Closing the SU(3)L⊗U(1)X symmetry at the electroweak scale

被引:40
作者
Dias, Alex G.
Montero, J. C.
Pleitez, V.
机构
[1] Univ Sao Paulo, Inst Fis, BR-05315970 Sao Paulo, Brazil
[2] Univ Estadual Paulista, Inst Fis Teor, BR-01405000 Sao Paulo, Brazil
来源
PHYSICAL REVIEW D | 2006年 / 73卷 / 11期
关键词
D O I
10.1103/PhysRevD.73.113004
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We show that some models with SU(3)(C)circle times SU(3)(L)circle times U(1)(X) gauge symmetry can be realized at the electroweak scale and that this is a consequence of an approximate global SU(2)(L+R) symmetry. This symmetry implies a condition among the vacuum expectation value of one of the neutral Higgs scalars, the U(1)(X)'s coupling constant, g(X), the sine of the weak mixing angle sin theta(W), and the mass of the W boson, M-W. In the limit in which this symmetry is valid it avoids the tree level mixing of the Z boson of the standard model with the extra Z(') boson. We have verified that the oblique T parameter is within the allowed range indicating that the radiative corrections that induce such a mixing at the 1-loop level are small. We also show that a SU(3)(L+R) custodial symmetry implies that in some of the models we have to include sterile (singlets of the 3-3-1 symmetry) right-handed neutrinos with Majorana masses, since the seesaw mechanism is mandatory to obtain light active neutrinos. Moreover, the approximate SU(2)(L+R)subset of SU(3)(L+R) symmetry implies that the extra nonstandard particles of these 3-3-1 models can be considerably lighter than it had been thought before so that new physics can be really just around the corner.
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页数:15
相关论文
共 72 条
[1]   Search for doubly charged Higgs boson pair production in the decay to μ+μ+μ-μ- in p(p)over-bar collisions at √s=1.96 TeV -: art. no. 141801 [J].
Abazov, VM ;
Abbott, B ;
Abolins, M ;
Acharya, BS ;
Adams, DL ;
Adams, M ;
Adams, T ;
Agelou, M ;
Agram, JL ;
Ahmed, SN ;
Ahn, SH ;
Alexeev, GD ;
Alkhazov, G ;
Alton, A ;
Alverson, G ;
Alves, GA ;
Anderson, S ;
Andrieu, B ;
Arnoud, Y ;
Askew, A ;
Åsman, B ;
Autermann, C ;
Avila, C ;
Babukhadia, L ;
Bacon, TC ;
Baden, A ;
Baffioni, S ;
Baldin, B ;
Balm, PW ;
Banerjee, S ;
Barberis, E ;
Bargassa, P ;
Baringer, P ;
Barnes, C ;
Barreto, J ;
Bartlett, JF ;
Bassler, U ;
Bauer, D ;
Bean, A ;
Beauceron, S ;
Beaudette, F ;
Begel, M ;
Beri, SB ;
Bernardi, G ;
Bertram, I ;
Besançon, M ;
Besson, A ;
Beuselinck, R ;
Bezzubov, VA ;
Bhat, PC .
PHYSICAL REVIEW LETTERS, 2004, 93 (14) :141801-1
[2]   R(b), R(c) and jet distributions at the Tevatron in a model with an extra vector boson [J].
Altarelli, G ;
DiBartolomeo, N ;
Feruglio, F ;
Gatto, R ;
Mangano, ML .
PHYSICS LETTERS B, 1996, 375 (1-4) :292-300
[3]  
[Anonymous], HEPPH9504216
[4]  
[Anonymous], 2005, EUR PHYS J C
[5]  
Antoniadis I, 2000, INT J MOD PHYS A, V15, P4237, DOI 10.1142/S0217751X00002172
[6]   The littlest Higgs [J].
Arkani-Hamed, N ;
Cohen, AG ;
Katz, E ;
Nelson, AE .
JOURNAL OF HIGH ENERGY PHYSICS, 2002, (07) :929-944
[7]   Implications of generalized Z-Z′ mixing [J].
Babu, KS ;
Kolda, C ;
March-Russell, J .
PHYSICAL REVIEW D, 1998, 57 (11) :6788-6792
[8]   Leptophobic U(1)'s and the R(b)-R(c) anomalies [J].
Babu, KS ;
Kolda, C ;
MarchRussell, J .
PHYSICAL REVIEW D, 1996, 54 (07) :4635-4647
[9]   Z′ gauge bosons at the Fermilab Tevatron -: art. no. 093009 [J].
Carena, M ;
Daleo, A ;
Dobrescu, BA ;
Tait, TMP .
PHYSICAL REVIEW D, 2004, 70 (09)
[10]   A Z' with enhanced couplings to quarks: A bridge from CERN LEP 1, SLC, and CDF to LEP 2 anomalies [J].
Chiappetta, P ;
Layssac, J ;
Renard, FM ;
Verzegnassi, C .
PHYSICAL REVIEW D, 1996, 54 (01) :789-797