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Evaluation of Matrix Elements

This converts the calculation of S to the evaluation of matrix elements together with linear algebra operations. Generalizations of this theory to multichaimel calculations exist and lead to a result of more or less tire same form. [Pg.989]

The results of this test of the TDB-FMS method are encouraging, and we expect the gain in efficiency to be more significant for larger molecules and/or longer time evolutions. Furthermore, as noted briefly before, the approximate evaluation of matrix elements of the Hamiltonian may be improved if we can further exploit the temporal nonlocality of the Schrodinger equation. [Pg.498]

While Eq. (3.30) is valid for any resonance, as a practical point only lower-order resonances are typically important. The reason is that the Fourier coefficients Vm [cf. Eq. (3.29)] are expected to decline rapidly once the oscillations of exp(-/m 0) are more rapid than those of 1/(1,0). This result is very familiar in the semiclassical evaluation of matrix elements, where to zeroth order the decline is exponential with Iml. [Pg.70]

For explicit evaluation of matrix elements it is necessary to expand the coupled basis of the previous two sections in terms of uncoupled states. The general theory is discussed in Appendix B. The expansion of the local-mode basis, which is that used in most calculations, is given by... [Pg.84]

The evaluation of matrix elements for exphcitly correlated Gaussians (46) and (49) can be done in a very elegant and relatively simple way using matrix differential calculus. A systematic description of this very powerful mathematical tool is given in the book by Magnus and Neudecker [105]. The use of matrix differential calculus allows one to obtain compact expressions for matrix elements in the matrix form, which is very suitable for numerical computations [116,118] and perhaps facilitates a new theoretical insight. The present section is written in the spirit of Refs. 116 and 118, following most of the notation conventions therein. Thus, the reader can look for information about some basic ideas presented in these references if needed. [Pg.401]

The evaluation of matrix elements of a given A -electron operator,... [Pg.307]

For the efficient evaluation of matrix elements, it is useful to have a representation of OMVME as a functional determinant. We consider subgroups and their cosets to obtain the desired form. [Pg.91]

Quantitative theories for the chemical shift and nuclear spin-spin interaction were developed by Ramsey (113) soon after the experimental discoveries of the effects. Unfortunately the complete treatments of these effects involve rather detailed knowledge of the electronic structures of molecules and require evaluation of matrix elements of the orbital angular momentum between ground and excited electronic states. These matrix elements depend sensitively on the behavior of the wave function near... [Pg.233]

To conclude this chapter, let us present the main formulas for sums of unit tensors, necessary for evaluation of matrix elements df the energy operator. They will be necessary in Part 5. The matrix element of any irreducible tensorial operator may be written as follows ... [Pg.46]

Of frequent interest is the need of evaluation of matrix elements for a tensor product of two irreducible tensor operators... [Pg.227]

Balint-Kurti and Karplus[28] implemented an earlier suggestion of Moffit[29] for the evaluation of matrix elements of the Hamiltonian by transforming the AOs to an orthogonalized set. If carried out correctly, this involves no approximations. The method was applied to ab initio and empirically corrected calculations of LiF, F2, and Fj. The transformation of the matrix elements to the orthogonalized form can be quite time consuming for large bases. [Pg.21]

In our own work on both diatomic and polyatomic molecules, we have found it valuable to have a summary of the most important results from irreducible spherical tensor algebra, particularly those relating to the evaluation of matrix elements in various angular momentum coupling schemes. We now provide a summary of those results detailed derivations are, of course, to be found in the main body of the text. [Pg.171]

The evaluation of matrix elements of the Breit interaction requires the calculation of even more difficult singular integrals, and this remained an unsolved problem until the recent development of new algorithms [70,71]. With these results in hand, it is now possible to include all the relativistic and QED terms as in the helium case. The resulting theoretical ionization energy for the ground state of 0.19814209(2) a.u. is larger than the experimental value by... [Pg.74]

In many-electron theories such as configuration interaction or coupled cluster theory, it is more convenient to deal with the -electron reference determinant, IOq), rather than the true vacuum state, I ). In the evaluation of matrix elements using Wick s theorem as described above, even the use of normal-ordered strings would be tremendously tedious if one had to include the complete set of operators required to generate ld>o) from the true vacuum (i.e., lOo) = aUjat I )). [Pg.60]

As a result of this simplification, the rules for the evaluation of matrix elements between APSG-type wave functions become similar to those between single determinants [126]. In particular, full density matrices as well as the energy formula can easily be evaluated. [Pg.74]

The composite potential translates to the form of eq (5) discussed in Section 2.2. The evaluation of matrix elements in terms of the... [Pg.90]

Appendix D Evaluation of matrix elements involving the dipole... [Pg.128]

The evaluation of matrix elements of the dipole moment operator in the full Cartesian basis makes use of the formulae given by Obara and Saika, [50, eqs (A22) - (A26)]. [Pg.130]


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