Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes

ABSTRACT: Auger CVV spectra of simple metals are generally believed to be well described by one-electronlike theories in the bulk which account for matrix elements and, in some cases, also static core-hole screening effects. We present here detailed calculations on Li, Be, Na, Mg, and Al using selfc...

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Autores:
Almbladh, Carl Olof
Morales Aramburo, Álvaro Luis
Tipo de recurso:
Article of investigation
Fecha de publicación:
1989
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/13081
Acceso en línea:
http://hdl.handle.net/10495/13081
Palabra clave:
Teoría de procesos
Metales simples
Efectos dinámicos
Formas de línea Auger
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 2.5 Colombia
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oai_identifier_str oai:bibliotecadigital.udea.edu.co:10495/13081
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network_name_str Repositorio UdeA
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dc.title.spa.fl_str_mv Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
title Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
spellingShingle Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
Teoría de procesos
Metales simples
Efectos dinámicos
Formas de línea Auger
title_short Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
title_full Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
title_fullStr Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
title_full_unstemmed Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
title_sort Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes
dc.creator.fl_str_mv Almbladh, Carl Olof
Morales Aramburo, Álvaro Luis
dc.contributor.author.none.fl_str_mv Almbladh, Carl Olof
Morales Aramburo, Álvaro Luis
dc.subject.none.fl_str_mv Teoría de procesos
Metales simples
Efectos dinámicos
Formas de línea Auger
topic Teoría de procesos
Metales simples
Efectos dinámicos
Formas de línea Auger
description ABSTRACT: Auger CVV spectra of simple metals are generally believed to be well described by one-electronlike theories in the bulk which account for matrix elements and, in some cases, also static core-hole screening effects. We present here detailed calculations on Li, Be, Na, Mg, and Al using selfconsistent bulk wave functions and proper matrix elements. The resulting spectra differ markedly from experiment and peak at too low energies. To explain this discrepancy we investigate effects of the surface and dynamical effects of the sudden disappearance of the core hole in the final state. To study core-hole effects we solve Mahan —Nozieres —De Dominicis (MND) model numerically over the entire band. The core-hole potential and other parameters in the MND model are determined by self-consistent calculations of the core-hole impurity. The results are compared with simpler approximations based on the final-state rule due to von Barth and Grossmann. To study surface and mean-free-path effects we perform slab calculations for Al but use a simpler infinite-barrier model in the remaining cases. The model reproduces the slab spectra for Al with very good accuracy. .In all cases investigated either the effects of the surface or the effects of the core hole give important modifications and a much improved agreement with experiment.
publishDate 1989
dc.date.issued.none.fl_str_mv 1989
dc.date.accessioned.none.fl_str_mv 2020-01-12T00:04:38Z
dc.date.available.none.fl_str_mv 2020-01-12T00:04:38Z
dc.type.spa.fl_str_mv info:eu-repo/semantics/article
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dc.identifier.citation.spa.fl_str_mv Almbladh, C. O., & Morales Aramburo, A. L. (1989). Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes. Physical Review B (Condensed Matter), 39(6), 3503-3516.
dc.identifier.issn.none.fl_str_mv 0163-1829
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10495/13081
dc.identifier.eissn.none.fl_str_mv 2469-9969
identifier_str_mv Almbladh, C. O., & Morales Aramburo, A. L. (1989). Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes. Physical Review B (Condensed Matter), 39(6), 3503-3516.
0163-1829
2469-9969
url http://hdl.handle.net/10495/13081
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournalabbrev.spa.fl_str_mv Physical Review B
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dc.publisher.spa.fl_str_mv American Physical Society
dc.publisher.group.spa.fl_str_mv Instrumentación Científica y Microelectrónica
institution Universidad de Antioquia
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spelling Almbladh, Carl OlofMorales Aramburo, Álvaro Luis2020-01-12T00:04:38Z2020-01-12T00:04:38Z1989Almbladh, C. O., & Morales Aramburo, A. L. (1989). Theory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapes. Physical Review B (Condensed Matter), 39(6), 3503-3516.0163-1829http://hdl.handle.net/10495/130812469-9969ABSTRACT: Auger CVV spectra of simple metals are generally believed to be well described by one-electronlike theories in the bulk which account for matrix elements and, in some cases, also static core-hole screening effects. We present here detailed calculations on Li, Be, Na, Mg, and Al using selfconsistent bulk wave functions and proper matrix elements. The resulting spectra differ markedly from experiment and peak at too low energies. To explain this discrepancy we investigate effects of the surface and dynamical effects of the sudden disappearance of the core hole in the final state. To study core-hole effects we solve Mahan —Nozieres —De Dominicis (MND) model numerically over the entire band. The core-hole potential and other parameters in the MND model are determined by self-consistent calculations of the core-hole impurity. The results are compared with simpler approximations based on the final-state rule due to von Barth and Grossmann. To study surface and mean-free-path effects we perform slab calculations for Al but use a simpler infinite-barrier model in the remaining cases. The model reproduces the slab spectra for Al with very good accuracy. .In all cases investigated either the effects of the surface or the effects of the core hole give important modifications and a much improved agreement with experiment.application/pdfengAmerican Physical SocietyInstrumentación Científica y Microelectrónicainfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/Teoría de procesosMetales simplesEfectos dinámicosFormas de línea AugerTheory of Auger core-valence-valence processes in simple metals. II. Dynamical and surface effects on Auger line shapesPhysical Review BPhysical Review B (Condensed Matter)35033516396ORIGINALMoralesAlvaro_1989_TheoryAugerCore.pdfMoralesAlvaro_1989_TheoryAugerCore.pdfArtículo de investigaciónapplication/pdf666996http://bibliotecadigital.udea.edu.co/bitstream/10495/13081/1/MoralesAlvaro_1989_TheoryAugerCore.pdfbdd0bcf210f6369a5bda3a4f04b5a6a3MD51CC-LICENSElicense_urllicense_urltext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/13081/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/13081/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/13081/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD54LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/13081/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD5510495/13081oai:bibliotecadigital.udea.edu.co:10495/130812021-05-16 11:48:19.464Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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