Structure of the X(3872) and its Isospin Symmetry Breaking

In order to understand the structure of the X(3872), we have studied the effects of the ${c}ar{c}$ charmonium core state coupling to the D0 $ar{D^{0}*}$ and D+ D−* molecule states. We determine the coupling strength so as to reproduce the observed mass of the the X(3872). The isospin symmetry break...

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Main Authors: Takeuchi S., Takizawa M.
Format: Article
Language:English
Published: EDP Sciences 2010-04-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20100303026
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author Takeuchi S.
Takizawa M.
author_facet Takeuchi S.
Takizawa M.
author_sort Takeuchi S.
collection DOAJ
description In order to understand the structure of the X(3872), we have studied the effects of the ${c}ar{c}$ charmonium core state coupling to the D0 $ar{D^{0}*}$ and D+ D−* molecule states. We determine the coupling strength so as to reproduce the observed mass of the the X(3872). The isospin symmetry breaking is introduced by the mass differences of the neutral and charged $ar{D*}}$ mesons. The obtained structure of the X(3872) is about 15% of ${c}ar{c}$ charmoniumu, 72% of the isoscalar D$ar{D*}}$ molecule and 13% of the isovector D$ar{D*}}$ molecule which explains observed properties of the X(3872) well.
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spelling doaj.art-6005e191b5e848e38a0a78819597f8982022-12-21T20:48:07ZengEDP SciencesEPJ Web of Conferences2100-014X2010-04-0130302610.1051/epjconf/20100303026Structure of the X(3872) and its Isospin Symmetry BreakingTakeuchi S.Takizawa M.In order to understand the structure of the X(3872), we have studied the effects of the ${c}ar{c}$ charmonium core state coupling to the D0 $ar{D^{0}*}$ and D+ D−* molecule states. We determine the coupling strength so as to reproduce the observed mass of the the X(3872). The isospin symmetry breaking is introduced by the mass differences of the neutral and charged $ar{D*}}$ mesons. The obtained structure of the X(3872) is about 15% of ${c}ar{c}$ charmoniumu, 72% of the isoscalar D$ar{D*}}$ molecule and 13% of the isovector D$ar{D*}}$ molecule which explains observed properties of the X(3872) well.http://dx.doi.org/10.1051/epjconf/20100303026
spellingShingle Takeuchi S.
Takizawa M.
Structure of the X(3872) and its Isospin Symmetry Breaking
EPJ Web of Conferences
title Structure of the X(3872) and its Isospin Symmetry Breaking
title_full Structure of the X(3872) and its Isospin Symmetry Breaking
title_fullStr Structure of the X(3872) and its Isospin Symmetry Breaking
title_full_unstemmed Structure of the X(3872) and its Isospin Symmetry Breaking
title_short Structure of the X(3872) and its Isospin Symmetry Breaking
title_sort structure of the x 3872 and its isospin symmetry breaking
url http://dx.doi.org/10.1051/epjconf/20100303026
work_keys_str_mv AT takeuchis structureofthex3872anditsisospinsymmetrybreaking
AT takizawam structureofthex3872anditsisospinsymmetrybreaking