Georgi-Glashow Model

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## Construction

## Breaking SU(5)

## Minimal supersymmetric SU(5)

### Spacetime

### Spatial symmetry

### Gauge symmetry group

### Global internal symmetry

### Matter parity

### Vector superfields

### Chiral superfields

### Superpotential

### Vacua

#### The ? sector

#### Decomposition

#### Fermion masses

## Proton decay in SU(5)

### Mechanism

## References

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

Georgi%E2%80%93Glashow Model

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In particle physics, the **Georgi-Glashow model**^{[1]} is a particular grand unified theory (GUT) proposed by Howard Georgi and Sheldon Glashow in 1974. In this model the standard model gauge groups SU(3) × SU(2) × U(1) are combined into a single simple gauge group SU(5). The unified group SU(5) is then thought to be spontaneously broken into the standard model subgroup below some very high energy scale called the grand unification scale.

Since the Georgi-Glashow model combines leptons and quarks into single irreducible representations, there exist interactions which do not conserve baryon number, although they still conserve the quantum number associated with the symmetry of the common representation. This yields a mechanism for proton decay, and the rate of proton decay can be predicted from the dynamics of the model. However, proton decay has not yet been observed experimentally, and the resulting lower limit on the lifetime of the proton contradicts the predictions of this model. However, the elegance of the model has led particle physicists to use it as the foundation for more complex models which yield longer proton lifetimes, particularly SO(10) in basic and SUSY variants.

(For a more elementary introduction to how the representation theory of Lie algebras are related to particle physics, see the article Particle physics and representation theory.)

This model suffers from the doublet-triplet splitting problem.^{[clarification needed]}

SU(5) acts on and hence on its exterior algebra . Picking a splitting restricts SU(5) to S(U(2)×U(3)), yielding matrices of the form

with kernel , hence isomorphic to the standard model's true gauge group . For the zeroth power , this acts trivially, matching a left-handed neutrino, . For the first exterior power , the standard model's group action preserves the splitting . The transforms trivially in SU(3), as a doublet in SU(2), and under the Y = ½ representation of U(1) (as weak hypercharge is conventionally normalized as ?^{3} = ?^{6Y}); this matches a right-handed anti-lepton, (as in SU(2)). The transforms as a triplet in SU(3), a singlet in SU(2), and under the Y = − representation of U(1) (as ?^{−2} = ?^{6Y}); this matches a right-handed down quark, .

The second power is obtained via the formula . As SU(5) preserves the canonical volume form of , Hodge duals give the upper three powers by . Thus the standard model's representation *F* ? *F** of one generation of fermions and antifermions lies within .

Similar motivations apply to Pati-Salam, and to SO(10), E6, and other supergroups of SU(5).

SU(5) breaking occurs when a scalar field, analogous to the Higgs field, and transforming in the adjoint of SU(5) acquires a vacuum expectation value proportional to the weak hypercharge generator,

When this occurs, SU(5) is spontaneously broken to the subgroup of SU(5) commuting with the group generated by *Y*.

This unbroken subgroup is just the standard model group,

Under their unbroken subgroup, the adjoint **24** transforms as

giving the gauge bosons of the standard model plus the new X and Y bosons. See restricted representation.

The standard model quarks and leptons fit neatly into representations of SU(5). Specifically, the left-handed fermions combine into 3 generations of . Under the unbroken subgroup these transform as

giving precisely the left-handed fermionic content of the standard model, where for every generation d^{c}, u^{c}, e^{c} and ?^{c} stand for anti-down-type quark, anti-up-type quark, anti-down-type lepton and anti-up-type lepton, respectively, and q and l stand for quark and lepton. Fermions transforming as a **1** under SU(5) are now thought to be necessary because of the evidence for neutrino oscillations, unless a way is found to introduce a tiny Majorana coupling for the left-handed neutrinos.

Since the homotopy group

this model predicts 't Hooft-Polyakov monopoles.

These monopoles have quantized Y magnetic charges. Since the electromagnetic charge Q is a linear combination of some SU(2) generator with Y/2, these monopoles also have quantized magnetic charges, where by magnetic here, we mean electromagnetic magnetic charges.

The superspace extension of 3+1 Minkowski spacetime.

SUSY over 3+1 Minkowski spacetime without R-symmetry.

SU(5).

(matter parity)

To prevent unwanted couplings in the supersymmetric version of the model, we assign a matter parity to the chiral superfields with the matter fields having odd parity and the Higgs having even parity. This is unnecessary in the non-supersymmetric version, but then, we can't protect the electroweak Higgs from quadratic radiative mass corrections. See hierarchy problem. In the non-supersymmetric version the action is invariant under a similar symmetry because the matter fields are all fermionic and thus must appear in the action in pairs, while the Higgs fields are bosonic.

Those associated with the SU(5) gauge symmetry

As complex representations:

label | description | multiplicity | SU(5) rep | rep |
---|---|---|---|---|

? | GUT Higgs field | 1 | 24 |
+ |

H_{u} |
electroweak Higgs field | 1 | 5 |
+ |

H_{d} |
electroweak Higgs field | 1 | + | |

matter fields | 3 | - | ||

10 |
matter fields | 3 | 10 |
- |

N^{c} |
sterile neutrinos | ? | 1 |
- |

A generic invariant renormalizable superpotential is a (complex) invariant cubic polynomial in the superfields. It is a linear combination of the following terms:

The first column is an Abbreviation of the second column (neglecting proper normalization factors), where capital indices are SU(5) indices, and i and j are the generation indices.

