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New Developments in Molecular Orbital Theory

New Developments in Molecular Orbital Theory. 20131006 김대겸. The use of molecular symmetry in the HF treatment of a closed-shell ground state. When a molecule has symmetry, group theory provides a powerful means of simplifying the problem of finding the exact electronic wave functions.

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New Developments in Molecular Orbital Theory

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  1. New Developments in Molecular Orbital Theory 20131006 김대겸

  2. The use of molecular symmetry in the HF treatment of a closed-shell ground state When a molecule has symmetry, group theory provides a powerful means of simplifying the problem of finding the exact electronic wave functions. It follows that the exact wave function(s) of a particular electronic state belong(s) to an irreducible representation of that symmetry group The wave functions of the various states can then be classified according to the symmetry species

  3. The use of molecular symmetry in the HF treatment of a closed-shell ground state we shall prove the following facts (1) The AP' built from Hartree-Pock MO's in the manner described in Sec. II is a singlet and is totally symmetrical; that is, it belongs to the identical representation of both the spin and symmetry groups. (2) The Hartree-Pock MO's used may be grouped in sets such that each set belongs to an irreducible representation of the symmetry group. (3) The Hartree-Fock MO's can always be chosen real.

  4. The use of molecular symmetry in the HF treatment of a closed-shell ground state we could obtain by changing spin functions one or several other AP's for which the energy would also reach its absolute minimum. r : radius vector of the point (x, y, s) R : the operator symbolizing the transformation If the operator R has an inverse

  5. The use of molecular symmetry in the HF treatment of a closed-shell ground state Let Φ(r) be the normalized AP‘ representing the closed-shell ground state, for all the space coordinates of the 2n electrons

  6. The use of molecular symmetry in the HF treatment of a closed-shell ground state We shall see presently that this representation has to be the identical representation, that is,

  7. The use of molecular symmetry in the HF treatment of a closed-shell ground state U : coefficient

  8. The use of molecular symmetry in the HF treatment of a closed-shell ground state

  9. The use of molecular symmetry in the HF treatment of a closed-shell ground state Matrix form

  10. The use of molecular symmetry in the HF treatment of a closed-shell ground state

  11. The use of molecular symmetry in the HF treatment of a closed-shell ground state Taking the complex conjugate and the inverse

  12. The use of molecular symmetry in the LCAO procedure we shall prove the following facts (1) The LCAO AP which minimizes the energy is necessarily a singlet and is totally symmetrical with respect to the symmetry group of the molecule. (2) The best LCAO MO's can be chosen so that they belong in sets to irreducible representations of the symmetry group of the molecule. (3) The best LCA0 MO's can all be chosen real.

  13. The use of molecular symmetry in the LCAO procedure

  14. The use of molecular symmetry in the LCAO procedure For NH3

  15. The use of molecular symmetry in the LCAO procedure For

  16. The use of molecular symmetry in the LCAO procedure

  17. The use of molecular symmetry in the LCAO procedure

  18. The use of molecular symmetry in the LCAO procedure In order to obtain the symmetry orbitals First, we pick the degenerate representations in a convenient manner, preferably in real form. Second, we construct then from each set of equivalent AO's a set of symmetry orbitals we can now define the corresponding matrix elements Mpq evaluated with the symmetry orbitals U is the matrix which forms the symmetry orbitals from the AO's

  19. The use of molecular symmetry in the LCAO procedure Irreducible representations or symmetry species of the symmetry group of the molecule be

  20. The use of molecular symmetry in the LCAO procedure Irreducible representations or symmetry species of the symmetry group of the molecule be

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