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Incompatible Coulomb hamiltonian extensions

We revisit the resolution of the one-dimensional Schrödinger hamiltonian with a Coulomb λ/|x| potential. We examine among its self-adjoint extensions those which are compatible with physical conservation laws. In the one-dimensional semi-infinite case, we show that they are classified on a U(1) circ...

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Autor principal: Abramovici, G.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7190704/
https://www.ncbi.nlm.nih.gov/pubmed/32350289
http://dx.doi.org/10.1038/s41598-020-62144-2
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author Abramovici, G.
author_facet Abramovici, G.
author_sort Abramovici, G.
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description We revisit the resolution of the one-dimensional Schrödinger hamiltonian with a Coulomb λ/|x| potential. We examine among its self-adjoint extensions those which are compatible with physical conservation laws. In the one-dimensional semi-infinite case, we show that they are classified on a U(1) circle in the attractive case and on [Formula: see text] in the repulsive one. In the one-dimensional infinite case, we find a specific and original classification by studying the continuity of eigenfunctions. In all cases, different extensions are incompatible one with the other. For an actual experiment with an attractive potential, the bound spectrum can be used to discriminate which extension is the correct one.
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spelling pubmed-71907042020-05-05 Incompatible Coulomb hamiltonian extensions Abramovici, G. Sci Rep Article We revisit the resolution of the one-dimensional Schrödinger hamiltonian with a Coulomb λ/|x| potential. We examine among its self-adjoint extensions those which are compatible with physical conservation laws. In the one-dimensional semi-infinite case, we show that they are classified on a U(1) circle in the attractive case and on [Formula: see text] in the repulsive one. In the one-dimensional infinite case, we find a specific and original classification by studying the continuity of eigenfunctions. In all cases, different extensions are incompatible one with the other. For an actual experiment with an attractive potential, the bound spectrum can be used to discriminate which extension is the correct one. Nature Publishing Group UK 2020-04-29 /pmc/articles/PMC7190704/ /pubmed/32350289 http://dx.doi.org/10.1038/s41598-020-62144-2 Text en © The Author(s) 2020 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Abramovici, G.
Incompatible Coulomb hamiltonian extensions
title Incompatible Coulomb hamiltonian extensions
title_full Incompatible Coulomb hamiltonian extensions
title_fullStr Incompatible Coulomb hamiltonian extensions
title_full_unstemmed Incompatible Coulomb hamiltonian extensions
title_short Incompatible Coulomb hamiltonian extensions
title_sort incompatible coulomb hamiltonian extensions
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7190704/
https://www.ncbi.nlm.nih.gov/pubmed/32350289
http://dx.doi.org/10.1038/s41598-020-62144-2
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