Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference

Autores
Chatterjee, S.; Misra, D.; Kelkar, A. H.; Fainstein, Pablo Daniel; Tribedi, L. C.
Año de publicación
2010
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
Electrons emitted from H2 in collisions with 5 MeV/u F9 + ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20° and 160°. The measured energy and Electrons emitted from H2 in collisions with 5 MeV/u F9+ ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20◦ and 160◦. The measured energy and angular distributions of double-differential cross sections (DDCSs) of these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.
Fil: Chatterjee, S.. Tata Institute of Fundamental Research; India
Fil: Misra, D.. Tata Institute of Fundamental Research; India
Fil: Kelkar, A. H.. Tata Institute of Fundamental Research; India
Fil: Fainstein, Pablo Daniel. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Patagonia Norte; Argentina. Comisión Nacional de Energía Atómica. Centro Atómico Bariloche; Argentina
Fil: Tribedi, L. C.. Tata Institute of Fundamental Research; India
Materia
Energy and angular distributions
Young-type interference
Ionization of molecular hydrogen
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:11336/279194

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repository_id_str 3498
network_name_str CONICET Digital (CONICET)
spelling Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interferenceChatterjee, S.Misra, D.Kelkar, A. H.Fainstein, Pablo DanielTribedi, L. C.Energy and angular distributionsYoung-type interferenceIonization of molecular hydrogenhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Electrons emitted from H2 in collisions with 5 MeV/u F9 + ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20° and 160°. The measured energy and Electrons emitted from H2 in collisions with 5 MeV/u F9+ ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20◦ and 160◦. The measured energy and angular distributions of double-differential cross sections (DDCSs) of these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.Fil: Chatterjee, S.. Tata Institute of Fundamental Research; IndiaFil: Misra, D.. Tata Institute of Fundamental Research; IndiaFil: Kelkar, A. H.. Tata Institute of Fundamental Research; IndiaFil: Fainstein, Pablo Daniel. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Patagonia Norte; Argentina. Comisión Nacional de Energía Atómica. Centro Atómico Bariloche; ArgentinaFil: Tribedi, L. C.. Tata Institute of Fundamental Research; IndiaIOP Publishing2010-06info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/279194Chatterjee, S.; Misra, D.; Kelkar, A. H.; Fainstein, Pablo Daniel; Tribedi, L. C.; Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference; IOP Publishing; Journal of Physics B: Atomic, Molecular and Optical Physics; 43; 12; 6-2010; 1-80953-4075CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/https://iopscience.iop.org/article/10.1088/0953-4075/43/12/125201info:eu-repo/semantics/altIdentifier/doi/10.1088/0953-4075/43/12/125201info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2026-02-26T10:34:11Zoai:ri.conicet.gov.ar:11336/279194instacron: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:34982026-02-26 10:34:11.364CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
title Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
spellingShingle Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
Chatterjee, S.
Energy and angular distributions
Young-type interference
Ionization of molecular hydrogen
title_short Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
title_full Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
title_fullStr Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
title_full_unstemmed Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
title_sort Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference
dc.creator.none.fl_str_mv Chatterjee, S.
Misra, D.
Kelkar, A. H.
Fainstein, Pablo Daniel
Tribedi, L. C.
author Chatterjee, S.
author_facet Chatterjee, S.
Misra, D.
Kelkar, A. H.
Fainstein, Pablo Daniel
Tribedi, L. C.
author_role author
author2 Misra, D.
Kelkar, A. H.
Fainstein, Pablo Daniel
Tribedi, L. C.
author2_role author
author
author
author
dc.subject.none.fl_str_mv Energy and angular distributions
Young-type interference
Ionization of molecular hydrogen
topic Energy and angular distributions
Young-type interference
Ionization of molecular hydrogen
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv Electrons emitted from H2 in collisions with 5 MeV/u F9 + ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20° and 160°. The measured energy and Electrons emitted from H2 in collisions with 5 MeV/u F9+ ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20◦ and 160◦. The measured energy and angular distributions of double-differential cross sections (DDCSs) of these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.
Fil: Chatterjee, S.. Tata Institute of Fundamental Research; India
Fil: Misra, D.. Tata Institute of Fundamental Research; India
Fil: Kelkar, A. H.. Tata Institute of Fundamental Research; India
Fil: Fainstein, Pablo Daniel. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Patagonia Norte; Argentina. Comisión Nacional de Energía Atómica. Centro Atómico Bariloche; Argentina
Fil: Tribedi, L. C.. Tata Institute of Fundamental Research; India
description Electrons emitted from H2 in collisions with 5 MeV/u F9 + ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20° and 160°. The measured energy and Electrons emitted from H2 in collisions with 5 MeV/u F9+ ions were measured in the energy range from 1 to 300 eV and a wide range of emission angles between 20◦ and 160◦. The measured energy and angular distributions of double-differential cross sections (DDCSs) of these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.these electrons are compared with the molecular continuum distorted wave-eikonal initial state (CDW-EIS) calculation. The observed energy and angular distributions can be explained, in general, with the help of the two-centre effect which is included in the CDW-EIS model. In addition, the DDCS ratios of molecular-to-atomic hydrogen exhibit an oscillatory structure which is discussed in terms of Young-type electron interference. We have obtained the frequencies of such oscillations and studied their angular dependence. The single-differential cross sections (SDCSs) are deduced by integrating the DDCSs over solid angle and emission energy. We demonstrate that the SDCS ratio spectra also preserve the signature of interference to some extent. The asymmetry parameter, derived only from the molecular cross sections for forward and backward angles, shows an oscillatory behaviour as a function of electron velocity. This is understood in terms of the interference effect superimposed with the post-collisional two-centre effect.
publishDate 2010
dc.date.none.fl_str_mv 2010-06
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/11336/279194
Chatterjee, S.; Misra, D.; Kelkar, A. H.; Fainstein, Pablo Daniel; Tribedi, L. C.; Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference; IOP Publishing; Journal of Physics B: Atomic, Molecular and Optical Physics; 43; 12; 6-2010; 1-8
0953-4075
CONICET Digital
CONICET
url http://hdl.handle.net/11336/279194
identifier_str_mv Chatterjee, S.; Misra, D.; Kelkar, A. H.; Fainstein, Pablo Daniel; Tribedi, L. C.; Ionization of molecular hydrogen by 5 MeV/u bare fluorine ion and electron interference; IOP Publishing; Journal of Physics B: Atomic, Molecular and Optical Physics; 43; 12; 6-2010; 1-8
0953-4075
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/url/https://iopscience.iop.org/article/10.1088/0953-4075/43/12/125201
info:eu-repo/semantics/altIdentifier/doi/10.1088/0953-4075/43/12/125201
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 IOP Publishing
publisher.none.fl_str_mv IOP Publishing
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
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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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