“…The method is nonperturbative and based on the well known AI search procedure, developed and mainly applied for large scale calculations on highly excited vibrational states in polyatomic molecules [42][43][44][45][46][47]. The efficiency of our vibrational method is essentially based on the availability of a completely symmetrized, separable (in product form), unrestricted vibrational basis set |iae (Eq.…”
Section: Description Of the Vibrational Calculation Proceduresmentioning
“…The method is nonperturbative and based on the well known AI search procedure, developed and mainly applied for large scale calculations on highly excited vibrational states in polyatomic molecules [42][43][44][45][46][47]. The efficiency of our vibrational method is essentially based on the availability of a completely symmetrized, separable (in product form), unrestricted vibrational basis set |iae (Eq.…”
Section: Description Of the Vibrational Calculation Proceduresmentioning
“…The important task is that of choosing the dimension N 0 of the model space S 0 and the mode of construction of S 0 around an initial unperturbed state ͉i͘. Various approaches to a suitable definition of S 0 have been proposed in the literature; these include the adiabatic reduced coupled equation method [30], the low-frequency expansion method [31], and several artificial intelligence techniques [32][33][34]. In our approach we use an algorithm based on the wave operator formalism.…”
Section: B Iterative Integration Of H⍀ = ⍀H⍀mentioning
We present an iterative method for calculating eigenvalues and eigenvectors of large non-Hermitian matrices. The method uses an iterative procedure to solve the basic Bloch equation HOmega=OmegaHOmega of wave operator theory. It involves nonlinear transformations such as the translation of diagonal matrix elements in the complex plane and the use of Padé approximants to treat the strongly coupled states which constitute an intermediate space around the model space. In the particular case of Floquet eigenstates the further step of adding time-dependent absorbing boundaries significantly improves the convergence properties of the iterative calculations.
“…Equation 17has the advantage over eq. (18) of showing clearly that the wave operator is a non-unitary and non-singular transformation (T = 1 + X) which possesses a trivial inverse (T ?1 = 1 ? X) 31] (see g.1).…”
Section: The Time-dependent Wave Operatormentioning
confidence: 99%
“…The vectors belong to a subspace of relatively small dimension, which is usually called the active space (A.S) The literature o ers various formulations for selecting these active spaces and for projecting the quantum dynamics into them. Probably the best known approaches are arti cial intelligence techniques 16,17,18] for subspace selection and the recursive residue generation method 19], in which transition amplitudes are computed from a recursive calculation which uses the Lanczos algorithm to give the residues and poles of several Green's functions.…”
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