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Eigenvalues orbitals-molecular

It is well known that the PES cannot be given analytically in quantum chemistry, but can be calculated point by point through iterative solution of matrix eigenvalue problems arising from the application of LCAO-MO SCF Cl (Linear Combination of Atomic Orbitals - Molecular Orbital Self-Consistent-Field Configuration Interaction) methods. If... [Pg.3]

HUCKEL MOLECULAR ORBITAL THEORY I EIGENVALUES by the matrix... [Pg.189]

Alternative procedure Mathcad. Follow the procedure above except that where QMOBAS is indicated, use Mathcad instead. Enter the Huckel molecular orbital matrix, modified by subtracting xl, with some letter name. For example, call the modified matrix A. Type the command eigenvals(A) = with the name of the modified HMO matrix in parentheses. Mathcad prints the eigenvalues. The command eigenvecs(A) yields the eigenvectors, which are useful in ordering the energy spectrum. [Pg.197]

The excess energies can be measured for a known by essentially a stopping potential method, giving a spechum. This spectrum is then matched with calculated orbital energies (eigenvalues) derived from molecular orbital calculations. [Pg.323]

The atomic orbital contributions for each atom in the molecule are given for each molecular orbital, numbered in order of increasing energy (the MO s energy is given in the row labeled EIGENVALUES preceding the orbital coefficients). The symmetry of the orbital and whether it is an occupied orbital or a virtual (unoccupied) orbital appears immediately under the orbital number. [Pg.18]

Where might these one-electron wavefunctions come from I explained the basic ideas of HF and HF-LCAO theory in Chapter 6 we could find the molecular orbitals as linear combinations of appropriate atomic orbitals by solving the HF eigenvalue problem... [Pg.123]

The equations may be simplified by choosing a unitary transformation (Chapter 13) which makes the matrix of Lagrange multipliers diagonal, i.e. Ay 0 and A This special set of molecular orbitals (f> ) are called canonical MOs, and they transform eq. (3.40) mto a set of pseudo-eigenvalue equations. [Pg.63]

In the unrestricted Hartree-Fock method, a single-determinant wave function is used with different molecular orbitals for a and jS spins, and the eigenvalue problem is solved with separate F and F matrices. With the zero differential overlap approximation, the F matrix elements (25) become... [Pg.337]

This looks like an eigenvalue equation, but is not, since instead of regenerating fa, a sum of functions 4>j is obtained. For the complete set of molecular orbitals the equation can be written in matrix notation as... [Pg.382]

These equations, derived from the Schrodinger equation of Quantum Mechanics, can be solved iteratively for matrices and jL, containing as elements the appropriately normalized molecular orbital (MO) coefficients and orbital energy eigenvalues of eq. [Pg.147]


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