Diffusion of Sn in different purity α-Ti

Autores
Perez, Rodolfo Ariel; Dyment, Fanny; Behar, Andrea Marcela
Año de publicación
2003
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
The diffusion of Sn in the hcp (α) phase of high purity (99.99%) and pure (99.9%) Ti was studied at different temperatures from 873 up to 1100 K. The Rutherford Backscattering Spectrometry (RBS) technique was used to obtain the penetration profiles. The evolution of the diffusion coefficient, D, as a function of temperature follows the prediction of the Arrhenius law. No significant difference between both kinds of Ti samples was observed. Normal diffusion parameters, Q and D0, close to the self-diffusion ones were obtained.
Fil: Perez, Rodolfo Ariel. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica; Argentina
Fil: Dyment, Fanny. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica; Argentina
Fil: Behar, Andrea Marcela. Universidade Federal do Rio Grande do Sul; Brasil
Materia
Diffusion
Enhanced Diffusion
Hcp Metals
Rbs
Sn
Ti
Ultra-Fast Diffusion
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/42734

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network_name_str CONICET Digital (CONICET)
spelling Diffusion of Sn in different purity α-TiPerez, Rodolfo ArielDyment, FannyBehar, Andrea MarcelaDiffusionEnhanced DiffusionHcp MetalsRbsSnTiUltra-Fast Diffusionhttps://purl.org/becyt/ford/1.1https://purl.org/becyt/ford/1The diffusion of Sn in the hcp (α) phase of high purity (99.99%) and pure (99.9%) Ti was studied at different temperatures from 873 up to 1100 K. The Rutherford Backscattering Spectrometry (RBS) technique was used to obtain the penetration profiles. The evolution of the diffusion coefficient, D, as a function of temperature follows the prediction of the Arrhenius law. No significant difference between both kinds of Ti samples was observed. Normal diffusion parameters, Q and D0, close to the self-diffusion ones were obtained.Fil: Perez, Rodolfo Ariel. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica; ArgentinaFil: Dyment, Fanny. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica; ArgentinaFil: Behar, Andrea Marcela. Universidade Federal do Rio Grande do Sul; BrasilElsevier Science2003-05info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/42734Perez, Rodolfo Ariel; Dyment, Fanny; Behar, Andrea Marcela; Diffusion of Sn in different purity α-Ti; Elsevier Science; Materials Letters; 57; 18; 5-2003; 2670-26740167-577XCONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/doi/10.1016/S0167-577X(02)01353-8info:eu-repo/semantics/altIdentifier/url/https://www.sciencedirect.com/science/article/pii/S0167577X02013538info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-09-29T09:51:59Zoai:ri.conicet.gov.ar:11336/42734instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-09-29 09:52:00.062CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Diffusion of Sn in different purity α-Ti
title Diffusion of Sn in different purity α-Ti
spellingShingle Diffusion of Sn in different purity α-Ti
Perez, Rodolfo Ariel
Diffusion
Enhanced Diffusion
Hcp Metals
Rbs
Sn
Ti
Ultra-Fast Diffusion
title_short Diffusion of Sn in different purity α-Ti
title_full Diffusion of Sn in different purity α-Ti
title_fullStr Diffusion of Sn in different purity α-Ti
title_full_unstemmed Diffusion of Sn in different purity α-Ti
title_sort Diffusion of Sn in different purity α-Ti
dc.creator.none.fl_str_mv Perez, Rodolfo Ariel
Dyment, Fanny
Behar, Andrea Marcela
author Perez, Rodolfo Ariel
author_facet Perez, Rodolfo Ariel
Dyment, Fanny
Behar, Andrea Marcela
author_role author
author2 Dyment, Fanny
Behar, Andrea Marcela
author2_role author
author
dc.subject.none.fl_str_mv Diffusion
Enhanced Diffusion
Hcp Metals
Rbs
Sn
Ti
Ultra-Fast Diffusion
topic Diffusion
Enhanced Diffusion
Hcp Metals
Rbs
Sn
Ti
Ultra-Fast Diffusion
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.1
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv The diffusion of Sn in the hcp (α) phase of high purity (99.99%) and pure (99.9%) Ti was studied at different temperatures from 873 up to 1100 K. The Rutherford Backscattering Spectrometry (RBS) technique was used to obtain the penetration profiles. The evolution of the diffusion coefficient, D, as a function of temperature follows the prediction of the Arrhenius law. No significant difference between both kinds of Ti samples was observed. Normal diffusion parameters, Q and D0, close to the self-diffusion ones were obtained.
Fil: Perez, Rodolfo Ariel. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica; Argentina
Fil: Dyment, Fanny. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica; Argentina
Fil: Behar, Andrea Marcela. Universidade Federal do Rio Grande do Sul; Brasil
description The diffusion of Sn in the hcp (α) phase of high purity (99.99%) and pure (99.9%) Ti was studied at different temperatures from 873 up to 1100 K. The Rutherford Backscattering Spectrometry (RBS) technique was used to obtain the penetration profiles. The evolution of the diffusion coefficient, D, as a function of temperature follows the prediction of the Arrhenius law. No significant difference between both kinds of Ti samples was observed. Normal diffusion parameters, Q and D0, close to the self-diffusion ones were obtained.
publishDate 2003
dc.date.none.fl_str_mv 2003-05
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/42734
Perez, Rodolfo Ariel; Dyment, Fanny; Behar, Andrea Marcela; Diffusion of Sn in different purity α-Ti; Elsevier Science; Materials Letters; 57; 18; 5-2003; 2670-2674
0167-577X
CONICET Digital
CONICET
url http://hdl.handle.net/11336/42734
identifier_str_mv Perez, Rodolfo Ariel; Dyment, Fanny; Behar, Andrea Marcela; Diffusion of Sn in different purity α-Ti; Elsevier Science; Materials Letters; 57; 18; 5-2003; 2670-2674
0167-577X
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/doi/10.1016/S0167-577X(02)01353-8
info:eu-repo/semantics/altIdentifier/url/https://www.sciencedirect.com/science/article/pii/S0167577X02013538
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/pdf
dc.publisher.none.fl_str_mv Elsevier Science
publisher.none.fl_str_mv Elsevier Science
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
collection CONICET Digital (CONICET)
instname_str Consejo Nacional de Investigaciones Científicas y Técnicas
repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
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score 13.070432