Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons

Autores
Yépez Martínez, Tochtli Cuauhtli; Civitarese, Enrique Osvaldo; Hess, Peter O.
Año de publicación
2018
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
Starting from an algebraic model based on the QCD-Hamiltonian and previously applied to study meson states, we have developed an extension of it in order to explore the structure of baryon states. In developing our approach we have adapted concepts taken from group theory and non-perturbative many-body methods to describe states built from effective quarks and anti-quarks degrees of freedom. As a Hamiltonian we have used the QCD Hamiltonian written in the Coulomb Gauge, and expressed it in terms of effective quark-antiquark, di-quarks and di-antiquark excitations. To gain some insights about the relevant interactions of quarks in hadronic states, the Hamiltonian was approximately diagonalized by mapping quark-antiquark pairs and di-quarks (di-antiquarks) onto phonon states. In dealing with the structure of the vacuum of the theory, color-scalar and color-vector states are introduced to account for ground-state correlations. While the use of a purely color-scalar ground state is an obvious choice, so that colorless hadrons contain at least three quarks, the presence of coupled color-vector pairs in the ground state allows for colorless excitations resulting from the action of color objects upon it.
Fil: Yepez-Martinez, Tochtli. Universidad Nacional de La Plata; Argentina. IFLP, CONICET/UNLP; Argentina; Argentina
Fil: Civitarese, Enrique Osvaldo. Universidad Nacional de La Plata; Argentina. IFLP, CONICET/UNLP; Argentina; Argentina
Fil: Hess, Peter O.. Universidad Nacional Autónoma de México. Instituto de Ciencias Nucleares; México. Frankfurt Institute For Advanced Studies;
Materia
Non perturbative qcd
Barions
Coulomb gauge
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:11336/95916

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network_name_str CONICET Digital (CONICET)
spelling Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesonsYépez Martínez, Tochtli CuauhtliCivitarese, Enrique OsvaldoHess, Peter O.Non perturbative qcdBarionsCoulomb gaugehttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Starting from an algebraic model based on the QCD-Hamiltonian and previously applied to study meson states, we have developed an extension of it in order to explore the structure of baryon states. In developing our approach we have adapted concepts taken from group theory and non-perturbative many-body methods to describe states built from effective quarks and anti-quarks degrees of freedom. As a Hamiltonian we have used the QCD Hamiltonian written in the Coulomb Gauge, and expressed it in terms of effective quark-antiquark, di-quarks and di-antiquark excitations. To gain some insights about the relevant interactions of quarks in hadronic states, the Hamiltonian was approximately diagonalized by mapping quark-antiquark pairs and di-quarks (di-antiquarks) onto phonon states. In dealing with the structure of the vacuum of the theory, color-scalar and color-vector states are introduced to account for ground-state correlations. While the use of a purely color-scalar ground state is an obvious choice, so that colorless hadrons contain at least three quarks, the presence of coupled color-vector pairs in the ground state allows for colorless excitations resulting from the action of color objects upon it.Fil: Yepez-Martinez, Tochtli. Universidad Nacional de La Plata; Argentina. IFLP, CONICET/UNLP; Argentina; ArgentinaFil: Civitarese, Enrique Osvaldo. Universidad Nacional de La Plata; Argentina. IFLP, CONICET/UNLP; Argentina; ArgentinaFil: Hess, Peter O.. Universidad Nacional Autónoma de México. Instituto de Ciencias Nucleares; México. Frankfurt Institute For Advanced Studies;Springer2018-02info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/95916Yépez Martínez, Tochtli Cuauhtli; Civitarese, Enrique Osvaldo; Hess, Peter O.; Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons; Springer; European Physical Journal A - Hadrons and Nuclei; 54; 22; 2-2018; 1-91434-6001CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/doi/10.1140/epja/i2018-12424-7info:eu-repo/semantics/altIdentifier/url/https://link.springer.com/article/10.1140%2Fepja%2Fi2018-12424-7info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-10-22T11:29:16Zoai:ri.conicet.gov.ar:11336/95916instacron: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:34982025-10-22 11:29:17.236CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
title Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
spellingShingle Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
Yépez Martínez, Tochtli Cuauhtli
Non perturbative qcd
Barions
Coulomb gauge
title_short Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
title_full Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
title_fullStr Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
title_full_unstemmed Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
title_sort Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons
dc.creator.none.fl_str_mv Yépez Martínez, Tochtli Cuauhtli
Civitarese, Enrique Osvaldo
Hess, Peter O.
