Spectrum and Bethe-Salpeter amplitudes of Ω baryons from lattice QCD
The Ω baryons with JP= 3/2^±, 1/2^± are studied on the lattice in the quenched approximation. Their mass levels are ordered as M3/2+〈 M3/2- 0≈M1/2-〈 M1/2+, as is expected from the constituent quark model. The mass values are also close to those of the four Ωstates observed in experiments. We calcula...
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Published in | Chinese physics C Vol. 40; no. 4; pp. 1 - 7 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
01.04.2016
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Subjects | |
Online Access | Get full text |
ISSN | 1674-1137 0254-3052 |
DOI | 10.1088/1674-1137/40/4/041001 |
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Summary: | The Ω baryons with JP= 3/2^±, 1/2^± are studied on the lattice in the quenched approximation. Their mass levels are ordered as M3/2+〈 M3/2- 0≈M1/2-〈 M1/2+, as is expected from the constituent quark model. The mass values are also close to those of the four Ωstates observed in experiments. We calculate the Bethe-Salpeter amplitudes of Ω(3/2^+) and Ω(1/2^+) and find there is a radial node for the Ω(1/2+) Bethe-Salpeter amplitude, which may imply that Ω(1/2+) is an orbital excitation of Ω baryons as a member of the(D, LN^P) =(70, 02^+) supermultiplet in the SU(6)×O(3) quark model description. Our results are helpful for identifying the quantum numbers of experimentally observed Ω states. |
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Bibliography: | Ω baryon, excited state, BS amplitude 11-5641/O4 Jian Liang, Ming Gong, Wei Sun,Chuan Liu,Ying Chen, Yu-Bin Liu, Wei-Feng Qiu, Zhao-Feng Liu,Jian-Ping Ma, Jian-Bo Zhang( 1 Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China ;2 Theoretical Center for Science Facilities, Chinese Academy of Sciences, Beijing 100049, China ; 3 School of Physics, Peking University, Beijing 100871, China ; 4 School of Physics, Nankai University, Tianjin 300071, China; 5 Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100080, China ; 6 Department of Physics, Zhejiang University, Hangzhou 310027, China) The Ω baryons with JP= 3/2^±, 1/2^± are studied on the lattice in the quenched approximation. Their mass levels are ordered as M3/2+〈 M3/2- 0≈M1/2-〈 M1/2+, as is expected from the constituent quark model. The mass values are also close to those of the four Ωstates observed in experiments. We calculate the Bethe-Salpeter amplitudes of Ω(3/2^+) and Ω(1/2^+) and find there is a radial node for the Ω(1/2+) Bethe-Salpeter amplitude, which may imply that Ω(1/2+) is an orbital excitation of Ω baryons as a member of the(D, LN^P) =(70, 02^+) supermultiplet in the SU(6)×O(3) quark model description. Our results are helpful for identifying the quantum numbers of experimentally observed Ω states. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1674-1137 0254-3052 |
DOI: | 10.1088/1674-1137/40/4/041001 |