THE <EM>SU</EM>(6) “UNITARY ENERGY BAND” STRUCTURE IN THE TRIBARYON SYSTEM

ZHANG YU-SHUN; LI YANG-GUO; WANG WEI-WEI; CHEN XIAO-TIAN; RUAN TU-NAN

近期发现有不法分子冒充我刊与作者联系，借此进行欺诈等不法行为，请广大作者加以鉴别，如遇诈骗行为，请第一时间与我刊编辑部联系确认（《中国物理C》（英文）编辑部电话：010-88235947,010-88236950），并作报警处理。

本刊再次郑重声明：

（1）本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137

（2）本刊采编系统作者中心是投稿的唯一路径，该系统为ScholarOne远程稿件采编系统，仅在本刊投稿网网址（https://mc03.manuscriptcentral.com/cpc）设有登录入口。本刊不接受其他方式的投稿，如打印稿投稿、E-mail信箱投稿等，若以此种方式接收投稿均为假冒。

（3）所有投稿均需经过严格的同行评议、编辑加工后方可发表，本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿，并收取发表费用，均为假冒。

《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 1981, Vol. 5> Issue(5) : 521-530

THE SU(6) “UNITARY ENERGY BAND” STRUCTURE IN THE TRIBARYON SYSTEM

Abstract
HTML
Reference
Related

PDF

Abstract：
A picture of the tribaryon system is proposed based on the papers [1—3]. It is considered that proton, neutron and A hyperon from the basic particles of SU(3) group and form the basic particles of SU(6) group on account for spin. It turns out that there exist "unitary energy band" structure in the tribaryon system. From the mass formula of T₃³ breaking, one can find that the SU(6) symmetry gives the mass relations between different spin levels of the same strangeness analog states. Finally, simple calculations are made and tbere is no discrepancy between tbe results and the experimental data.

References

[1]	陈晓天、阮图南、张禹顺、李扬国,9eientia 8iniaa, 4(1980), 823;高能物理与核物理,4(1980), 445,[2] 张禹顺、王潍潍、陈晓天、李扬国、阮图南,高能物理与核物理,5(1981), 149.[3] 王潍潍、张禹顺、李扬国、陈晓夭、阮图南,高能物理与核物理,5(1981), 441.[4] S. Fiarman and S. S. Hanna, Nucl. Phys., A251(1976), 1.

