ELECTRO-WEAK UNIFIED THEORY——A MODEL IN <EM>SU</EM>(3)×<EM>U</EM>(1)

CHEN Shi-Hao

Chinese Physics C> 1985, Vol. 9> Issue(6) : 679-686

ELECTRO-WEAK UNIFIED THEORY——A MODEL IN SU(3)×U(1)

CHEN Shi-Hao ^,

Northeast Teachers' University

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Abstract：
An electro-weak unified model based on SU(3)×U(1) group is suggested, which is left-right symmetrical and assuming the same interactions of neutrinos (or antineutrinos) with charge leptons and antileptons before spontaneous symmetry breaking. It is anomaly free and sin²θ_w1/4 can be drived. The difference between the model and the Weinberg-Salam model is very small in the low energy range. The lepton number is generalized to the lepton charge. It is proved that only lepton charge is strictly conserved and the individual conservation of the lepton number of every generation of leptons hold only approximately. The quarks have not only baryon number and charge but also lepton charge. This model predicts processes μ_R→e_R+ν_eL+ν_μR, e^－+e^－→μ^－+μ^－, etc.

References

[1]

S. Weinberg, Phys. Rev. Lett. 19 (1967F 1264; S. Salam, Proc. of the 8th Nobel Symposinm,Stockholm, 1968; S. L. Glashow, J. Iliopoulos and L. Maiani, Phys. Rev., D2 (1970), 1285.[2] Phys. Today, 36, 11 (1983) 17. G. Arnison et al., Phys. Lett., 126B (1983), 398; 129B (1983).273; P. Bagnala et al., Phys. Lett., 129B(1983), 130.[3] B. W. Lee and S. Weinberg, Phys. Rev. Left.. 38 (1977), 1237; B. W. Lee and R.E. Shrock, Phys.Rev., 17D (l978), 2410; G. Segre md J. Weyers, Phys. Lett., 65B (1976), 243; P. Langagker and G. Segre,Phys. Rev. Lett.; 39(2977), 259; F. Buccella et al., Phys. Rev. Lett., 40 (1973); 1475;M. Yoshimura, Prog. Theor. Phys., 57 (1977), 237; K. Ishikawa et al, Prog. Theor. Phys, 58 (1977), 1256; T. Moriya,Prog.. Theor. Phys., 59(1978), 2028; H. Komatsu, Prog. Theor. Phys.,59(1978), 2013; C. H: Albright et al., Nucl. Phys., B86 (1975), 535; J. Schechter and Y. Ueda, Phys. Rev., D8 (1973 ), 484; M. Singer and K. S. Viswanatfian, Phys. Rev., D28 (1983) , 1721; M. Singer et al., Phys. Rev., D22 (1980) , 738.[4] K. C. Chou and C. S. Gao, SLAGPUB-2445 (1999); Scientia Sinca, 23 (1980), 566[5] Y. Ne'eman, Phys. Lett., 81B (19791, 190; D. B. Fairlie, Phys. Lett., 82b (1979), 97.

