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Element, Fock matrix

In full analogy with the formula (8.53), we can express the Fock matrix elements by using the bond order matrix P for the crystal  [Pg.472]

Now let us do the same for all the occupied COs and sum the results. On the left-hand side we sum just 1, therefore we obtain the number of doubly oecupied COs, i.e. o(2N +1), because denotes [Pg.472]

The first term on the right-hand side of (9.65) represents me kmetic energy matrix element [Pg.473]

Electronic Motion in the Mean Field Periodic Systems [Pg.474]


If Lhc live iiul c pun lien i oiic-ceiiicr iwo-cIccLroii integrals are expressed by symbols such as Gss, Gsp, defiiietJ above, then the Fock matrix element contributions from the one-center two-elec-iron in icgrals are ... [Pg.291]

By replacing the superscripts a and (i by Pand tx, respectively, in th e above th ree eq u ation s. you can easily get three similar equations for the Fock matrix elements for beta orbitals. Similar expressions to the above for Fock matrix elements ol restricted Ilartree-Fock (RIIF) calculations can be generated by simply icplaeing 1- (or I P) by 1/2 P in the above equation s. [Pg.291]

The Fock matrix elements for a closed-shell system can be expanded as follows by substituting the expression for the Fock operator ... [Pg.77]

When the Coulomb and exchange operators are expressed in terms of the basis functions and the orbital expansion is substituted for xu then their contributions to the Fock matrix element take the following form ... [Pg.78]

In ub initio calculations all elements of the Fock matrix are calculated using Equation (2.226), ii re peifive of whether the basis functions ip, cp, formally bonded. To discuss the semi-empirical melh ids it is useful to consider the Fock matrix elements in three groups (the diagonal... [Pg.107]

With these approximations the Fock matrix elements for CNDO become ... [Pg.111]

In a closed-shell system, P = P) = P and the Fock matrix elements can be obtained by making this substitution. If a basis set containing s, p orbitals is used, then many of the one-centre integrals nominally included in INDO are equal to zero, as are the core elements Specifically, only the following one-centre, two-electron integrals are non-zero (/x/x /x/x), (pit w) and (fti/lfM/). The elements of the Fock matrix that are affected can then be written a." Uxllow s ... [Pg.113]

Unlike the Hiickel and extended Hiickel methods, the semi-empirical approaches that explicitly treat electron-electron interactions give rise to Fock matrix element... [Pg.611]

The S matrix contains the overlap elements between basis functions, and the F matrix contains the Fock matrix elements. Each element contains two parts from the Fock operator (eq. (3.36)), integrals involving the one-electron operators, and a sum over... [Pg.65]

Level Shifting. This technique is perhaps best understood in the formulation of a rotation of the MOs which form the basis for the Fock operator. Section 3.6. At convergence the Fock matrix elements in the MO basis between occupied and virtual orbitals are zero. The iterative procedure involves mixing (making linear... [Pg.72]

The first and second derivatives of the energy with respect to the X variables ( 0) and "(O)) can be written in term of Fock matrix elements and two-electron integrals in the MO basis. For an RHF type wave function these are given as... [Pg.74]

Rewriting eq. (3.51) with semi-empirical labels gives the following expres.sion for a Fock matrix element, where a two-electron integral is abbreviated as (LLv a), (eq. (3.56)). [Pg.82]

The Huckel methods perform the parameterization on the Fock matrix elements (eqs. (3.50) and (3.51)), and not at the integral level as do NDDO/INDO/CNDO. This means that Huckel methods are non-iterative, they only require a single diagonalization of the Fock (Huckel) matrix. The Extended Huckel Theory (EHT) or Method (EHM), developed primarily by Hoffmann again only considers the valence electrons. It makes use of Koopmans theorem (eq. (3.46)) and assigns the diagonal elements in the F... [Pg.92]

The hKs matrix is analogous to the Fock matrix in wave mechanics, and the one-electron and Coulomb parts are identical to the corresponding Fock matrix elements. The exchange-correlation part, however, is given in terms of the electron density, and possibly also involves derivatives of the density (or orbitals, as in the BR functional, eq. (6.25)). [Pg.190]

At the HF level of theory, the operator corresponds to addition of an extra term to the Fock matrix elements (Section 3.5). [Pg.396]

In step 3, a criterion of convergence may be introduced to terminate the iterations. Two other points should be mentioned instead of taking the correct Singles-CI matrix, we may resort to a simpler one, omitting single bi-electronic integrals and using only Fock-matrix elements as ... [Pg.141]

Fock matrix elements are set to zero, the barrier essentially disappears. Six donor-acceptor interactions become most favorable in the lowest energy, staggered conformation of C2H6. Steric interactions play only a secondary role. [Pg.177]

Without detailing the derivation, the diagonal Fock matrix elements take the following form, in the CNDO model, for d> on atom A and [Pg.21]

Due to their spatial localization, it follows that the interaction eneigy of an occupied LMO with any distant virtual LMO will be zero, and so the computational problem becomes reduced to annihilating matrix elements connecting LMOs that are close in space. These LMOs can be easily identified from the molecular connectivity table given the requirement that any allowed LMO spans one or two atoms. The Fock matrix element, Fif takes the form ... [Pg.38]

The actual Fock-matrix elements between orthogonalized ctch and ctc H orbitals are too small to account for appreciable conformational energy differences in the actual geometry of ethane (as can be seen from the small numerical values of /fsteric in Fig. 3.57). [Pg.230]

It is inherently surprising that geminal interactions are typically weaker than vicinal interactions, because the former involve orbitals that are in closer spatial proximity. The reasons for this counterintuitive distance dependence can be seen by decomposing the geminal Fock-matrix element into individual atomic hybrid contributions. [Pg.264]

The geminal Fock-matrix element is therefore written in terms of four contributions,... [Pg.265]


See other pages where Element, Fock matrix is mentioned: [Pg.281]    [Pg.285]    [Pg.78]    [Pg.79]    [Pg.107]    [Pg.113]    [Pg.115]    [Pg.116]    [Pg.120]    [Pg.279]    [Pg.309]    [Pg.281]    [Pg.285]    [Pg.291]    [Pg.78]    [Pg.403]    [Pg.144]    [Pg.179]    [Pg.33]    [Pg.34]    [Pg.35]    [Pg.38]    [Pg.58]    [Pg.82]    [Pg.95]    [Pg.99]    [Pg.265]   
See also in sourсe #XX -- [ Pg.141 ]




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