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Doublet–triplet splitting problem

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In particle physics, the doublet–triplet (splitting) problem is a problem of some Grand Unified Theories, such as SU(5), SO(10), and E 6 {\displaystyle E_{6}} . Grand unified theories predict Higgs bosons (doublets of S U ( 2 ) {\displaystyle 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 μ-problem

In 'minimal' SU(5), the way one accomplishes doublet–triplet splitting is through a combination of interactions

∫ d 2 θ λ H 5 ¯ Σ H 5 + μ H 5 ¯ H 5 {\displaystyle \int d^{2}\theta \;\lambda H_{\bar {5}}\Sigma H_{5}+\mu H_{\bar {5}}H_{5}}

where Σ {\displaystyle \Sigma } is an adjoint of SU(5) and is traceless. When Σ {\displaystyle \Sigma } acquires a vacuum expectation value

⟨ Σ ⟩ = d i a g ( 2 , 2 , 2 , − 3 , − 3 ) f {\displaystyle \langle \Sigma \rangle ={\rm {{diag}(2,2,2,-3,-3)f}}}

that breaks SU(5) to the Standard Model gauge symmetry the Higgs doublets and triplets acquire a mass

∫ d 2 θ ( 2 λ f + μ ) H 3 ¯ H 3 + ( − 3 λ f + μ ) H 2 ¯ H 2 {\displaystyle \int d^{2}\theta \;(2\lambda f+\mu )H_{\bar {3}}H_{3}+(-3\lambda f+\mu )H_{\bar {2}}H_{2}}

Since f {\displaystyle f} is at the GUT scale ( 10 16 {\displaystyle 10^{16}} GeV) and the Higgs doublets need to have a weak scale mass (100 GeV), this requires

μ ∼ 3 λ f ± 100 GeV {\displaystyle \mu \sim 3\lambda f\pm 100{\mbox{GeV}}} .

So to solve this doublet–triplet splitting problem requires a tuning of the two terms to within one part in 10 14 {\displaystyle 10^{14}} . 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.

Solutions to the doublet-triplet splitting

The missing partner mechanism

One solution to the doublet–triplet splitting (DTS) in the context of supersymmetric S U ( 5 ) {\displaystyle SU(5)} proposed in and is called the missing partner mechanism (MPM). The main idea is that in addition to the usual fields there are two additional chiral super-fields Z 50 {\displaystyle Z_{50}} and Z 50 ¯ {\displaystyle Z_{\overline {50}}} . Note that 50 {\displaystyle {\mathbf {50} }} decomposes as follows under the SM gauge group:

50 → ( 1 , 1 , − 2 ) + ( 3 , 1 , − 1 3 ) + ( 3 ¯ , 2 , − 7 6 ) + ( 6 , 1 , 4 3 ) + ( 6 ¯ , 3 , − 1 3 ) + ( 8 , 2 , 1 2 ) {\displaystyle \mathbf {50} \rightarrow (\mathbf {1} ,\mathbf {1} ,-2)+(\mathbf {3} ,\mathbf {1} ,-{\frac {1}{3}})+({\overline {\mathbf {3} }},\mathbf {2} ,-{\frac {7}{6}})+(\mathbf {6} ,\mathbf {1} ,{\frac {4}{3}})+({\overline {\mathbf {6} }},\mathbf {3} ,-{\frac {1}{3}})+(\mathbf {8} ,\mathbf {2} ,{\frac {1}{2}})}

which contains no field that could couple to the S U ( 2 ) {\displaystyle SU(2)} doublets of H 5 ¯ {\displaystyle H_{\overline {5}}} or H 5 {\displaystyle H_{5}} . Due to group theoretical reasons S U ( 5 ) {\displaystyle SU(5)} has to be broken by a 75 {\displaystyle \mathbf {75} } instead of the usual 24 {\displaystyle \mathbf {24} } , at least at the renormalizable level. The superpotential then reads

W M P M = y 1 H 5 ¯ H 75 Z 50 + y 2 Z 50 ¯ H 75 H 5 + m 50 Z 50 Z 50 ¯ . {\displaystyle W_{MPM}=y_{1}H_{\overline {5}}H_{75}Z_{50}+y_{2}Z_{\overline {50}}H_{75}H_{5}+m_{50}Z_{50}Z_{\overline {50}}.}

After breaking to the SM the colour triplet can get super heavy, suppressing proton decay, while the SM Higgs does not. Note that nevertheless the SM Higgs will have to pick up a mass in order to reproduce the electroweak theory correctly.

