An extension to the theory of Schrodinger equations has been made ẅhich enables the derivation of eigenvalues from a consideration of a very small part of geometric space. The concomitant unwanted continuum effects have been removed. The theory enables very convergent or ''superconvergent'' calculat
An Efficient Chebyshev–Lanczos Method for Obtaining Eigensolutions of the Schrödinger Equation on a Grid
✍ Scribed by M. Braun; S.A. Sofianos; D.G. Papageorgiou; I.E. Lagaris
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 432 KB
- Volume
- 126
- Category
- Article
- ISSN
- 0021-9991
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✦ Synopsis
been employed in bound state calculations, where the spectrum of the Hamiltonian can be obtained from the solution A grid method for obtaining eigensolutions of bound systems is presented. In this, the block-Lanczos method is applied to a Chebyof the TDSE. The problem usually encountered is the shev approximation of exp(ϪH/⌬), where ⌬ is the range of eigenvaldiagonalization of the Hamiltonian H in (1). Since this in ues we are interested in. With this choice a preferential convergence practice cannot be done, it is impossible to compute the of the eigenvectors corresponding to low-lying eigenvalues of H is action of the propagator e ϪitH on an arbitrary wave function achieved. The method is used to solve a variety of one-, two-, and three-dimensional problems. To apply the kinetic energy operator [2] and, thus, the time-evolution is accomplished using we use the fast sine transform instead of the fast Fourier transform, various approximations to the exponential. We mention thus fullfilling, a priori, the box boundary conditions. We further here the Crank-Nicolson scheme [3-5] and the Kosloff extend the Chebyshev approximation to treat general functions of and Tal-Ezer method [6]. For a detailed discussion we refer matrices, thus allowing its application to cases for which no analytithe reader to the review article of de Raedt [2]. The existing cal expressions of the expansion coefficients are available. ᮊ 1996 Academic Press, Inc.
methods, although simple to use, can be quite CPU-time intensive, especially in calculating a large number of bound states in more than one dimension.
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A family of new hybrid explicit four-step tenth algebraic order methods ## Ž . with phase lag of order 18 2 26 is developed for efficient computations of the Schrodinger ëquation. Based on these new methods, a new embedded variable-step method is obtained. Numerical results produced for the nume
The form ⌿ x, t s F x q F x, t e q F x, t e e is 0 1 y1 used for the wave function in the transient solutions. This expression is similar to the three dominant terms in the steady-state solution from the Floquet theory, except that now F and F depend on t as well as x. The function F is the static