Symmetrically orthogonalized

Equation (13.20) corresponds to a symmetrical orthogonalization of the basis. The initial coordinate system, (the basis functions %) is non-orthogonal, but by multiplying with a matrix such as S the new coordinate system has orthogonal axes. 

Let us consider the simple case of the H atom and its variational approximation at the standard HF/3-21G level, for which we can follow a few of the steps in terms of corresponding density-matrix manipulations. After symmetrically orthogonalizing the two basis orbitals of the 3-21G set to obtain orthonormal basis functions A s and dA, we obtain the corresponding AO form of the density operator (i.e., the 2 x 2 matrix representation of y in the... 

To restore orthogonality, while preserving as far as possible the desirable features of hi and h2, we carry out Lowdin s symmetric orthogonalization procedure12... 

Results obtained from the alkali iodides on the isomer shift, the NMR chemical shift and its pressure dependence, and dynamic quadrupole coupling are compared. These results are discussed in terms of shielding by the 5p electrons and of Lbwdins technique of symmetrical orthogonalization which takes into account the distortion of the free ion functions by overlap. The recoilless fractions for all the alkali iodides are approximately constant at 80°K. Recent results include hybridization effects inferred from the isomer shifts of the iodates and the periodates, magnetic and electric quadrupole hyperfine splittings, and results obtained from molecular iodine and other iodine compounds. The properties of the 57.6-k.e.v. transition of 1 and the 27.7-k.e.v. transition of 1 are compared. 

In addition Kondo and Yamashita (22), and others (15,17,18) have used Lowdin s work by applying the symmetrical orthogonalization technique to the chemical shifts in the alkali halides. All of these results agree remarkably well with the experimental data. 

To calculate the isomer shift (11) the electron density is obtained easily using the symmetric orthogonalization technique ... 

With simple, symmetrical, orthogonal designs like the full factorial designs, when all of the experiments have been done exactly the same number of times, then the factor effects can be calculated using simple algebra. 

Chirgwin- Coulson Inverse- overlap Symmetric orthogon. EGSO ... 

Orthogonalize (using Lowdin (symmetric) orthogonalization) the following Is (core), 2s (valence), and 3s (Rydberg) STO s for the Li atom given ... 

A modified INDO model that is not entirely obsolete is the symmetric orthogonal-ized INDO (SINDOl) model of Jug and co-workers, first described in 1980 (Nanda and Jug 1980). The various conventions employed by SINDOl represent slightly different modifications to INDO theory than those adopted in the MINDO/3 model, but the more fundamental difference is the inclusion of d functions for atoms of the second row in the periodic table. Inclusion of such functions in the atomic valence basis set proves critical for handling hyper-valent molecules containing these atoms, and thus SINDO1 performs considerably better for phosphorus-containing compounds, for instance, than do otlier semiempirical models that lack d functions (Jug and Schulz 1988). 

To alleviate a number of these problems, Lowdin proposed that population analysis not be carried out until the AO basis functions tp were transformed into an orthonormal set of basis functions / using a symmetric orthogonalization scheme (Lowdin 1970 Cusachs and Politzer 1968)... 

SINDO symmetrically orthogonalized intermediate neglect of differential overlap... 

A normal matrix is one that commutes with its adjoint, AA = A A. Normal matrices include diagonal, real symmetric, orthogonal, unitary, Hermitian (self-adjoint), permutation, and pseudo-permutation matrices. 

Now, if the differential overlaps of the original AO basis are approximated by the formula eq. (2.28), it turns out that applying the Lowdin transformation S 2 to the set of the AOs makes the products i.e. the differential overlaps of the symmetrically orthogonal OAOs vanishing ... 

Symmetrically Orthogonalized INDO (Method) Minimum Basis Set of Slater-type Orbitals, each Represented by 3 Gaussian Orbitals... 

Firstly, the function (70) is invariant under a linear transformation of the m doubly occupied orbitals amongst themselves. A proof of this statement seems hardly necessary as, in the case m = N, equation (70) is equivalent to a Slater determinant, and this property of a determinant is well-known. The m orbitals m may therefore be orthogonalized amongst themselves by a linear transformation, without altering the total wavefunction. This, of course, may be done in several ways, by transforming to MOs for example, but perhaps the most convenient method is to employ the Lowdin symmetric orthogonalization method 73... 

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