for the study of polyatomic systems where the calculation of a multidimensional potential function is an impossible task. For a recent review of standard non-adiabatic dynamics methods using analytical PES functions see [1]. [Pg.251]

With a given set of potential functions we can evaluate various average properties of the solvent. In particular, we would like to simulate experimentally observed macroscopic properties using microscopic solvent models. To do this we have to exploit the theory of statistical mechanics... [Pg.76]

With analytical potential functions we can try to evaluate the molecular equilibrium geometries and the vibrations around these configurations. This task can be accomplished in the simplest way using the Cartesian representation (Ref. l.)That is, the potential surface for a molecule with n atoms can be expanded formally around the equilibrium configuration r0 and give... [Pg.113]

Within the framework of the Bom-Oppenheimer approximation, a diatomic molecule consists of two nuclei that are more-or-less attached by the surrounding electron cloud. Often the specific form of the resulting potential function is not known. However, if a chemical bond is formed between the two nuclei, the potential function displays a minimum at a distance that corresponds to the equilibrium bond length. Furthermore, the energy necessary to break the chemical bond, the dissociation energy, is often evaluated by spectroscopic measurements. It can be concluded, then, that the potential fiinction has the general form shown in Fig. 6. A simple derivation of the Born- Qppenheimer approximation is presented in Section 12.1. [Pg.283]

Chapter 12. The forces which act on the atoms to maintain them in certain equilibrium positions are associated with changes in bond lengths and angles, and, furthermore in the present application, torsional angles around specific chemical bonds. Once a potential function has been established the so-called steric energy of the molecule can, in principle, be evaluated. [Pg.336]

The interatomic potential function for the diatomic molecule was described in Section 6 5. In the Taylpr-series development of this function (6-72)3 cubic and higher terms were neglected in the harmonic approximation. It is now of interest to evaluate the importance of these so-called anharmonic terms with the aid of the perturbation theory outlined above. If cubic and quartic... [Pg.362]

It was shown above that the cubic term in the potential function for the anharmonic oscillator cannot, for reasons of symmetry, contribute to a first-order perturbation. However, if the matrix elements of = ax3 are evaluated, it is found that this term results in a second-order correction to the... [Pg.363]

In the following we will present the explicit form of the potential functions and the parameterization of most of the force fields used in molecular mechanics calculations of amino, nitro and nitroso compounds and evaluate their performance according to these criteria. [Pg.4]

The potential function corresponding to this chain can be easily evaluated and is given by... [Pg.172]

Electron transfer was considered to occur at the intersection region S of the potential energy hypersurface and precursor (before electron transfer) and successor (after electron transfer) complexes, respectively. Both energy surfaces were evaluated using the potential function that was built up with an ab initio method. For each configuration, the parameter A = - Hpp was calculated. This parameter was used as... [Pg.99]


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See also in sourсe #XX -- [ Pg.3 , Pg.1755 ]




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