author Yépez Martínez, Tochtli Cuauhtli
author_facet Yépez Martínez, Tochtli Cuauhtli
Civitarese, Enrique Osvaldo
Hess, Peter O.
author_role author
author2 Civitarese, Enrique Osvaldo
Hess, Peter O.
author2_role author
author
dc.subject.none.fl_str_mv Non perturbative qcd
Barions
Coulomb gauge
topic Non perturbative qcd
Barions
Coulomb gauge
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv Starting from an algebraic model based on the QCD-Hamiltonian and previously applied to study meson states, we have developed an extension of it in order to explore the structure of baryon states. In developing our approach we have adapted concepts taken from group theory and non-perturbative many-body methods to describe states built from effective quarks and anti-quarks degrees of freedom. As a Hamiltonian we have used the QCD Hamiltonian written in the Coulomb Gauge, and expressed it in terms of effective quark-antiquark, di-quarks and di-antiquark excitations. To gain some insights about the relevant interactions of quarks in hadronic states, the Hamiltonian was approximately diagonalized by mapping quark-antiquark pairs and di-quarks (di-antiquarks) onto phonon states. In dealing with the structure of the vacuum of the theory, color-scalar and color-vector states are introduced to account for ground-state correlations. While the use of a purely color-scalar ground state is an obvious choice, so that colorless hadrons contain at least three quarks, the presence of coupled color-vector pairs in the ground state allows for colorless excitations resulting from the action of color objects upon it.
Fil: Yepez-Martinez, Tochtli. Universidad Nacional de La Plata; Argentina. IFLP, CONICET/UNLP; Argentina; Argentina
Fil: Civitarese, Enrique Osvaldo. Universidad Nacional de La Plata; Argentina. IFLP, CONICET/UNLP; Argentina; Argentina
Fil: Hess, Peter O.. Universidad Nacional Autónoma de México. Instituto de Ciencias Nucleares; México. Frankfurt Institute For Advanced Studies;
description Starting from an algebraic model based on the QCD-Hamiltonian and previously applied to study meson states, we have developed an extension of it in order to explore the structure of baryon states. In developing our approach we have adapted concepts taken from group theory and non-perturbative many-body methods to describe states built from effective quarks and anti-quarks degrees of freedom. As a Hamiltonian we have used the QCD Hamiltonian written in the Coulomb Gauge, and expressed it in terms of effective quark-antiquark, di-quarks and di-antiquark excitations. To gain some insights about the relevant interactions of quarks in hadronic states, the Hamiltonian was approximately diagonalized by mapping quark-antiquark pairs and di-quarks (di-antiquarks) onto phonon states. In dealing with the structure of the vacuum of the theory, color-scalar and color-vector states are introduced to account for ground-state correlations. While the use of a purely color-scalar ground state is an obvious choice, so that colorless hadrons contain at least three quarks, the presence of coupled color-vector pairs in the ground state allows for colorless excitations resulting from the action of color objects upon it.
publishDate 2018
dc.date.none.fl_str_mv 2018-02
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/11336/95916
Yépez Martínez, Tochtli Cuauhtli; Civitarese, Enrique Osvaldo; Hess, Peter O.; Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons; Springer; European Physical Journal A - Hadrons and Nuclei; 54; 22; 2-2018; 1-9
1434-6001
CONICET Digital
CONICET
url http://hdl.handle.net/11336/95916
identifier_str_mv Yépez Martínez, Tochtli Cuauhtli; Civitarese, Enrique Osvaldo; Hess, Peter O.; Non-perturbative RPA-method implemented in the Coulomb gauge QCD Hamiltonian: From quarks and gluons to baryons and mesons; Springer; European Physical Journal A - Hadrons and Nuclei; 54; 22; 2-2018; 1-9
1434-6001
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/doi/10.1140/epja/i2018-12424-7
info:eu-repo/semantics/altIdentifier/url/https://link.springer.com/article/10.1140%2Fepja%2Fi2018-12424-7
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 Springer
publisher.none.fl_str_mv Springer
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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