A systematic improved comparison equation method to solve the Schrijdinger equation is described. The method is useful in quantum mechanical calculations inv&~ -0 or more titian or turning points and is applicable to real potentials with continuol;s derivatives. As a computatior 4 example of the met
An improved shooting method for one-dimensional Schrödinger equation
✍ Scribed by Tomasz BŁeński; Jacques Ligou
- Publisher
- Elsevier Science
- Year
- 1988
- Tongue
- English
- Weight
- 756 KB
- Volume
- 50
- Category
- Article
- ISSN
- 0010-4655
No coin nor oath required. For personal study only.
✦ Synopsis
The phase function theory is used to improve the shooting method with the Noumerov finite difference scheme in application to finding bound states of the radial Schrodinger equation. The phase functions are constructed from Noumerov trial solutions which prevents the separate calculations of eigenvalues and eigenfunctions. The difference of the forward and backward phases is a monotomc function of the trial eigenvalue with zero at the eigenvalue. The radial quantum number is introduced as input in the phase difference. The discontinuity of the phase function with respect to the trial eigenvalue at singular points is used as diagnostics for the matching points. The modified shooting method with the Noumerov scheme and the phase function method connected with the first order nonlinear equation are compared in the numerical example.
leads to the same problems as the Noumerov References scheme in case of a wrong matching point.
📜 SIMILAR VOLUMES
An alternative formulation of the "shooting" method for a numerical solution of the Schr0dinger equation is described for :ases of general asymmetric one-dimensional potential (planar geometry), and spherically symmetric potential. The method relies on matching the asymptotic wavefunctions and the p
A new integral equation method for the numerical solution of the radial Schrödinger equation in one dimension, developed by the authors (1997, J. Comput. Phys. 134, 134), is extended to systems of coupled Schrödinger equations with both positive and negative channel energies. The method, carried out