Two- and three-body resonances in the $ar{K}$NN − πΣN system

One of the most important characteristics of a two-body interaction is existence and properties of its bound states or resonances. When the interaction is used in a few- or many-body calculation they also strongly influence the properties of the few- or many-body system. We investigate the depende...

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Main Author: Shevchenko N.V.
Format: Article
Language:English
Published: EDP Sciences 2010-04-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20100303018
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author Shevchenko N.V.
author_facet Shevchenko N.V.
author_sort Shevchenko N.V.
collection DOAJ
description One of the most important characteristics of a two-body interaction is existence and properties of its bound states or resonances. When the interaction is used in a few- or many-body calculation they also strongly influence the properties of the few- or many-body system. We investigate the dependence of the three-body resonance properties in the $ar{K}$NN system on the different models of $ar{K}$N interaction, providing one or two poles for Λ(1405) resonance. The $ar{K}$NN − πΣN system is described by coupled-channel Faddeev equations in AGS form, our two-body $ar{K}$N − πΣ interaction models reproduce all existing experimental data on K− p scattering and K− p atom level shift.
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spelling doaj.art-c006860ae0bc40699d1dd06e7bd470682022-12-21T23:18:35ZengEDP SciencesEPJ Web of Conferences2100-014X2010-04-0130301810.1051/epjconf/20100303018Two- and three-body resonances in the $ar{K}$NN − πΣN systemShevchenko N.V.One of the most important characteristics of a two-body interaction is existence and properties of its bound states or resonances. When the interaction is used in a few- or many-body calculation they also strongly influence the properties of the few- or many-body system. We investigate the dependence of the three-body resonance properties in the $ar{K}$NN system on the different models of $ar{K}$N interaction, providing one or two poles for Λ(1405) resonance. The $ar{K}$NN − πΣN system is described by coupled-channel Faddeev equations in AGS form, our two-body $ar{K}$N − πΣ interaction models reproduce all existing experimental data on K− p scattering and K− p atom level shift.http://dx.doi.org/10.1051/epjconf/20100303018
spellingShingle Shevchenko N.V.
Two- and three-body resonances in the $ar{K}$NN − πΣN system
EPJ Web of Conferences
title Two- and three-body resonances in the $ar{K}$NN − πΣN system
title_full Two- and three-body resonances in the $ar{K}$NN − πΣN system
title_fullStr Two- and three-body resonances in the $ar{K}$NN − πΣN system
title_full_unstemmed Two- and three-body resonances in the $ar{K}$NN − πΣN system
title_short Two- and three-body resonances in the $ar{K}$NN − πΣN system
title_sort two and three body resonances in the ar k nn πσn system
url http://dx.doi.org/10.1051/epjconf/20100303018
work_keys_str_mv AT shevchenkonv twoandthreebodyresonancesinthearknnpsnsystem