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Atomic orbitals tabulated

Based on equations (2-5) with initial data calculated with quantum-mechanical techniques [6-8], the values of P0-parameters of the majority of elements being tabulated constant values for each valence atom orbital were calculated. Mainly covalent radii were applied as a dimensional characteristic for calculating PE-parameter - by main type of chemical bond of interactions considered (table 1). For hydrogen atom also the value of Bohr radius and value of atomic ( metal ) radius were applied. [Pg.112]

B. Overlap Integrals.—The two atom overlap integrals (Sy s) between the various atomic orbitals were found in the tabulations available in the literature.39-48 The group overlap integrals (G j s) of interest in the M.O. calculation are related to the S s as... [Pg.236]

It is in the definition of the integrals or the lack of it, that most m.o. methods differ. The overlap integrals are easy to compute and were, indeed, tabulated for Slater-type atomic orbitals a long time ago (ref. 79). In some simple calculations, namely extended Huckel-type calculations a rough estimation of Hmn is as follows (see also page 79). [Pg.162]

There are a number of factors which contribute to the lack of consistency among current DFT programs. For example, many different basis representations of the KS orbitals are employed, including plane waves, Slater-type orbitals, numerically tabulated atomic orbitals, numerical functions generated from muffin-tin potentials, and delta functions. Gaussian basis functions, ubiquitous in the ab initio realm, were introduced into KS calculations in 1974 by Sambe and... [Pg.176]

Next, using the conventional atomic orbital basis as well as the K extra tt basis functions, one carries out an EOM calculation for the EA of the N2 molecule. In this calculation, one tabulates the energies of many (say M) of the EOM-EA eigenvalues. One then scales the orbital exponents uj of the K extra tt basis orbitals by a factor 17 Uj rjaj and repeats the calculation of the energies of the M lowest EOM eigenvalues. This scaling causes the extra tt basis orbitals to contract radially (if rj > 1) or to expand radially (if rj < 1). It is this basis orbital expansion and contraction that produces expansion and contraction of the box discussed above. That is, one does not employ a box directly instead, one varies the radial extent of the more diffuse basis orbitals to simulate the box variation. [Pg.458]

Neff is calculated from and for the orbital, using the tabulated moments for accurate Hartree-Fock atomic orbitals 22). These should not be confused with the effective values of the principal quantum number for overlap, which are determined from and . [Pg.5]

The values of / Q-parameter are tabulated constants for electrons of the given atom orbital. [Pg.136]

Using the HMO approximation, the ir-electron wave function is expressed as a linear combination of atomic orbitals (for the case in which the plane of the molecule coincides with the y-z plane of the coordinate axis), in much the same way as described previously for the generalized MO method. Minimizing the total -jT-electron energy of the molecule with respect to the coefficients (the variation method) leads to a series of equations from which the coefficients can be extracted by way of a secular determinant. The mathematical operations involved in solving the equations are not difficult. We will not describe them in detail, but will instead concentrate on the interpretation of the results of the calculations. For many systems, the Huckel MO energies and atomic coefficients have been tabulated." ... [Pg.28]

The formulas for the hydrogenlike ion solutions (in atomic units) of most interest in quantum chemistry are listed in Table 4-2. The tabulated functions are all in real, rather than complex, form. Problems involving atomic orbitals are generally far easier to solve in atomic units. [Pg.110]

Functions with higher / values and with sizes like those of lower-/ valence orbitals are also used to introduce additional angular correlation by pemiitting angularly polarized orbital pairs to be fomied. Optunal polarization functions for first- and second-row atoms have been tabulated and are included in the PNNL Gaussian orbital web site data base [45]. [Pg.2172]

Funetions with higher 1-values and with sizes more in line with those of the lower-1 orbitals are also used to introduee additional angular eorrelation into the ealeulation by permitting polarized orbital pairs (see Chapter 10) involving higher angular eorrelations to be formed. Optimal polarization funetions for first and seeond row atoms have been tabulated (B. Roos and P. Siegbahn, Theoret. Chim. Aeta (Berl.) 17, 199 (1970) M. J. Friseh, J. A. Pople, and J. S. Binkley, J. Chem. Phys., 3265 (1984)). [Pg.473]


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See also in sourсe #XX -- [ Pg.6 ]




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