The last two rows presupposes the multiplicity of is not zero (i.e. that a sterile neutrino exists). The coupling has coefficients which are symmetric in *i* and *j*. The coupling has coefficients which are symmetric in *i* and *j*. The number of sterile neutrino generations need not be three, unless the SU(5) is embedded in a higher unification scheme such as SO(10).

The vacua correspond to the mutual zeros of the F and D terms. Let's first look at the case where the VEVs of all the chiral fields are zero except for ?.

The F zeros corresponds to finding the stationary points of W subject to the traceless constraint So, where ? is a Lagrange multiplier.

Up to an SU(5) (unitary) transformation,

The three cases are called case I, II and III and they break the gauge symmetry into and respectively (the stabilizer of the VEV).

In other words, there are at least three different superselection sections, which is typical for supersymmetric theories.

Only case III makes any phenomenological sense and so, we will focus on this case from now onwards.

It can be verified that this solution together with zero VEVs for all the other chiral multiplets is a zero of the F-terms and D-terms. The matter parity remains unbroken (right up to the TeV scale).

The gauge algebra **24** decomposes as

This **24** is a real representation, so the last two terms need explanation. Both and are complex representations. However, the direct sum of both representation decomposes into two irreducible real representations and we only take half of the direct sum, i.e. one of the two real irreducible copies. The first three components are left unbroken. The adjoint Higgs also has a similar decomposition, except that it is complex. The Higgs mechanism causes one real HALF of the and of the adjoint Higgs to be absorbed. The other real half acquires a mass coming from the D-terms. And the other three components of the adjoint Higgs, and acquire GUT scale masses coming from self pairings of the superpotential,

The sterile neutrinos, if any exists, would also acquire a GUT scale Majorana mass coming from the superpotential coupling ?^{c2}.

Because of matter parity, the matter representations and **10** remain chiral.

It is the Higgs fields 5_{H} and which are interesting.

The two relevant superpotential terms here are and . Unless there happens to be some fine tuning, we would expect both the triplet terms and the doublet terms to pair up, leaving us with no light electroweak doublets. This is in complete disagreement with phenomenology. See doublet-triplet splitting problem for more details.

Unification of the Standard Model via an SU(5) group has significant phenomenological implications. Most notable of these is proton decay, which is present in SU(5) with and without supersymmetry. This is allowed by the new vector bosons introduced from the adjoint representation of SU(5), which also contains the gauge bosons of the standard model forces. Since these new gauge bosons are in (3,2)_{-5/6}bifundamental representations, they violated baryon and lepton number. As a result, the new operators should cause protons to decay at a rate inversely proportional to their masses. This process is called dimension 6 proton decay and is an issue for the model, since the proton is experimentally determined to have a lifetime greater than the age of the universe. This means that an SU(5) model is severely constrained by this process.

As well as these new gauge bosons, in SU(5) models the Higgs field is usually embedded in a **5** representation of the GUT group. The caveat of this is that since the Higgs field is an SU(2) doublet, the remaining part, an SU(3) triplet, must be some new field - usually called D. This new scalar would be able to generate proton decay as well and, assuming the most basic Higgs vacuum alignment, would be massless, allowing the process at very high rates.

While not an issue in the Georgi-Glashow model, a supersymmeterised SU(5) model would have additional proton decay operators due to the superpartners of the standard model fermions. The lack of detection of proton decay (in any form) brings into question the veracity of SU(5) GUTs of all types, however, while the models are highly constrained by this result, they are not in general ruled out.

In the lowest-order Feynman diagram corresponding to the simplest source of proton decay in SU(5), a left-handed and a right-handed up quark annihilate, yielding an X^{+} boson, which decays to a right-handed (or left-handed) positron and a left-handed (or right-handed) anti-down quark:

- ,

- .

This process conserves weak isospin, weak hypercharge, and color. GUTs equate anti-color with having 2 colors, , and SU(5) defines left-handed normal leptons as "white" and right-handed antileptons as "black." The first vertex only involves fermions of the **10** representation, while the second only involves fermions in the **5?** (or **10**), demonstrating the preservation of SU(5) symmetry.

**^**Georgi, Howard; Glashow, Sheldon (1974). "Unity of All Elementary-Particle Forces".*Physical Review Letters*.**32**(8): 438. Bibcode:1974PhRvL..32..438G. doi:10.1103/PhysRevLett.32.438. S2CID 9063239.

- Georgi, Howard; Glashow, Sheldon (1974). "Unity of All Elementary-Particle Forces".
*Physical Review Letters*.**32**(8): 438. Bibcode:1974PhRvL..32..438G. doi:10.1103/PhysRevLett.32.438. S2CID 9063239. - Baez, J. C.; Huerta, J. (2010). "The Algebra of Grand Unified Theories".
*Bull. Amer. Math. Soc.***47**(3): 483-552. arXiv:0904.1556. doi:10.1090/S0273-0979-10-01294-2. S2CID 2941843. - Langacker, Paul (2012). "Grand unification".
*Scholarpedia*.**7**(10): 11419. Bibcode:2012SchpJ...711419L. doi:10.4249/scholarpedia.11419.

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

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