1999
DOI: 10.1071/ph98109
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Towards a Direct Numerical Solution of Schrödinger’s Equation for (e, 2e) Reactions

Abstract: The finite-difference method for electron{hydrogen scattering is presented in a simple, easily understood form for a model collision problem in which all angular momentum is neglected. The model Schrödinger equation is integrated outwards from the atomic centre on a grid of fixed spacing h. The number of difference equations is reduced each step outwards using an algorithm due to Poet, resulting in a propagating solution of the partial-differential equation. By imposing correct asymptotic boundary conditions o… Show more

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Cited by 5 publications
(6 citation statements)
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“…where the sparse matrices, A, B and C, and the − → χ vector are determined from the coefficients of a two-dimensional 3-point Numerov finite difference formula, modified to allow for arbitrary changes in grid spacing, including the change from real to complex coordinates at R 0 . This propagation technique is based on that used by Poet (1980) for e-H scattering and more recently by Jones and Stelbovics (1999) and Jones and Stelbovics (2002) for their benchmark calculations for the Temkin-Poet model for e-H ionization. We have previously given details for the l = 0 modified Numerov formula (Bartlett and Stelbovics 2004), which uses the eight nearest-neighbour grid points in its calculations.…”
Section: L70mentioning
confidence: 99%
“…where the sparse matrices, A, B and C, and the − → χ vector are determined from the coefficients of a two-dimensional 3-point Numerov finite difference formula, modified to allow for arbitrary changes in grid spacing, including the change from real to complex coordinates at R 0 . This propagation technique is based on that used by Poet (1980) for e-H scattering and more recently by Jones and Stelbovics (1999) and Jones and Stelbovics (2002) for their benchmark calculations for the Temkin-Poet model for e-H ionization. We have previously given details for the l = 0 modified Numerov formula (Bartlett and Stelbovics 2004), which uses the eight nearest-neighbour grid points in its calculations.…”
Section: L70mentioning
confidence: 99%
“…To begin the propagation at the first column (i = 1) we note that A (1) is a null vector and D (0) and − → E (0) are not required to be known, and in fact are also null. We can therefore reduce (51) and (52) to…”
Section: Propagation Methodsmentioning
confidence: 99%
“…The Numerov formula has been used successfully for e-H model problems for scattering [30] and ionization [52] and the full e-H scattering problem [54], but to our knowledge has not previously been adapted for variable grids. Jones and Stelbovics [55] used a grid-doubling method that allowed their grid spacing to be increased by integer multiples (whilst continuing to use evenly spaced points for the Numerov formula).…”
Section: Numerov Formulaementioning
confidence: 99%
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“…Nevertheless, a solution can be found by the standard method of minimizing the sum of the squares of the residuals [the differences between the left-and right-hand sides of equations (11)]. Previously we found [5] that the least-squares method is generally stabler than keeping any subset of just N equations (11).…”
mentioning
confidence: 99%