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Quantal Treatments

In this treatment, the Anderson-Newns Hamiltonian was utilized to determine the potential energy surface for both ion transfer, 21 - I2 and electron transfer, + e at a Pt electrode. Here the solvent part [Pg.99]

Note that the important system parameters such as the occupation probability interaction with polar solvent polarization ) strength of interaction of the reactant with the metal A, and the electronic energy of reactants are the functions of position x of the reactant from the electrode surface. These parameters are given below as a function of x. [Pg.100]

The occupation probability can be obtained from the self-consistency equation, [Pg.100]

The energy involves electronic energy s°, solvent interaction energy Ep, and the image interaction energy e, . The distance-dependent effective solvent dielectric constant k(x), which appears in the image term, was taken as [Pg.101]

Utilizing Eqs. (34) to (39) in Eq. (33), the potential energy surface for the iodide ion-iodine system as a function of distance x from the electrode and the normalized solvent coordinate qig was determined as given in Fig. 15 as a contour plot. It is observed that far from the electrode surface, the ionic and the atomic states are separated by an energy barrier [Pg.101]


In recent years, electrochemical charge transfer processes have received considerable theoretical attention at the quantum mechanical level. These quantal treatments are pivotal in understanding underlying processes of technological importance, such as electrode kinetics, electrocatalysis, corrosion, energy transduction, solar energy conversion, and electron transfer in biological systems. [Pg.71]

On the other hand. Fig. 1 demonstrates the power of classical collision theory. In view of the complexity of a complete quantal treatment of the stopping of a point charge in a many-electron target, or even a many-electron projectile in a many-electron target, utilizing the power of classical collision theory whereever justified, and knowing its limitations, is nothing less than a necessity from a practical point of view. [Pg.95]

Manson, J.R. and Ritchie, R.H. (1985). Completely quantal treatment of the van der Waals forces between atoms application to positronium. Phys. Rev. Lett. 54 785-788. [Pg.426]

The combination of quantum mechanical and classical modes is particularly important for larger systems which prohibit a complete quantal treatment. It is most suitable for direct processes with short interaction times and it is less applicable for long-lived intermediate complexes. The ultimate step in the hierarchy of time-dependent approximations is a complete classical treatment of all degrees of freedom. This is the topic of the next chapter. [Pg.90]

Secrest, D. (1979a). Rotational excitation I The quantal treatment, in Atom-Molecule Collision Theory, ed. R.B. Bernstein (Plenum Press, New York). [Pg.404]

It is the purpose of this review to discuss and illustrate the methods presently employed to obtain potential energy surfaces by approximate, but non-empirical solutions to Schrodinger s electronic equation. In addition to discussing the different levels of approximation employed in these ab initio calculations, we emphasize the type of chemical system (in terms of its electronic structure) to which each level of calculation may be expected to yield usable results, i.e. results with acceptable errors or with predictable bounds on the error. Our interest will be primarily in surfaces which have been determined for the prediction and understanding of chemical reactions. This will include a survey of those calculations which have concentrated on determining the reaction path, and the geometry and properties of the system at points on this path, as well as those in which an essentially complete surface has been determined. The latter type of calculation coupled with either classical or quantal treatments of the nuclear motion on such a surface provides a total theoretical prediction of a chemical reaction. This ultimate objective has been achieved in the case of the H + Ha exchange reaction. [Pg.4]

Although this semiclassical result seems to be very simple, still there is no generalization for the quantal treatment except for the linear model (vide infra). [Pg.327]

W. A. Lester, Jr., The N coupled-channel problem, Modern Theoretical Chemistry, Vol. I (W. H. Miller, ed.), Plenum Press, New York, 1976, p. 1 D. Secrest, Rotational excitation I The quantal treatment, in Atom-Molecule Collision Theory (R. B. Bernstein, ed.), Plenum Press, New York, 1979. [Pg.55]

R.E, Wyatt. Reactive scattering cross sections ii Approximate quantal treatments. In Atom-Moiecule Coliision Theory. A Guide for the Experimentalist, edited by R. B. Bernstein (Plenum. New York. 1979) pp. 477-503. [Pg.284]

A fundamental approach, now routinely employed in essentially all quantal treatments of molecular collisions (both inelastic and reactive), is to use rotating coordinate systems which are generalizations of those commonly used to describe rigid-body dynamics. Additionally, the most accurate and widely used quantal approximations for rotationally inelastic molecular collisions are those based on the so-called sudden assumption (essentially a time-scale criterion in which an internal degree of freedom is assumed to be slow compared to the time scale or suddenness of the collision). We give a brief summary of these ideas, focussing on Curtiss role both in his research and as a mentor. We conclude with a summary of subsequent developments which show the success of Curtiss research and mentoring. [Pg.123]

The limitations of this oicture are discussed by G. Kurizki and J.K. Mclver, in Phys. Rev. 32 4358 (1985), where a unified quantal treatment of all types of radiation from fast particles in crystals is presented. [Pg.345]

A quantal treatment of photoeffect at the semiconductor-solution interface can be obtained using the general expression of the photocurrent of the following form ... [Pg.65]

Several other approaches have been explored for collisions involving polyatomics. In particular we want to mention reviews emphasizing a quasiclassical treatment of energy transfer into polyatomics [41], a semiclassical coupled-channels approach for polyatomics [42,43], quantal treatments where slow (usually rotational) degrees of freedom are treated in a sudden-collision approximation [44], and approaches based on the solution of the time-dependent Schrodinger equation for scattering wave-packets [45-50], No attempt will however be made to review the extensive literature on molecular collisions. This has been periodically done in publications of reviews and workshop lectures [51-55]. [Pg.333]

R. E. Wyatt, Reactive scattering cross sections II Approximate quantal treatments, in reference 4, chapter 15. [Pg.303]

Fig. 5. Quantal treatments capable of incorporating both rearrangement and dissociation in energy transfer processes are just now appearing. A many-body approach should be advantageous in processes with large total energies, such as high collision energies or highly excited reactants. It is also applicable to collisions involving polyatomic molecules and solid surfaces. Fig. 5. Quantal treatments capable of incorporating both rearrangement and dissociation in energy transfer processes are just now appearing. A many-body approach should be advantageous in processes with large total energies, such as high collision energies or highly excited reactants. It is also applicable to collisions involving polyatomic molecules and solid surfaces.
D. Secrest, Rotational excitation Quantal treatment, in reference 2, p. 265. [Pg.698]


See other pages where Quantal Treatments is mentioned: [Pg.2051]    [Pg.2055]    [Pg.2159]    [Pg.318]    [Pg.94]    [Pg.99]    [Pg.150]    [Pg.6]    [Pg.54]    [Pg.189]    [Pg.114]    [Pg.108]    [Pg.16]    [Pg.47]    [Pg.2051]    [Pg.2055]    [Pg.2159]    [Pg.329]    [Pg.312]    [Pg.125]   


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