Study of Doubly Heavy Baryon Spectrum via QCD Sum Rules
In this work, we calculate the mass spectrum of doubly heavy baryons with the diquaxk model in terms of the QCD sum rules. The interpolating currents are composed of a heavy diquaxk field and a light quark field. Contributions of the operators up to dimension six are taken into account in the operat...
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Published in | Communications in theoretical physics Vol. 57; no. 3; pp. 435 - 444 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
01.03.2012
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ISSN | 0253-6102 |
DOI | 10.1088/0253-6102/57/3/15 |
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Abstract | In this work, we calculate the mass spectrum of doubly heavy baryons with the diquaxk model in terms of the QCD sum rules. The interpolating currents are composed of a heavy diquaxk field and a light quark field. Contributions of the operators up to dimension six are taken into account in the operator product expansion. Within a reasonable error tolerance, our numerical results axe compatible with other theoretical predictions. This indicates that the diquaxk picture reflects the reality and is applicable to the study of doubly heavy baryons. |
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AbstractList | In this work, we calculate the mass spectrum of doubly heavy baryons with the diquaxk model in terms of the QCD sum rules. The interpolating currents are composed of a heavy diquaxk field and a light quark field. Contributions of the operators up to dimension six are taken into account in the operator product expansion. Within a reasonable error tolerance, our numerical results axe compatible with other theoretical predictions. This indicates that the diquaxk picture reflects the reality and is applicable to the study of doubly heavy baryons. In this work, we calculate the mass spectrum of doubly heavy baryonswith the diquark model in terms of the QCD sum rules. The interpolating currents are composed of a heavy diquark Held and a light quark Geld. Contributions of the operators up to dimension six are taken into account in the operator product expansion. Within a reasonable error tolerance, our numerical results are compatible with other theoretical predictions. This indicates that the diquark picture reflects the reality and is applicable to the study of doubly heavy baryons. |
Author | TANG Liang YUAN Xu-Hao QIAO Cong-Feng LI Xue-Qian |
AuthorAffiliation | School of Physics, Nankai University, Tianjin 300071, China Department of Physics, Graduate University, Chinese Academy of Sciences, Beijing 100049, China |
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CitedBy_id | crossref_primary_10_1103_PhysRevD_96_114006 crossref_primary_10_1103_PhysRevD_90_094507 crossref_primary_10_1088_1361_6471_aafffc crossref_primary_10_1016_j_physletb_2016_01_011 crossref_primary_10_1103_PhysRevD_95_116005 crossref_primary_10_1103_PhysRevD_103_114004 crossref_primary_10_1103_PhysRevD_107_074010 crossref_primary_10_1140_epjp_s13360_024_05697_9 crossref_primary_10_1140_epjc_s10052_017_4688_x crossref_primary_10_1140_epjc_s10052_017_5447_8 crossref_primary_10_1103_PhysRevD_97_094006 crossref_primary_10_1103_PhysRevD_99_073006 crossref_primary_10_1140_epjc_s10052_024_12426_0 crossref_primary_10_1140_epjc_s10052_022_10006_8 crossref_primary_10_1103_PhysRevD_97_054008 crossref_primary_10_1142_S0217732323500529 crossref_primary_10_1103_PhysRevD_105_014010 crossref_primary_10_1140_epjc_s10052_016_4379_z crossref_primary_10_1140_epja_s10050_023_01044_1 crossref_primary_10_1142_S0217751X23410038 crossref_primary_10_1103_PhysRevD_92_076008 crossref_primary_10_1016_j_physletb_2022_137404 crossref_primary_10_1140_epja_s10050_020_00049_4 crossref_primary_10_1103_PhysRevD_108_054015 crossref_primary_10_1103_PhysRevD_99_014018 |
Cites_doi | 10.1016/j.nuclphysbps.2005.01.058 10.1103/PhysRevD.77.014020 10.1016/j.physletb.2005.09.043 10.1088/0954-3899/39/1/015005 10.1088/0253-6102/54/2/23 10.1016/0550-3213(79)90022-1 10.1016/0370-2693(93)90090-5 10.1016/0550-3213(79)90023-3 10.1016/S0031-9163(64)92001-3 10.1088/0253-6102/55/6/20 10.1088/0253-6102/54/6/22 10.1007/BF01284677 10.1016/0370-1573(85)90065-1 10.1103/PhysRevLett.48.1653 10.1143/PTP.36.846 10.1016/j.physletb.2010.09.051 10.1016/j.physrep.2004.11.005 10.1103/PhysRevD.66.034030 10.1103/PhysRevD.74.011103 10.1103/PhysRevD.66.014008 10.1088/0954-3899/37/7A/075021 10.1103/PhysRevD.62.054024 10.1103/PhysRevD.49.555 10.1103/PhysRevD.78.094007 10.1103/PhysRevLett.89.112001 10.1016/j.nuclphysbps.2010.10.068 10.1007/BF02894866 10.1103/PhysRevLett.97.162001 10.1103/PhysRevD.70.094004 10.1070/PU2002v045n05ABEH000958 10.1016/j.nuclphysbps.2010.10.078 10.1016/j.physletb.2005.05.043 |
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Notes | 11-2592/O3 In this work, we calculate the mass spectrum of doubly heavy baryons with the diquaxk model in terms of the QCD sum rules. The interpolating currents are composed of a heavy diquaxk field and a light quark field. Contributions of the operators up to dimension six are taken into account in the operator product expansion. Within a reasonable error tolerance, our numerical results axe compatible with other theoretical predictions. This indicates that the diquaxk picture reflects the reality and is applicable to the study of doubly heavy baryons. baryons, QCD sun rules, other nonperturbative calculation ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
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Snippet | In this work, we calculate the mass spectrum of doubly heavy baryons with the diquaxk model in terms of the QCD sum rules. The interpolating currents are... In this work, we calculate the mass spectrum of doubly heavy baryonswith the diquark model in terms of the QCD sum rules. The interpolating currents are... |
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SubjectTerms | Baryons Compatibility Mathematical models Operators Permissible error QCD求和规则 Quantum chromodynamics Sum rules Tolerances 插值 计算结果 误差范围 质谱 轻夸克 运营商 重子谱 |
Title | Study of Doubly Heavy Baryon Spectrum via QCD Sum Rules |
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