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Integrals multicenter

ADF uses a STO basis set along with STO fit functions to improve the efficiency of calculating multicenter integrals. It uses a fragment orbital approach. This is, in essence, a set of localized orbitals that have been symmetry-adapted. This approach is designed to make it possible to analyze molecular properties in terms of functional groups. Frozen core calculations can also be performed. [Pg.333]

The A q-SW technique does not suffer from this deficiency because the calculations do not involve multicenter integrals and converge rapidly to a final solution. Johnson (121) has noted that this method is suitable for solving geometric problems, and the high quality of the... [Pg.10]

The main obstacles to the solution of this problem lie in the formidable number of multicentered integrals which arise even with the use of a minimal basis set, and the difficulty involved in their evaluation. This is illustrated in Table 1, where the number of electron interaction integrals is computed for a minimal basis set calculation of various compounds. The total number of such bielectronic integrals can be computed by the following equation. [Pg.11]

G. S. Tschumper, Multicentered integrated QM QM methods for weakly bound clusters An efficient and accurate 2-body many-body treatment of hydrogen bonding and van der waals interactions, Chem. Phys. Lett., 427 (2006) 185-191. [Pg.536]

In brief, the CNDO (the acronym stands for complete neglect of differential overlap) approach is an all valence electron, self-consistent field calculation in which multicenter integrals have been neglected and some of the two electron integrals parameterized using atomic data. Slater type atomic orbitals are used as the basis 2s, 2px, 2p, 2p for carbon and oxygen. In these calculations two-electron in egrafs are approximated as... [Pg.34]

The QSM integrals treated in the LCAO framework lead to the computation of linear combinations of multicenter integrals. We will describe here how to explicit this kind of integrals when dealing with spinorbital functions, whose space part is made of GTO functions or linear combinations of a set of them. [Pg.309]

Weatherford CA, Jones HW (eds) (1982) International Conference on ETO Multicenter Integrals. Reidel, Dordrecht, Netherlands... [Pg.98]

Revised versions of the DFT codes developed at Yang s Lab are used. Multicenter integrations are evaluated using Becke s decomposition scheme [59]. Electrostatic potential is computed via Delley s method [60], A simple damping is used to achieve the convergence. All calculations are for fixed geometries only. The bond lengths used are C-H 1.06A C-C 1.36A OC 1.20A. [Pg.138]

C. Multicenter, Integral, Closed Shell, and Restricted Chemistry... [Pg.33]

The building blocks of the model (multicenter integrals) are nonobservables. [Pg.51]

I. Shavitt and M. Karplus, Multicenter Integrals in Molecular Quantum Mechanics, J. Chem. Phys. 36, 550-551 (1962). [Pg.11]

We will use a, P, y, and S for orbital exponents of functions centered at R, respectively. The reason why Gaussians simplify multicenter integrations is that the product of two Is Gaussians, each on different centers, is proportional to a Is Gaussian on a third center. Thus... [Pg.411]

Semi-empirical methods avoid the solution of multicenter integrals that describe elec-tron lectron interactions and instead fit these interactions to match exprerimental data [4,9.10] gjjjy discuss ab initio wavefrmction and DFT methods here as they are... [Pg.428]

The self-consistent field approximation, which was briefly introduced earlier, is used to reduce the A -electron problem into the solution of n-single-electron systems. It reduces a 3n variable problem into n single electron functions that depend on three variables each. The individual electron-electron repulsive interactions shown in Eq. (A4) are replaced by the the repulsive interactions between individual electrons and an electronic field described by the spatially dependent electron density, p(r). This avoids trying to solve the difficult multicenter integrals that describe electron-electron interactions. The only trouble is that the electron density depends upon how each electron interacts with it. At the same time, the electron interaction with the field depends upon the density. A solution to this dilemma is to iterate upon the density until it convergences. The electron density that is used as the input to calculate the electron-field interactions must be equivalent, to within some tolerance, to that which results from the convergence of the electronic structure calculation. This is termed the self-consistent field (SCF). [Pg.428]

This index is not, however, very convenient for the direct calculation of similarity index. This is due to the fact that the values of calculated using eq. (138) are not invariant with respect to the distance and the mutual position of the corresponding molecules. The origin of this noninvariance arises from the presence of generally multicenter integrals (139) in which the integration is performed over the orbitals centered on the molecules A and B... [Pg.115]

In order to eliminate this unconvenient feature various procedures were proposed of which the simplest is probably the topological approximation arising from the philosophy of the overlap determinant method with its assigning tables. Rewriting these tables in the alternative matrix form (140), the problem of the multicenter integrals can be substantially simplified. [Pg.115]

As we have seen, EHT is a nonself-consistent method but the self-consistency over charge and configuration is included in the MR approximation. The Ab-initio HE SCF method requires the self-consistent calculation of the density matrix (see Chap. 4). This feature of the HE approach is maintained in the semiempirical methods, based on the zero differential overlap (ZDO) approximation. This approximation is used to reduce the number of multicenter integrals appearing in HE LCAO calculations. [Pg.203]

The Slater-type orbitals were the first to be used in the molecular quantum chemistry semiempirical calculations. Unfortunately, such functions are not suitable for fast calculations of multicenter integrals in ab-initio calculations. Gaussian-type functions (GTFs) were introduced to remedy the difficulties. GTFs are used in basis sets in practically all modern codes for LCAO calculations of molecules. We know two exclusions... [Pg.284]


See other pages where Integrals multicenter is mentioned: [Pg.162]    [Pg.170]    [Pg.604]    [Pg.6]    [Pg.162]    [Pg.589]    [Pg.3]    [Pg.4]    [Pg.83]    [Pg.2731]    [Pg.2741]    [Pg.162]    [Pg.74]    [Pg.89]    [Pg.100]    [Pg.309]    [Pg.9]    [Pg.273]    [Pg.56]    [Pg.2730]    [Pg.2740]    [Pg.219]    [Pg.4]    [Pg.493]    [Pg.708]    [Pg.51]    [Pg.282]    [Pg.448]    [Pg.655]    [Pg.250]   
See also in sourсe #XX -- [ Pg.8 ]

See also in sourсe #XX -- [ Pg.442 , Pg.443 ]




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