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Doublet–triplet splitting problem
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Doublet–triplet splitting problem : ウィキペディア英語版
Doublet–triplet splitting problem
In particle physics, the doublet–triplet (splitting) problem is a problem of ''some'' Grand Unified Theories, such as SU(5), SO(10), E_6. Grand unified theories predict Higgs bosons (doublets of SU(2)) arise from representations of the unified group that contain other states, in particular, states that are triplets of color. The primary problem with these color triplet Higgs, is that they can mediate proton decay in supersymmetric theories that are only suppressed by two powers of GUT scale (i.e. they are dimension 5 supersymmetric operators). In addition to mediating proton decay, they alter gauge coupling unification. The doublet–triplet problem is the question 'what keeps the doublets light while the triplets are heavy?'
==Doublet–triplet splitting and the \mu-problem==
In 'minimal' SU(5), the way one accomplishes doublet–triplet splitting is through a combination of interactions
\int d^2\theta \; \lambda H_ + \mu H_
where \Sigma is an adjoint of SU(5) and is traceless. When \Sigma acquires a vacuum expectation value
\langle \Sigma\rangle = \rm(2, 2, 2, -3, -3) f
that breaks SU(5) to the Standard Model gauge symmetry the Higgs doublets and triplets acquire a mass
\int d^2\theta \; (2 \lambda f + \mu) H_}H_2
Since f is at the GUT scale ( 10^ GeV) and the Higgs doublets need to have a weak scale mass (100 GeV), this requires
\mu \sim 3 \lambda f \pm 100 \mbox.
So to solve this doublet–triplet splitting problem requires a tuning of the two terms to within one part in 10^.
This is also why the mu problem of the MSSM (i.e. why are the Higgs doublets so light) and doublet–triplet splitting are so closely intertwined.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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