Doublet–triplet splitting problem explained

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} . 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 μ-problem

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

\int d ^{2\theta} λ H _{\bar{5} } \Sigma H_ + \mu H_ H_

where

\Sigma is an adjoint of SU(5) and is traceless. When \Sigma acquires a vacuum expectation value\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

\int d ^{2\theta} ( 2 λ f + \mu) H _{\bar{3} }H_3 + (-3\lambda f +\mu) H_H_2

Since

f is at the GUT scale (10 ^{16} GeV) and the Higgs doublets need to have a weak scale mass (100 GeV), this requires\mu \sim 3 λ f \pm 100 GeV .

So to solve this doublet–triplet splitting problem requires a tuning of the two terms to within one part in

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

SU( 5 ) proposed in ^[1] and ^[2] 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} and Z _{\overline{50} }. Note that { 50 } decomposes as follows under the SM gauge group:50 → ( 1 , 1 , -2 ) + ( 3 , 1 , - (13 ) + (\overline{ 3)/() },\mathbf,-\frac 76)+(\mathbf,\mathbf,\frac 43)+(\overline,\mathbf,-\frac 13)+(\mathbf,\mathbf,\frac 12)which contains no field that could couple to the SU( 2 ) doublets of H _{\overline{5} } or H _{{5} }. Due to group theoretical reasons SU( 5 ) has to be broken by a 75 instead of the usual 24 , at least at the renormalizable level. The superpotential then readsW _{MPM} = y _{1} H _{\overline{5} }H_Z_+y_2 Z_H_H_+m_Z_Z_.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,

\Sigma acquires a vacuum expectation value of the form\langle \Sigma \rangle = 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} and f _{3} give masses to the Higgs doublet and triplet, respectively, and are independent of each other, because \Sigma is traceless for any values they may have. If 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\over} ⊕ ( 3 , 1 ) _{-{1\over} }\bar{ 5 } → ( 1 , 2 ) _{-{1\over} }\oplus (\bar,1)_

In SO(10):

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

Proton decay

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

• 'Supersymmetry at Ordinary Energies. 1. Masses AND Conservation Laws.' Steven Weinberg. Published in Phys. Rev. D 26:287,1982.
• 'Proton Decay in Supersymmetric Models.' Savas Dimopoulos, Stuart A. Raby, Frank Wilczek. Published in Phys. Lett. B 112:133,1982.
• 'Incomplete Multiplets in Supersymmetric Unified Models.' Savas Dimopoulos, Frank Wilczek.

External links

• Web site: Where in the World are SUSY & WIMPS? - Nima Arkani-Hamed. 20 July 2017. YouTube. https://ghostarchive.org/varchive/youtube/20211213/dKVXxcbJ4YY. 2021-12-13 . live. (In this video from 12:00 to 18:00, Arkani-Hamed gives a brief discussion of the relation between the doublet–triplet splitting problem and the hierarchy problem.)

Notes and References

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