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

LI BING-AN; RUAN TONG-ZE

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> 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

Abstract
HTML
Reference
Related

PDF

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.

[1]	HUI Ping . Higher Order RPA Calculation of the Glueball Wave Function in 2+1-D SU(2) LGT. Chinese Physics C, 2005, 29(4): 345-349.
[2]	BAI Hong-Bo , ZHANG Jin-Fu , ZHOU Xian-Rong . Energy Level Statistics of the SO(6) Limit of Super-Symmetry U(6/4)in the IBFM. Chinese Physics C, 2005, 29(8): 752-756.
[3]	Hul Ping . (2+1)-D SU(3)0⁺⁺ Glueball Wavefunction. Chinese Physics C, 1999, 23(4): 340-346.
[4]	Hui Ping . Fifth Order Approximate Analytic Calculation of (2+1)-D SU(2) Vacuum Wavefunction. Chinese Physics C, 1998, 22(4): 322-325.
[5]	Hui Ping , Chen Qizhou . Fourth Order Approximate Analytic Calculation of (2+1)-D SU(2) Vacuum Wavefunction. Chinese Physics C, 1995, 19(9): 820-825.
[6]	Chen Qizhou , Li Lei , Li Zhibing , Guo Shuohong . Vacuum Wave Function Study of 2+1 Dimensional SU(2) Gauge Field. Chinese Physics C, 1994, 18(5): 417-423.
[7]	Chen Qizhou , Li Zhibing , Li Lei , Guo Shuohong . Infrared Vacuum Wavefunction of (2+1)-Dimensional SU(2) Gauge Field. Chinese Physics C, 1994, 18(1): 37-42.
[8]	LI Guang-Hua , HE Hui-Yong . Calculating on Wavefunctions of the Ground State Band for the Strong Coupling SU(3) Limit in IBM4. Chinese Physics C, 1992, 16(3): 278-284.
[9]	BAO Shu-Qing , XUE Xiao-Zhou . ANALYSIS OF THE CHIRALITY IN SU(N) CRAND UNIFIED PREON MODELS. Chinese Physics C, 1990, 14(12): 1073-1080.
[10]	XU Fu-Xin , CUI Ke-Fan . TRACELESS OPERATORS AND SO₆ WAVE FUNCTIONS OF sd BOSONS. Chinese Physics C, 1986, 10(3): 343-348.
[11]	ZHU Pei-Yu , CAO Yu-Fang , WU You-Shi . THE SPIN (6) LIMIT OF INTERACTING BOSON-FERMION MODEL Ⅱ. Chinese Physics C, 1985, 9(2): 154-160.
[12]	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.
[13]	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.
[14]	JIANG Xiang-Dong . AN SU(6) GRAND UNIFIED MODEL. Chinese Physics C, 1984, 8(3): 272-278.
[15]	SUN HONG-ZHOU , HAN QI-ZHI . THE U(6/4) SUPERSYMMETRY IN COMPLEX NUCLEAR SPECTRA. Chinese Physics C, 1982, 6(4): 401-408.
[16]	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.
[17]	CHEN BAO-QIU , LI ZHU-XIA , JIN KING-NAN . ON THE RELATIVE WAVE FUNCTION OF α-AND d-CLUSTERS IN ⁶Li. Chinese Physics C, 1979, 3(2): 226-231.
[18]	GAO CHUNG-SHOU . SU（4）×S₃^{^α} SCHEME OF STRATON MODEL AND THE NEWLY DISCOVERED HEAVY PARTICLE γ（9.5）. Chinese Physics C, 1978, 2(5): 394-402.
[19]	LI TIE-ZHONG . NEW PARTICLES γ NEAR 9.5GeV AND SU(5) EXTENSION OF THE STRATON MODEL. Chinese Physics C, 1978, 2(2): 183-187.
[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.

Access

Get Citation

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

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1976-11-17
Revised: 1900-01-01

Article Metric

Article Views(1759)
PDF Downloads(261)
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

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.