A LOW-STORAGE FILTER DIAGONALIZATION METHOD FOR QUANTUM EIGENENERGY CALCULATION OR FOR SPECTRAL-ANALYSIS OF TIME SIGNALS

Citation
Va. Mandelshtam et Hs. Taylor, A LOW-STORAGE FILTER DIAGONALIZATION METHOD FOR QUANTUM EIGENENERGY CALCULATION OR FOR SPECTRAL-ANALYSIS OF TIME SIGNALS, The Journal of chemical physics, 106(12), 1997, pp. 5085-5090
Citations number
22
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
106
Issue
12
Year of publication
1997
Pages
5085 - 5090
Database
ISI
SICI code
0021-9606(1997)106:12<5085:ALFDMF>2.0.ZU;2-B
Abstract
A new version of the filter diagonalization method of diagonalizing la rge real symmetric Hamiltonian matrices is presented. Our previous ver sion would first produce a small set of adapted basis functions by app lying the Chebyshev polynomial expansion of the Green's function on a generic initial vector chi. The small Hamiltonian, H, and overlap, S, matrices would then be evaluated in this adapted basis and the corresp onding generalized eigenvalue problem would be solved yielding the des ired spectral information. Here in analogy to a recent work by Wall an d Neuhauser [J. Chem. Phys. 102, 8011 (1995)]H and S are computed dire ctly using only the Chebyshev coefficients c(n) = [chi/T-n((H) over ca p)/chi], calculation of which requires a minimal storage if the (H) ov er cap matrix is sparse. The expressions for H and S are analytically simple, computationally very inexpensive and stable. The method can be used to obtain all the eigenvalues of (H) over cap using the same seq uence {c(n)}. We present an application of the method to a realistic q uantum dynamics problem of calculating all bound state energies of H-3 (+) molecule. Since the sequence {c(n)} is the only input required to obtain all the eigenenergies, the present method can be reformulated f or the problem of spectral analysis of a real symmetric time signal de fined on an equidistant time grid. The numerical example considers a m odel signal C(t(n)) = Sigma(k)d(k) cos(t(n) omega(k)) generated by a s et of N = 100 000 frequencies and amplitudes, (omega(k),d(k)). It is d emonstrated that all the omega(k)'s and d(k)'s can be obtained to very high precision using the minimal information, i.e., 200 000 sampling points. (C) 1997 American Institute of Physics.