Self-breaking of the standard model gauge symmetry

被引:96
作者
Arkani-Hamed, N [1 ]
Cheng, HC
Dobrescu, BA
Hall, LJ
机构
[1] Univ Calif Berkeley, Lawrence Berkeley Lab, Theoret Phys Grp, Berkeley, CA 94720 USA
[2] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[3] Univ Chicago, Enrico Fermi Inst, Chicago, IL 60637 USA
[4] Fermi Natl Accelerator Lab, Batavia, IL 60510 USA
来源
PHYSICAL REVIEW D | 2000年 / 62卷 / 09期
关键词
D O I
10.1103/PhysRevD.62.096006
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
If the gauge fields of the standard model propagate in TeV-size extra dimensions, they rapidly become strongly coupled and can form scalar bound states of quarks and leptons. If the quarks and leptons of the third generation propagate in 6 or 8 dimensions, we argue that the most tightly bound scalar is a composite of top quarks, having the quantum numbers of the Higgs doublet and a large coupling to the top quark. In the case where the gauge bosons propagate in a bulk of a certain volume, this composite Higgs doublet can successfully trigger electroweak symmetry breaking. The mass of the top quark is correctly predicted to within 20%, without the need to add a fundamental Yukawa interaction, and the Higgs boson mass is predicted to lie in the range 165-230 GeV. In addition to the Higgs boson, there may be a few other scalar composites sufficiently light to be observed at upcoming collider experiments.
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页码:1 / 12
页数:12
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