Chinese Physics C > 1996, Vol. 20 > Issue(4): 363-368

Quark-Chiral Field interaction inSU(3) Model

Institute of High Energy Physics,The Chinese Academy of Sciences, Beijing 100039

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Abstract：
A quark-quark potential is derived from the linear expression of the Lagrangian Which is invariant under the SU(3) _L× SU(3) _Rinfinitesimal transformation,and further used to make a qualitative analysis on the Λ-N interaction.The result shows that the SU(3)chiral scalar fields are important in explaining the spin-dependence feature of the Λ-N interaction.

References

[1]

余友文、张宗烨、沈彭年等，高能物理与核物理，19（1995）441.[2]Howard Georgi,Weak Interactions and Moden Particle Theory.The Benjamin/Cummings Publishing Company,Inc.[3]F.Fernandez,A.Valcarce,U.Straub et al.,J.Phys.,G19（1993）2013.[4]P.M.M.Maessen,Th.A.Rijken,J.J.deSwart,Phys.Rev,C.40（1989）2226.[5]M.Oka,K.Shimizu,K.Yazaki,Nucl.Phys.,A464（1987）700.[6]ZhangZongye,A.Faessler,U.Straub et al.,Nucl.Phys.,A578（1994）573.[7]G.Alexander,U.Karshon,A.Shapira et al.,Phys.Rev,173（1968）1452;B.Sechi-Zorn,B.Kehoe,J.Twitty et al.,Phys.Rev,175（1968）1735;J.A.Kadyk,G.Alexander,J.H.Chan et al.,Nucl.Phys.,B27（1971）13.

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Zhang Zongye, Yu Youwen and Dai Lianrong. Quark-Chiral Field interaction in SU(3) Model[J]. Chinese Physics C, 1996, 20(4): 363-368.

Zhang Zongye, Yu Youwen and Dai Lianrong. Quark-Chiral Field interaction in SU(3) Model[J]. Chinese Physics C, 1996, 20(4): 363-368. shu

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Received: 1900-01-01
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

Quark-Chiral Field interaction inSU(3) Model

Corresponding author:Zhang Zongye,

Institute of High Energy Physics,The Chinese Academy of Sciences, Beijing 100039

Received Date:1900-01-01
Accepted Date:1900-01-01
Available Online:1996-04-05

Abstract:A quark-quark potential is derived from the linear expression of the Lagrangian Which is invariant under theSU(3)_L×SU(3)_Rinfinitesimal transformation,and further used to make a qualitative analysis on the Λ-N interaction.The result shows that theSU(3)chiral scalar fields are important in explaining the spin-dependence feature of the Λ-N interaction.