1965
DOI: 10.1063/1.1696963
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Calculation of Matrix Elements for One-Dimensional Quantum-Mechanical Problems and the Application to Anharmonic Oscillators

Abstract: A simple method using the techniques of transformation theory for the generation of the matrix elements of unusual potential fUnctions for. one-dimensional quantum-mechanical problems is described. It is applicable both to functions which exist as a set of points, for example, a curve or table, as welJ as to those in explicit form. Some representative calculations have been made for anharmonic oscillators.

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Cited by 636 publications
(278 citation statements)
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“…It turns out that this is conveniently performed in the discrete eigenbasis of the position operator q. This representation is the so-termed discrete variable representation (DVR) [58]. The reason for this basis transformation is that only then can the influence phase, Eq.…”
Section: The Reduced Density Matrix In the Discrete Variable Repmentioning
confidence: 99%
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“…It turns out that this is conveniently performed in the discrete eigenbasis of the position operator q. This representation is the so-termed discrete variable representation (DVR) [58]. The reason for this basis transformation is that only then can the influence phase, Eq.…”
Section: The Reduced Density Matrix In the Discrete Variable Repmentioning
confidence: 99%
“…Next we perform a basis transformation to the so-called discrete variable representation (DVR) [58]. The new basis is chosen as the eigenbasis of that operator which couples the bare system to the harmonic bath.…”
Section: B Real-time Paths In the Dvr Basismentioning
confidence: 99%
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“…Starting from the system-plusreservoir model of a driven ratchet system bilinearly coupled to a harmonic oscillator bath, we proceed in three steps: (i) We consider the regime of temperature and driving parameters which allow the truncation of the full dynamics to the Hilbert space spanned by the M lowest bands of the periodic ratchet potential. (ii) A rotation to the so-called discrete variable representation (DVR) [12], being the eigenbasis of the discrete position operator coupling to the bath, is performed. In this basis, the isolated ratchet problem is described by a tightbinding model with a periodicity of M sites, and with further nearest-neighbor coupling.…”
mentioning
confidence: 99%
“…This requires one, however, to express the full system-plusbath Hamiltonian H t in the basis of the eigenstates of the position operator, the so-termed DVR [12,13]. The contributions H ext t and H B to H t are already diagonal in this basis, but not the isolated ratchet Hamiltonian.…”
mentioning
confidence: 99%