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[2]	HU Lian , HUI Ping , CHEN Qi-Zhou . Glueball Masses of the 0⁺⁺ and 0^－－ in 3+1-D SU(3) LGT. Chinese Physics C, 2002, 26(8): 773-778.
[3]	HUI Ping , CHEN QiZhou . 0⁺⁺ Glueball Mass in 2+1-D SU(3) LGT. Chinese Physics C, 2000, 24(9): 805-809.
[4]	CHEN FengZhi , WANG Ping . An SU (3)_L×U(1)_X Electroweak Model. Chinese Physics C, 2000, 24(11): 985-990.
[5]	Hul Ping . (2+1)-D SU(3)0⁺⁺ Glueball Wavefunction. Chinese Physics C, 1999, 23(4): 340-346.
[6]	Chen Fengzhi , Wang Ping . SU(3)_L×U(1)_X Model and a New Candidate for Dark Matter. Chinese Physics C, 1999, 23(11): 1062-1065.
[7]	Liu Yaoyang , Sun Lazhen , Jiang Xiangdong . SU(3)_C×SU(2)_I×U(1)_Y Theory of Composite Leptons. Chinese Physics C, 1998, 22(11): 996-1003.
[8]	Chen Qizhou , Fang Xiyan , Guo Shouhong . Calculation of Vacuum State for 2+1-Dimensional SU(3) Lattice Gauge Theory. Chinese Physics C, 1995, 19(5): 398-404.
[9]	Chen Qizhou , Fang Xiyan , Guo Shouhong . Calculation of Vacuum State for 2+1-Dimensional SU(3) Lattice Gauge Theory. Chinese Physics C, 1995, 19(S3): 265-272.
[10]	CHEN Feng-Zhi . SU(23) Grand Unified Model. Chinese Physics C, 1993, 17(3): 222-226.
[11]	PAN Feng . Vector Coherent State Representations of SU₃ in U₁ U₁ Basis. Chinese Physics C, 1991, 15(1): 80-86.
[12]	Liu Jinming , Zheng Weihong , Guo Shuohong . The Mass Gap in 2 + 1 Dimensional SU(3) Lattice Gauge Theory. Chinese Physics C, 1988, 12(S2): 137-142.
[13]	LIU Jin-Ming , ZHENG Wei-Hong , GUO Shuo-Hong . THE MASS GAP IN 2+1 DIMENSIONAL SU(3) LATTICE CAUGE THEORY. Chinese Physics C, 1988, 12(3): 420-424.
[14]	CHEN Tian-Lun , Zhou Hong-Mo , LI Tie-Zong , XIAN Ding-Chang , ZHENG Xi-Te . VARIATIONAL ANALYSIS OF THE SU(3) LATTICE GAUGE THEORY. Chinese Physics C, 1984, 8(5): 653-656.
[15]	JIANG Xiang-Dong . AN SU(6) GRAND UNIFIED MODEL. Chinese Physics C, 1984, 8(3): 272-278.
[16]	XU De-Zhi . AN SU(4)×SU(2)×U(1) UNIFIED MODEL. Chinese Physics C, 1983, 7(1): 13-19.
[17]	MA ZHONG-QI , DONG FANG-XIAO , YUE ZONG-WU , ZHOU XIAN-JIAN , XUE PEI-YOU . DISCUSSION OF A SU(2)×U(1)×S₃ MODEL WITH TWO HIGGS DOUBLETS AND CALCULATION OF CABIBBO-LIKE-PARAMETERS. Chinese Physics C, 1981, 5(3): 298-306.
[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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CHEN Shi-Hao. ELECTRO-WEAK UNIFIED THEORY——A MODEL IN SU(3)×U(1)[J]. Chinese Physics C, 1985, 9(6): 679-686.

CHEN Shi-Hao. ELECTRO-WEAK UNIFIED THEORY——A MODEL IN SU(3)×U(1)[J]. Chinese Physics C, 1985, 9(6): 679-686. 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

ELECTRO-WEAK UNIFIED THEORY——A MODEL IN SU(3)×U(1)

CHEN Shi-Hao ^,

Corresponding author: CHEN Shi-Hao,

Northeast Teachers' University

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1985-12-05

Abstract: An electro-weak unified model based on SU(3)×U(1) group is suggested, which is left-right symmetrical and assuming the same interactions of neutrinos (or antineutrinos) with charge leptons and antileptons before spontaneous symmetry breaking. It is anomaly free and sin²θ_w1/4 can be drived. The difference between the model and the Weinberg-Salam model is very small in the low energy range. The lepton number is generalized to the lepton charge. It is proved that only lepton charge is strictly conserved and the individual conservation of the lepton number of every generation of leptons hold only approximately. The quarks have not only baryon number and charge but also lepton charge. This model predicts processes μ_R→e_R+ν_eL+ν_μR, e^－+e^－→μ^－+μ^－, etc.