ΩN Bound State in SU(3) Quark Model

YU You-Wen; ZHANG Zong-Ye; LI Qiang-Bing

Chinese Physics C> 2002, Vol. 26> Issue(10) : 1041-1045

ΩN Bound State in SU(3) Quark Model

Institute of High Energy Physics,CAS,Beijing 100039,China

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Abstract：
The structures of (ΩN)_LST systems are studied in the SU(3) quark model,in which the coupling between quark antiquark and the meson fields is included. A resonating group method (RGM) calculation shows that (ΩN)0212 could be a bound state with considerably large binding energy,when the mechanism of s(s) annihilation to K* is considered.

References

[1]

Faexsler A.Lübeck G.Shimizu K. Phys. Rev.，1982,D26:32A02 ZHANG Zong-Ye.YU You-Wen. DAI Lien-Rong,HEP NP.1996,20(4):363 (in Chinese)(张宗烨，余友文，戴连荣.高能物理与核物理，1996,211(4):363)3 ZHANG Zong-Ye,YU You-Wen.SHEN Peng-Nian et al. Nucl，Phys .，1997,A625:594 Pavlopoulos P et al . Phys Lett .，1977,72B:415;Richter B et al.Phys. Lett., 1983.126B:284:Adicls I. et al.Phys. Lett.，1984,8138:2355 Angelopoulos A et al. Phys. Lett。1986,B178:441:Adiels L et al. Phys. Lett. ,1986,B182:4056 Green A M,Niskancn H A. Nucl. Phys,1984;A412:448:A430aU6;Niskanen J A.Green A M. Nucl.Phvs.，1984,A431:593;Green A M,Kuikka V,Niskancn J A. Nucl. Phys.，1985.A446:5437 Manryarm M.Ueda T. Pmg. Theor. Phys..1985,73:1211;1985,74:5268 Maruvarm M et al.Nucl. Phvs.，1987 , A473:649: Gutsche T,Maruyama. Faessler A. Nucl.Phys.1989 , A3115 : 7379 Dover.C B Gutsche T, Maruyama M，Faessler A. Prog. Part. Nucl.Phys.1992.29:8710 YU Y W ,ZHANG Z Y ,YUAN X Q .Commun.Theor.Phys.,1999,31:1;ZHANG Z Y et al.Phys.Rev.,2000,C61:065204 11 Anderson E et al.Phys.Lett.,1998,B433:209 12 YUYW ,WANGP ,ZHANG Z Y et al.Commun.Theor.Phys.,2001,35:553 13 Isgur N ,Karl G .Phys.Rev.,1978,D18:4187;Phys.Rev.,1979,D19:2653;CapstickS ,Isgur N .Phys.Rev.,1986,D34:280914 Glozman L Ya,Riska D O .Phys.Rep.,1996,268:263;Glozman L Ya,Rapp Z ,Plessas W et al.Phys.Rev.,1998,C57:340615 Yamamoto Y ,Bando H .Prog.Theor.Phys.Suppl.,1985,81:9

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[14]	BAO Shu-Qing . COMPLEMENTARITY IN SU(N) UNIFIED PREON MODELS. Chinese Physics C, 1989, 13(5): 393-402.
[15]	WANG Shun-Jin , CAO Jian-Min , XU Gong-Ou . CONTINUOUS VARIABLE REPRESENTATION OF ELLIOTT SU(3) MODEL. Chinese Physics C, 1987, 11(1): 111-119.
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[17]	CHEN Shi-Hao . ELECTRO-WEAK UNIFIED THEORY——A MODEL IN SU(3)×U(1). Chinese Physics C, 1985, 9(6): 679-686.
[18]	ZHOU GUANG-ZHAO , . SOME DISCUSSIONS ON THE SU(3)×U(1) ELECTRO-WEAK UNIFIED MODEL OF LEPTONS AND QUARKS. Chinese Physics C, 1981, 5(1): 39-46.
[19]	Zhou Guang-zhao , Gao Chong-shou . UNIFIED ELECTRO-WEAK MODEL IN SU (3). Chinese Physics C, 1980, 4(5): 609-622.
[20]	DONG FANG-XIAO , DU DONG-SHENG . SU_4×SU'₃MODEL AND γ-NEW PARTICLES. Chinese Physics C, 1979, 3(6): 788-790.

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YU You-Wen, ZHANG Zong-Ye and LI Qiang-Bing. ΩN Bound State in SU(3) Quark Model[J]. Chinese Physics C, 2002, 26(10): 1041-1045.

YU You-Wen, ZHANG Zong-Ye and LI Qiang-Bing. ΩN Bound State in SU(3) Quark Model[J]. Chinese Physics C, 2002, 26(10): 1041-1045. shu

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Received: 2001-12-19
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

ΩN Bound State in SU(3) Quark Model

Corresponding author: YU You-Wen,

Institute of High Energy Physics,CAS,Beijing 100039,China

Received Date: 2001-12-19
Accepted Date: 1900-01-01
Available Online: 2002-10-05

Abstract: The structures of (ΩN)_LST systems are studied in the SU(3) quark model,in which the coupling between quark antiquark and the meson fields is included. A resonating group method (RGM) calculation shows that (ΩN)0212 could be a bound state with considerably large binding energy,when the mechanism of s(s) annihilation to K* is considered.