The quantum-mechanical Coulomb propagator in an L2 function representation

Abstract The quantum-mechanical Coulomb propagator is represented in a square-integrable basis of Sturmian functions. Herein, the Stieltjes integral containing the Coulomb spectral function as a weight is evaluated. The Coulomb propagator generally consists of two parts. The sum of the discrete part...

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Autores principales: Rolf Gersbacher, John T. Broad
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Lenguaje:EN
Publicado: Nature Portfolio 2021
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Acceso en línea:https://doaj.org/article/c219527a745f4e418a373e11a2abe5f3
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spelling oai:doaj.org-article:c219527a745f4e418a373e11a2abe5f32021-12-02T18:14:08ZThe quantum-mechanical Coulomb propagator in an L2 function representation10.1038/s41598-021-96925-02045-2322https://doaj.org/article/c219527a745f4e418a373e11a2abe5f32021-09-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-96925-0https://doaj.org/toc/2045-2322Abstract The quantum-mechanical Coulomb propagator is represented in a square-integrable basis of Sturmian functions. Herein, the Stieltjes integral containing the Coulomb spectral function as a weight is evaluated. The Coulomb propagator generally consists of two parts. The sum of the discrete part of the spectrum is extrapolated numerically, while three integration procedures are applied to the continuum part of the oscillating integral: the Gauss–Pollaczek quadrature, the Gauss–Legendre quadrature along the real axis, and a transformation into a contour integral in the complex plane with the subsequent Gauss–Legendre quadrature. Using the contour integral, the Coulomb propagator can be calculated very accurately from an L $$^2$$ 2 basis. Using the three-term recursion relation of the Pollaczek polynomials, an effective algorithm is herein presented to reduce the number of integrations. Numerical results are presented and discussed for all procedures.Rolf GersbacherJohn T. BroadNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-16 (2021)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Rolf Gersbacher
John T. Broad
The quantum-mechanical Coulomb propagator in an L2 function representation
description Abstract The quantum-mechanical Coulomb propagator is represented in a square-integrable basis of Sturmian functions. Herein, the Stieltjes integral containing the Coulomb spectral function as a weight is evaluated. The Coulomb propagator generally consists of two parts. The sum of the discrete part of the spectrum is extrapolated numerically, while three integration procedures are applied to the continuum part of the oscillating integral: the Gauss–Pollaczek quadrature, the Gauss–Legendre quadrature along the real axis, and a transformation into a contour integral in the complex plane with the subsequent Gauss–Legendre quadrature. Using the contour integral, the Coulomb propagator can be calculated very accurately from an L $$^2$$ 2 basis. Using the three-term recursion relation of the Pollaczek polynomials, an effective algorithm is herein presented to reduce the number of integrations. Numerical results are presented and discussed for all procedures.
format article
author Rolf Gersbacher
John T. Broad
author_facet Rolf Gersbacher
John T. Broad
author_sort Rolf Gersbacher
title The quantum-mechanical Coulomb propagator in an L2 function representation
title_short The quantum-mechanical Coulomb propagator in an L2 function representation
title_full The quantum-mechanical Coulomb propagator in an L2 function representation
title_fullStr The quantum-mechanical Coulomb propagator in an L2 function representation
title_full_unstemmed The quantum-mechanical Coulomb propagator in an L2 function representation
title_sort quantum-mechanical coulomb propagator in an l2 function representation
publisher Nature Portfolio
publishDate 2021
url https://doaj.org/article/c219527a745f4e418a373e11a2abe5f3
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