μB-driven electroweak symmetry breaking
We consider a scenario in which the dominant quartic coupling for the Higgs doublets arises from the F-term potential, rather than the conventional SU(2)L×U(1)YD-term potential, in supersymmetric theories. The quartic coupling arises from a superpotential interaction between the two Higgs doublets a...
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Published in | Physics letters. B Vol. 633; no. 4-5; pp. 573 - 582 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Amsterdam
Elsevier B.V
16.02.2006
Elsevier Science |
Subjects | |
Online Access | Get full text |
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Summary: | We consider a scenario in which the dominant quartic coupling for the Higgs doublets arises from the F-term potential, rather than the conventional SU(2)L×U(1)YD-term potential, in supersymmetric theories. The quartic coupling arises from a superpotential interaction between the two Higgs doublets and a singlet field, but unlike the case in the next-to-minimal supersymmetric standard model the singlet field is not responsible for the generation of the supersymmetric or holomorphic supersymmetry-breaking masses for the Higgs doublets. We find that this naturally leads to a deviation from the conventional picture of top–Yukawa driven electroweak symmetry breaking—electroweak symmetry breaking is triggered by the holomorphic supersymmetry breaking mass for the Higgs doublets (the μB term). This allows a significant improvement for fine-tuning in electroweak symmetry breaking, since the top squarks do not play a major role in raising the Higgs boson mass or in triggering electroweak symmetry breaking and thus can be light. The amount of fine-tuning is given by the squared ratio of the lightest Higgs boson mass to the charged Higgs boson mass, which can be made better than 20%. Solid implications of the scenario include a small value for tanβ, tanβ≲3, and relatively light top squarks. |
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ISSN: | 0370-2693 1873-2445 |
DOI: | 10.1016/j.physletb.2005.12.011 |