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Hatree-Fock

If we understand FM or magnetic properties of quark matter more deeply, we must proceeds to a self-consistent approach, like Hartree-Fock theory, beyond the previous perturbative argument. In ref. [11] we have described how the axial-vector mean field (AV) and the tensor one appear as a consequence of the Fierz transformation within the relativistic mean-field theory for nuclear matter, which is one of the nonperturbative frameworks in many-body theories and corresponds to the Hatree-Fock approximation. We also demonstrated... [Pg.245]

Hatree-Fock Approximation and Single Electron Hamiltonian... [Pg.313]

Each vibrational mode was assigned to one of the six types of motion predicted by theoretical analysis (C=0, stretch, N-C stretch, N-Cl stretch, N-C-N bend, N-Cl bend, and C=0 bend). The vibrational frequencies of 1,3-dichloro-l,3-diazetidine-2,4-dione 45 were calculated at Hatree-Fock level, DFT (B3LYP) level, and MP-2 level of theory using a standard 6-311G basis set. For N-C stretching modes all operators except E have a trace of zero. [Pg.636]

Groups Hatree-Fock (B3LYP) MP2 Groups Hatree—Fock (B3LYP) MP2 Experimentals... [Pg.637]

One of the applications of the n-particle picture made below involves the generalization of the Hatree-Fock approximation to n-particle states. If one attempted to determine n-particle states directly from the equations, coupled with an antisymmetrization procedure with respect to particle indices, one would encounter precisely the same difficulty as noted above. Instead, the problem must be approached from a different perspective. [Pg.93]

However, there has still been problem in their calculation. In the molecular orbital calculation, the basis set is often expanded so as to include some excited atomic orbitals in order to achieve a high accuracy. For estimation of the peak intensity of the XPS spectrum, information of the ionization cross section for the atomic orbital employed for the basis function is required. By the use of Hatree-Fock-Slater model, the ionization cross sections for atomic sub-shell orbitals have been calculated by several authors . Although these data are very useful for evaluation of the XPS... [Pg.180]

In the case of the TA and DA molecules all stable conformers obtained from semiempirical methods have been examined at RHF/3-21G level. For TMDA, due to limited computer resources, we have had to limit the number of starting geometries and we have selected several conformers of the lowest energy. (Gawrohski et al., 1997) These structures have been examined at 3-21G basis set. After having obtained the results for the TA, DA and TMDA at RHF/3-21G level we have fully reoptimised the geometries with the use of the restricted Hatree-Fock method at another commonly used basis set 6-3IG. Finally we have performed calculations at MP2/6-31G //RHF/6-31G level of theory. [Pg.113]

Multiresolution Quantum Chemistry in Multiwavelet Bases Analytic Derivatives for Hatree-Fock and Density Functional Theory. [Pg.327]

Fig. 3.9 Correlation of the Frobenius distance of the LDM obtained with the best basis set cc-pvqz versus the total Hatree-Fock energy with datapoints calculated using basis sets of varying quality. The best quality calculations reside in the lower left side of each plot and the least accurate ones reside in the upper-right comer... Fig. 3.9 Correlation of the Frobenius distance of the LDM obtained with the best basis set cc-pvqz versus the total Hatree-Fock energy with datapoints calculated using basis sets of varying quality. The best quality calculations reside in the lower left side of each plot and the least accurate ones reside in the upper-right comer...
Permethylated and partially pentylated CF6 have been used as chiral selectors for gas chromatography (GC) [47]. The geometry of these chiral selectors was optimized using Hatree-Fock theory calculations at the 6-3Ig level. Computational... [Pg.89]

This is called the central field approximation or the Hatree-Fock model. [Pg.211]

All quantum chemical calculations are based on the self-consistent field (SCF) method of Hatree and Fock (1928-1930) and the MO theory of Hund, Lennard-Jones, and Mulliken (1927-1929). A method of obtaining SCF orbitals for closed shell systems was developed independently by Roothaan and Hall in 1951. In solving the so-called Roothan equations, ab initio calculations, in contrast to semiempirical treatments, do not use experimental data other than the values of the fundamental physical constants. [Pg.34]


See other pages where Hatree-Fock is mentioned: [Pg.47]    [Pg.309]    [Pg.309]    [Pg.403]    [Pg.187]    [Pg.263]    [Pg.1276]    [Pg.536]    [Pg.47]    [Pg.309]    [Pg.309]    [Pg.403]    [Pg.187]    [Pg.263]    [Pg.1276]    [Pg.536]   


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