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Chebyshev recursion relations

B. Iterative Calculation of (E - H) 1 Using Modified Chebyshev Recursion Relations... [Pg.284]

Here, both the expansion coefficients and the phase (j) are energy-dependent, and Ai7 is the so-called spectral range of the Hamiltonian, A/f = (iJmax iJmin) /2, where Tfmin and i7max are the minimum and maximum eigenvalues of the Hamiltonian in a finite basis representation. The Chebyshev vectors = Tj H)xo can be iteratively generated from the recursion relation, designed by Mandelshtam and Taylor [221],... [Pg.150]

These states obey the same recursion relation as the Chebyshev polynomials ... [Pg.86]

We note here in passing that Chebyshev propagation is related to several other recursive methods based on the Krylov subspace = span i//(, Hy/(, ...,H Wq) ... [Pg.220]


See other pages where Chebyshev recursion relations is mentioned: [Pg.6]    [Pg.151]    [Pg.277]    [Pg.278]    [Pg.284]    [Pg.293]    [Pg.6]    [Pg.151]    [Pg.277]    [Pg.278]    [Pg.284]    [Pg.293]    [Pg.305]    [Pg.308]    [Pg.309]    [Pg.21]    [Pg.326]    [Pg.572]    [Pg.64]   
See also in sourсe #XX -- [ Pg.277 , Pg.284 ]




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