WAVE FUNCTIONS WITHOUT <EM>SU</EM><SUB>6</SUB> SYMMETRY IN THE STRATON MODEL AND THEIR APPLICATIONS

LI BING-AN; RUAN TONG-ZE

Chinese Physics C> 1979, Vol. 3> Issue(1) : 1-18

WAVE FUNCTIONS WITHOUT SU₆ SYMMETRY IN THE STRATON MODEL AND THEIR APPLICATIONS

LI BING-AN ,
RUAN TONG-ZE

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Abstract：
On the basis of the straton model^[1],using the general groundstate wave functionsof mesons and baryons given in ref.[2],we have constructed under some specific as-sumptions the meson and baryon wave functions without SU₆ symmetry.We applythese wave functions to explain the mesonic and baryonic properties of the electroma-gnetic and weak interactions;many results obtained are in agreement with the experi-ments.By using the 1/2⁺-baryon wave functions without SU₆ symmetry,we obtain ananomalous magnetic moment for the proton.There is no need to introduce an ano-malous magnetic moment for the straton in the effective Hamiltonian of electromag-netic interaction between stratons.Similarly,the magnetic moment of the neutroncan also be explained.

References

[1]

1966年北京署期物理讨论会上北京基本粒子理论组的论文.[2] 李炳安，物理学报，24 (1975), 21.[3] 李炳安，物理学报，24 (1975), 124;李炳安、阮同泽，物理学报,25 (1976), 331;阮同泽、李炳安，物理学报,26 (1977), 397.[4] 中国科学院原子能研究所基本粒子理论组，原子能,1966,3, 167.[5] C. J. Bebek et al., Phys. Rev., D13 (1966), 25.[6] W. Bartel et al., Nucl. Phys., B58 (1973), 429.[7] R. Wilson, Proceedings of the 1971 International Symposium on Electron and Photon In-teractions at High Energy, 97.[8] Particle, Data Group. Rev. Mod. Phys., 48 (1976), 51.[9] M. Gourdin P.H.Salin Nuovo Cimento, 27 (1963), 183;28 (1963), 1294.[10] P. Pillantini et al., Nucl. Phys., B13 (1969), 320.[11] P. Noelle et al., Nucl. Phys., B26 (1971), 461.[12] R. L. Walker, 4th International Symposium on Electron and Photon Interactions at high energies(1969), 23.[13] G. Morpurgo, 14th International Conference on High-Energy Physics, Vienna (1968), 225.[14] L. Durand et al., Phys. Rev., 126 (1962), 1882.[15] C. Bemporad, Proceedings of the 1975 International Symposium on Lepton and Photon In-teractions at High Energies, 113.[16] D. H. Petkin, ibid., 571.[17] P. A. Schreiner, F. Von Hippel. Nucl. Phys., B58 (1973), 333.

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[20]	ELEMENTARY PARTICLE THEORY GROUP , DEPARTMENT OF PHYSICS , PEKING UNIVERSITY . AN SU（4）×S₃^a SCHEME OF THE STRATON MODEL. Chinese Physics C, 1978, 2(1): 1-9.

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LI BING-AN and RUAN TONG-ZE. WAVE FUNCTIONS WITHOUT SU₆ SYMMETRY IN THE STRATON MODEL AND THEIR APPLICATIONS[J]. Chinese Physics C, 1979, 3(1): 1-18.

LI BING-AN and RUAN TONG-ZE. WAVE FUNCTIONS WITHOUT SU₆ SYMMETRY IN THE STRATON MODEL AND THEIR APPLICATIONS[J]. Chinese Physics C, 1979, 3(1): 1-18. shu

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Received: 1976-11-17
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

WAVE FUNCTIONS WITHOUT SU₆ SYMMETRY IN THE STRATON MODEL AND THEIR APPLICATIONS

LI BING-AN
RUAN TONG-ZE

Received Date: 1976-11-17
Accepted Date: 1900-01-01
Available Online: 1979-02-05

Abstract: On the basis of the straton model^[1],using the general groundstate wave functionsof mesons and baryons given in ref.[2],we have constructed under some specific as-sumptions the meson and baryon wave functions without SU₆ symmetry.We applythese wave functions to explain the mesonic and baryonic properties of the electroma-gnetic and weak interactions;many results obtained are in agreement with the experi-ments.By using the 1/2⁺-baryon wave functions without SU₆ symmetry,we obtain ananomalous magnetic moment for the proton.There is no need to introduce an ano-malous magnetic moment for the straton in the effective Hamiltonian of electromag-netic interaction between stratons.Similarly,the magnetic moment of the neutroncan also be explained.