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Electronic coupling integral

We have assumed here that J can be treated as a constant. In some types of calculation, the explicit distance-dependence of the electron coupling integral must be taken into account. Little is yet known of the appropriate form of such a dependence. ... [Pg.311]

R. K. Riech, R. W. Mountain, W. H. McGonagle, C. M. Huang, J. C. Twichell, B. B. Kosicki, and E. D. Savoye, An integrated electronic shutter for back-illuminated charge-coupled devices, Proc. IEEE 91, 171-174(1991). [Pg.19]

As noted above, inherent in the expressions derived for et in the previous section is the assumption that the intemuclear separation between reactants, r, is fixed. In fact, kti has a dependence on r, ket = ket(r), arising from solvent trapping (equation 23), and a much stronger dependence on r through the electronic coupling integral V. [Pg.345]

More recently, Goldman has introduced two additional modifications to MCI. First, modified radial functions are introduced which are functions of r> and r[54]. In these variables, all multidimensional integrals reduce to simple, one-electron integrals a simplification even over Cl, where coupled two-electron integrals always appear. Secondly, modified angular functions are introduced which implicitly contain an infinite number of coupled harmon-ics[55]. Several examples of such angular functions are given, one of which has an obvious connection to the ECG basis ... [Pg.382]

To the lowest order, the electronic matrix elements in Eq. (8) are determined by the vibronic coupling integral [37, 38]... [Pg.65]

The Lippmann—Schwinger equations (6.73) are written formally in terms of a discrete notation i) for the complete set of target states, which includes the ionisation continuum. For a numerical solution it is necessary to have a finite set of coupled integral equations. We formulate the coupled-channels-optical equations that describe reactions in a channel subspace, called P space. This is projected from the chaimel space by an operator P that includes only a finite set of target states. The entrance channel 0ko) is included in P space. The method was first discussed by Feshbach (1962). Its application to the momentum-space formulation of electron—atom scattering was introduced by McCarthy and Stelbovics... [Pg.179]

SECM theory has been developed for lour mechanisms with homogeneous chemical reactions coupled with electron transfer, i.e., a first-order irreversible reaction (ErQ mechanism) (5), a second-order irreversible dimerization (ErC2i mechanism) (36), ECE and DISP1 reactions (38). [The solution obtained for a EqCr mechanism in terms of multidimensional integral equations (2) has not been utilized in any calculations.] While for ErC, and ErC2i mechanisms analytical approximations are available (39), only numerical solutions have been reported for more complicated ECE and DISP1 reactions (38). [Pg.170]

Direct observation of intermediates (or lack thereof) provides credence to any mechanistic assignment. Integrated rate expressions for the intermediates will generally be less convoluted than the products since they are further upstream in the kinetic cascade. However, it is often difficult to observe independent spectroscopic signatures for each of the four PCET states. This is partly a consequence of the inherent coupling between electronic states and protonic states in PCET systems. In addition, PCET systems have not incorporated design elements for independent spectroscopic signatures of the proton and the electron. [Pg.510]

Direct dynamics simulations, in which the methodology of classical trajectory simulations is coupled to electronic structure, have had and will continue to have an enormous impact on the use of computational chemistry to develop [111,112] the theory of unimolecular kinetics. In these simulations the derivatives of the potential, required for numerically integrating the classical trajectory, are obtained directly from electronic stmcture theory without the need for an analytic PES. Direct dynamics is particularly important for studying the unimolecular dynamics of molecules with many degrees of freedom, for which it is difficult to construct an accurate analytic PES. [Pg.415]

See also Electron Transport, P/O Ratio, Chemiosmotic Coupling, Integrity of Mitochondrial Membranes, Uncoupling ETS and Oxidative Phosphorylation, The FIFO Complex, Oxidation as a Metabolic Energy Source (from Chapter 12)... [Pg.342]


See other pages where Electronic coupling integral is mentioned: [Pg.3026]    [Pg.171]    [Pg.19]    [Pg.37]    [Pg.531]    [Pg.148]    [Pg.309]    [Pg.4]    [Pg.1051]    [Pg.358]    [Pg.147]    [Pg.516]    [Pg.31]    [Pg.175]    [Pg.94]    [Pg.174]    [Pg.303]    [Pg.378]    [Pg.96]    [Pg.101]    [Pg.611]    [Pg.2732]    [Pg.118]    [Pg.194]    [Pg.9]    [Pg.69]    [Pg.401]    [Pg.13]    [Pg.111]    [Pg.179]    [Pg.19]    [Pg.37]    [Pg.16]    [Pg.138]    [Pg.138]    [Pg.352]    [Pg.3026]    [Pg.587]   
See also in sourсe #XX -- [ Pg.311 , Pg.313 , Pg.315 ]




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