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Matrix diagonalization eigenvalues

A unitary transformation is then introduced whieh diagonalizes the FG matrix, yielding eigenvalues s, and eigenvectors q,. The kinetic energy operator is still diagonal in these eoordinates. [Pg.312]

In the column-problem we compute the matrix of generalized column-eigenvectors B and the diagonal matrix of eigenvalues from ... [Pg.186]

L is a diagonal matrix of eigenvalues % P is the modal matrix whose columns are the % corresponding eigenvectors % Check that the results are correct... [Pg.236]

The classification of critical points in one dimension is based on the curvature or second derivative of the function evaluated at the critical point. The concept of local curvature can be extended to more than one dimension by considering partial second derivatives. d2f/dqidqj, where qt and qj are x or y in two dimensions, or x, y, or z in three dimensions. These partial curvatures are dependent on the choice of the local axis system. There is a mathematical procedure called matrix diagonalization that enables us to extract local intrinsic curvatures independent of the axis system (Popelier 1999). These local intrinsic curvatures are called eigenvalues. In three dimensions we have three eigenvalues, conventionally ranked as A < A2 < A3. Each eigenvalue corresponds to an eigenvector, which yields the direction in which the curvature is measured. [Pg.149]

Given that a matrix diagonalization (Equation 3.A1.7) of the matrix Fm has been carried out with the matrix B to yield eigenvalues V investigate now what happens to the expressions for T and V when new coordinates and corresponding velocities, Qi and Qi, are introduced... [Pg.73]

The diagonal eigenvalue matrix corresponding to H is composed of the two roots,... [Pg.366]

The orthogonal matrix Q transforms the real symmetric metric matrix M to its diagonal matrix of eigenvalues e ... [Pg.365]

If the basis set used is finite and incomplete, solution of the secular equation yields approximate, rather than exact, eigenvalues. An example is the linear variation method note that (2.78) and (1.190) have the same form, except that (1.190) uses an incomplete basis set. An important application of the linear variation method is the Hartree-Fock-Roothaan secular equation (1.298) here, basis AOs centered on different nuclei are nonorthogonal. Ab initio and semiempirical SCF methods use matrix-diagonalization procedures to solve the Roothaan equations. [Pg.56]

This secular equation is a polynomial in A of degree equal to the order of the square matrix A. Note from Theorem 6 on determinants in Section 1.2 and (2.39) that for a diagonal matrix, the eigenvalues are equal to the diagonal elements. [Pg.300]

The eigenvalue problem for the simple cos y potential of Eq. (4) can be solved easily by matrix diagonalization using a basis of free-rotor wave functions. For practical purposes, however, it is also useful to have approximate analytical expressions for the channel potentials V,(r). The latter can be constructed by suitable interpolation between perturbed free-rotor and perturbed harmonic oscillator eigenvalues in the anisotropic potential for large and small distances r, respectively. Analogous to the weak-field limit of the Stark effect, for linear closed-shell dipoles at large r, one has [7]... [Pg.822]

In this regime, where the levels are discrete, it is possible to calculate the intensities of the transitions by matrix diagonalization, just as the energies are calculated. It is simply a matter of computing the eigenvectors of the Hamiltonian as well as its eigenvalues. For example, to calculate the intensities in the spectra shown in Fig. 8.12 we calculate the rcp amplitude in each of the Stark states and multiply it by the matrix element connecting the 3s state to the n p state,... [Pg.136]

QM grew out of studies of blackbody radiation and of the photoelectric effect. Besides QM, radioactivity and relativity contributed to the transition from classical to modem physics. The classical Rutherford nuclear atom, the Bohr atom, and the Schrodinger wave-mechanical atom are discussed. Hybridization, wavefunctions, Slater determinants and other basic concepts are explained. For obtaining eigenvectors and eigenvalues from the secular equations the elegant and simple matrix diagonalization method is explained and used. All the necessary mathematics is explained. [Pg.85]


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