[1]	YU Guo-Wei , FANG Shuang-Shi , LI Wei-Guo , WU Ning . SU(3) Flavor Symmetry Breaking in J/ψ →baryon-antibaryon. Chinese Physics C, 2006, 30(7): 599-602.
[2]	WANG Hong-Min , ZHANG Ben-Ai . Contribution of SU(6) Breaking Effects in the Nucleon Form Factors. Chinese Physics C, 2004, 28(8): 821-826.
[3]	Dai Guangxi , Wu Heyu , Fu Yanbiao , Duan Limin , He Zhiyong , Li Zuyu , Zhang Baoguo , Liu Guoxing . Two Modes in Three-fold Fragmentation of hot Nuclei. Chinese Physics C, 1999, 23(1): 51-58.
[4]	Xie Wenfang . Q-Effect of Structures of 3-Particle Systems. Chinese Physics C, 1997, 21(5): 465-469.
[5]	Dai Guangxi , Wu Heyu , Duan Limin , Li Zuyu , He Zhiyong , Luo Qingzheng , Zhang Baoguo . The Threefold Fragmentation of Hot Nuclei With Medium Mass Number. Chinese Physics C, 1996, 20(7): 588-595.
[6]	HOU Yunzhi , GAO Lixin . SU(3)_f Predictions for Nonleptonic Decays of Charmless B-Flavoured Baryons. Chinese Physics C, 1993, 17(12): 1091-1101.
[7]	DUAN Yi-Wu . Three-Body Structure and Interparticle Correlations of the Doubly Λ Hypernucleus ΛΛ6He. Chinese Physics C, 1991, 15(10): 913-918.
[8]	XIE Shu-Qin , ZHANG Qi-Ren . AN SU(3) SYMMETRY IN THE TRIBARYON SYSTEM. Chinese Physics C, 1988, 12(5): 673-682.
[9]	LI Xian-Yin , YAO Shi-Huai . A MAPPING BETWEEN THE SU₆ SUBSPACE IN THE INTERACTING BOSON MODEL OF NUCLEI AND THE SU₆ SUBSPACE OF D.JANSSEN ET AL.. Chinese Physics C, 1985, 9(4): 476-482.
[10]	ZHU Pei-Yu , CAO Yu-Fang , WU You-Shi . SU(3) LIMIT OF U(6/20) SUPERSYMMETRY IN NUCLEI. Chinese Physics C, 1985, 9(5): 542-545.
[11]	YAO Nai-Guo , YU Zu-Rong . THE PHYSICAL BASES OF THE THREE PARTICLE SYSTEM. Chinese Physics C, 1984, 8(6): 720-731.
[12]	JIANG Xiang-Dong . AN SU(6) GRAND UNIFIED MODEL. Chinese Physics C, 1984, 8(3): 272-278.
[13]	YU Zu-Rong . TRANSFORMATION COEFFICIENTS BETWEEN SO(6) AND SU(4) GELFAND-ZETLIN STATES. Chinese Physics C, 1983, 7(1): 121-125.
[14]	WANG Wei-Wei , ZHANG Yu-Shun , LI YANG , RUAN Tu-Nan . UNITARY THEORY OF BARYON-SYSTEM. Chinese Physics C, 1983, 7(1): 57-66.
[15]	WANG Wei-Wei , ZHANG Yu-Shun , PAN Ji-Zhi , WANG Ru-Ling . THE SPECTROSCOPY OF FOUR-BARYON SYSTEM. Chinese Physics C, 1983, 7(1): 109-113.
[16]	ZHANG QI-REN , XIE SHU-QIN . BARYONIUM AND THE HIGH DIMENSIONAL REPRESENTATIONS OF SU(3). Chinese Physics C, 1982, 6(6): 732-736.
[17]	WANG WEI-WEI , ZHANG YU-SHUN , LI YANG-GUO , CHEN XIAO-TIAN , RUAN TU-NAN . THE “UNIRARY ENERGY BAND” STRUCTURE IN THE BARYON-ANTIBARYON SYSTEN. Chinese Physics C, 1981, 5(4): 441-451.
[18]	ZHANG YU-SHUN , WANG WEI-WEI , LI YANG-GUO , CHEN XIAO-TIAN , RUAN TU-NAN . SU₆ UNITARY SYMMETRY IN DIBARYON SYSTEMS. Chinese Physics C, 1981, 5(2): 149-156.
[19]	Chen Xiao-tian , Yuan Tu-nan , Zhang Yu-shun , Li Yang-guo . UNITARY SYMMETRY IN BARYON-ANTIBARYON SYSTEMS. Chinese Physics C, 1980, 4(4): 445-454.
[20]	LI BING-AN , RUAN TONG-ZE . WAVE FUNCTIONS WITHOUT SU₆ SYMMETRY IN THE STRATON MODEL AND THEIR APPLICATIONS. Chinese Physics C, 1979, 3(1): 1-18.

Access

Get Citation

ZHANG YU-SHUN, LI YANG-GUO, WANG WEI-WEI, CHEN XIAO-TIAN and RUAN TU-NAN. THE SU(6) “UNITARY ENERGY BAND” STRUCTURE IN THE TRIBARYON SYSTEM[J]. Chinese Physics C, 1981, 5(5): 521-530.

ZHANG YU-SHUN, LI YANG-GUO, WANG WEI-WEI, CHEN XIAO-TIAN and RUAN TU-NAN. THE SU(6) “UNITARY ENERGY BAND” STRUCTURE IN THE TRIBARYON SYSTEM[J]. Chinese Physics C, 1981, 5(5): 521-530. shu

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1979-12-20
Revised: 1900-01-01

Article Metric

Article Views(2278)
PDF Downloads(245)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

THE SU(6) “UNITARY ENERGY BAND” STRUCTURE IN THE TRIBARYON SYSTEM

Received Date: 1979-12-20
Accepted Date: 1900-01-01
Available Online: 1981-10-05

Abstract: A picture of the tribaryon system is proposed based on the papers [1—3]. It is considered that proton, neutron and A hyperon from the basic particles of SU(3) group and form the basic particles of SU(6) group on account for spin. It turns out that there exist "unitary energy band" structure in the tribaryon system. From the mass formula of T₃³ breaking, one can find that the SU(6) symmetry gives the mass relations between different spin levels of the same strangeness analog states. Finally, simple calculations are made and tbere is no discrepancy between tbe results and the experimental data.