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Hartree-Fock-Roothaan crystal-orbital formalism

Hartree-Fock-Roothaan Crystal-Orbital Formalism [Pg.16]

Until now we have not specified matrices H(q) in equation (1.18). To do this we write the Hamiltonian of the whole polymer (in atomic units) as [Pg.16]

the operator is given by expression (1.36) and the Coulomb and exchange operators 7(p, h) and. (p, h) are defined, respectively, as [Pg.17]

It was seen above that if we take into account the translational symmetry of the system and introduce the Bom-von Karman periodic boundary conditions, our matrix equations (1.3) reduce to relationship (1.17). In the Hartree-Fock-Roothaan case the elements of the Fock matrices F(q) occurring in the expression [Pg.17]

The charge-bond-order matrix of a three-dimensional polymer can be introduced in the form [Pg.17]


Hartree-Fock-Roothaan Crystal-Orbital Formalism... [Pg.16]


See also in sourсe #XX -- [ Pg.16 ]




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Crystal orbital

Crystal orbitals, Hartree-Fock

Hartree-Fock crystal orbital

Hartree-Fock formalism

Hartree-Fock orbital

Orbitals Hartree-Fock

Roothaan

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