Note that although solving the DTS problem the MPM tends to render models non-perturbative just above the GUT scale. This problem is addressed by the Double missing partner mechanism.

Dimopoulos–Wilczek mechanism

In an SO(10) theory, there is a potential solution to the doublet–triplet splitting problem known as the 'Dimopoulos–Wilczek' mechanism. In SO(10), the adjoint field, Σ {\displaystyle \Sigma } acquires a vacuum expectation value of the form

⟨ Σ ⟩ = diag ( i σ 2 f 3 , i σ 2 f 3 , i σ 2 f 3 , i σ 2 f 2 , i σ 2 f 2 ) {\displaystyle \langle \Sigma \rangle ={\mbox{diag}}(i\sigma _{2}f_{3},i\sigma _{2}f_{3},i\sigma _{2}f_{3},i\sigma _{2}f_{2},i\sigma _{2}f_{2})} .

f 2 {\displaystyle f_{2}} and f 3 {\displaystyle f_{3}} give masses to the Higgs doublet and triplet, respectively, and are independent of each other, because Σ {\displaystyle \Sigma } is traceless for any values they may have. If f 2 = 0 {\displaystyle f_{2}=0} , then the Higgs doublet remains massless. This is very similar to the way that doublet–triplet splitting is done in either higher-dimensional grand unified theories or string theory.

To arrange for the VEV to align along this direction (and still not mess up the other details of the model) often requires very contrived models, however.

Higgs representations in Grand Unified Theories

In SU(5):

5 → ( 1 , 2 ) 1 2 ⊕ ( 3 , 1 ) − 1 3 {\displaystyle 5\rightarrow (1,2)_{1 \over 2}\oplus (3,1)_{-{1 \over 3}}}
5 ¯ → ( 1 , 2 ) − 1 2 ⊕ ( 3 ¯ , 1 ) 1 3 {\displaystyle {\bar {5}}\rightarrow (1,2)_{-{1 \over 2}}\oplus ({\bar {3}},1)_{1 \over 3}}

In SO(10):

10 → ( 1 , 2 ) 1 2 ⊕ ( 1 , 2 ) − 1 2 ⊕ ( 3 , 1 ) − 1 3 ⊕ ( 3 ¯ , 1 ) 1 3 {\displaystyle 10\rightarrow (1,2)_{1 \over 2}\oplus (1,2)_{-{1 \over 2}}\oplus (3,1)_{-{1 \over 3}}\oplus ({\bar {3}},1)_{1 \over 3}}

Proton decay

Dimension 6 proton decay mediated by the triplet Higgs T ( 3 , 1 ) − 1 3 {\displaystyle T(3,1)_{-{\frac {1}{3}}}} and the anti-triplet Higgs T ¯ ( 3 ¯ , 1 ) 1 3 {\displaystyle {\bar {T}}({\bar {3}},1)_{\frac {1}{3}}} in S U ( 5 ) {\displaystyle SU(5)} GUT

Non-supersymmetric theories suffer from quartic radiative corrections to the mass squared of the electroweak Higgs boson (see hierarchy problem). In the presence of supersymmetry, the triplet Higgsino needs to be more massive than the GUT scale to prevent proton decay because it generates dimension 5 operators in MSSM; there it is not enough simply to require the triplet to have a GUT scale mass.

References

  1. A. Masiero; D. V. Nanopoulos; K. Tamvakis; T. Yanagida (1982). "Naturally Massless Higgs Doublets in Supersymmetric SU(5)" (PDF). Physics Letters B. 115 (5): 380–384. Bibcode:1982PhLB..115..380M. doi:10.1016/0370-2693(82)90522-6.
  2. B. Grinstein (1982). "A Supersymmetric SU(5) Gauge Theory with No Gauge Hierarchy Problem". Nuclear Physics B. 206 (3): 387–396. Bibcode:1982NuPhB.206..387G. doi:10.1016/0550-3213(82)90275-9.

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