Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order

In this proceeding results for hyperon-nucleon interactions calculated at next-to-leading order (i.e. one-loop order) in SU(3) chiral effective field theory are presented. The potentials include contributions from one- and two-meson exchange, and four-baryon contact terms provided by the SU(3) chira...

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Main Author: Petschauer S.
Format: Article
Language:English
Published: EDP Sciences 2014-06-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20147305012
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author Petschauer S.
author_facet Petschauer S.
author_sort Petschauer S.
collection DOAJ
description In this proceeding results for hyperon-nucleon interactions calculated at next-to-leading order (i.e. one-loop order) in SU(3) chiral effective field theory are presented. The potentials include contributions from one- and two-meson exchange, and four-baryon contact terms provided by the SU(3) chiral Lagrangian. SU(3) flavor symmetry is imposed for the low-energy constants, while explicit SU(3) symmetry breaking is included only through the physical pseudoscalar-meson and baryon masses. Calculations have been performed for hyperon-nucleon scattering cross sections using a regularized Lippmann-Schwinger equation. A good description of the available data is achieved, comparable to modern phenomenological hyperon-nucleon interaction models. These results provide a new basis for studies of hypernuclei or hyperons in nuclear matter.
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spelling doaj.art-fcf445277ba64afa91582d78e235ca982022-12-21T21:04:27ZengEDP SciencesEPJ Web of Conferences2100-014X2014-06-01730501210.1051/epjconf/20147305012epjconf_menu2013_05012Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading orderPetschauer S.In this proceeding results for hyperon-nucleon interactions calculated at next-to-leading order (i.e. one-loop order) in SU(3) chiral effective field theory are presented. The potentials include contributions from one- and two-meson exchange, and four-baryon contact terms provided by the SU(3) chiral Lagrangian. SU(3) flavor symmetry is imposed for the low-energy constants, while explicit SU(3) symmetry breaking is included only through the physical pseudoscalar-meson and baryon masses. Calculations have been performed for hyperon-nucleon scattering cross sections using a regularized Lippmann-Schwinger equation. A good description of the available data is achieved, comparable to modern phenomenological hyperon-nucleon interaction models. These results provide a new basis for studies of hypernuclei or hyperons in nuclear matter.http://dx.doi.org/10.1051/epjconf/20147305012
spellingShingle Petschauer S.
Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
EPJ Web of Conferences
title Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
title_full Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
title_fullStr Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
title_full_unstemmed Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
title_short Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
title_sort chiral effective field theory description of the hyperon nucleon interaction at next to leading order
url http://dx.doi.org/10.1051/epjconf/20147305012
work_keys_str_mv AT petschauers chiraleffectivefieldtheorydescriptionofthehyperonnucleoninteractionatnexttoleadingorder