A model that folds the three Standard Model forces into one.
Georgi-Glashow SU(5)
The minimal grand unified theory, in which one SU(5) symmetry holds all three Standard Model forces and every quark and lepton.
Placeholder for a 3D visualisation of Grand Unified Theories. The interactive scene will land in Phase 3. Grand unified theories place the strong, weak and electromagnetic forces inside one larger symmetry with a single coupling strength. Georgi and Glashow proposed a complete model based on the group SU(5) in 1974. Above a very high unification energy the three forces act as one. Below it the symmetry breaks, and the single force splits into the three we measure today. Quarks and leptons share multiplets, so new superheavy force carriers can turn one into the other. That makes the proton unstable, and proton decay is the family's main experimental test. The same theories predict superheavy magnetic monopoles formed in the early universe. Gravity stays outside this unification, so these theories unify the Standard Model forces and leave general relativity as it is.
§1 · The claim, in one sentence
Georgi and Glashow proposed in 1974 that three of nature's forces come from one SU(5) force; the minimal SU(5) model predicts a proton decay rate that experiments have ruled out, while larger SU(5) models are still studied.
Why this was rejected
- ▸Ellis, Gaillard, Nanopoulos and Rudaz (1980) estimated the minimal SU(5) proton lifetime at 8 x 10^30 years, uncertain by about two orders of magnitude. Super-Kamiokande (2020) excludes lifetimes below 2.4 x 10^34 years for decay into a positron and a neutral pion.
- ▸Amaldi, de Boer and Furstenau (1991) used LEP coupling measurements to show that a single unification point in the minimal non-supersymmetric model is excluded by more than seven standard deviations.
§2 · Why it might be true
The Standard Model has three separate forces, each with its own symmetry and strength. Georgi and Glashow proposed in 1974 that all three come from one symmetry, SU(5). At very high energy there is a single force. As the universe cools, the symmetry breaks and that force splits into the strong, weak and electromagnetic forces.
Think of quarks and leptons as distant relatives who turn out to share a household. SU(5) places each generation of matter in two shared multiplets, a five and a ten. Particles in the same multiplet can turn into one another through new superheavy force carriers, called X bosons.
That link makes the proton unstable. A proton can decay into a positron and a neutral pion, a flash that large underground water detectors watch for. Georgi, Quinn and Weinberg showed the same year that the forces meet only at an enormous energy. That is why the predicted decay is so rare.
The family stance
Grand unified theories propose that the three forces of the Standard Model come from a single symmetry at very high energy, and leave gravity for a later step. Whether nature follows this pattern is unconfirmed. The proposed merger happens far beyond any accelerator, typically near 10^16 GeV in supersymmetric versions, and quarks and leptons merge into shared multiplets at the same time. The traces at low energy would be fixed relations between the measured coupling strengths and, in most models, a proton that eventually decays.
§2.5 · Evidence
- Each generation of quarks and leptons fits into two SU(5) multiplets, a five and a ten.
- Later models, including supersymmetric SU(5), keep its symmetry group and its assignment of particles, so the framework outlived the minimal model.
§3 · What you'd need to test it
- The proton decays, most visibly into a positron and a neutral pion, with a lifetime the minimal model puts near 10^31 years
- The three Standard Model coupling strengths become equal at a single, very high unification energy
- The weak mixing angle, which sets how the weak and electromagnetic forces blend, is fixed by the symmetry and can be checked against measurement
- Stable superheavy magnetic monopoles can form when the unified symmetry breaks in the early universe, in numbers set by the cosmological history
§4 · Where it breaks
- Super-Kamiokande found no proton decaying into a positron and a neutral pion and set a lifetime limit above 2.4 x 10^34 years, far beyond the minimal prediction.
- Precise LEP data show that the three couplings of the non-supersymmetric model miss a single meeting point by more than seven standard deviations.
- The model offers no reason why the light Higgs doublet stays light while its colored partner, which also drives proton decay, must be superheavy.
- A hot early universe would fill with monopoles. Removing them needs an extra ingredient such as inflation, which Guth linked to monopole suppression in 1981.
Go deeper
Matter content: each generation fills a 5-bar (the down-type antiquark triplet and the lepton doublet) and a 10 (the quark doublet, the up-type antiquark and the positron). The gauge bosons sit in the 24-dimensional adjoint. It holds the 12 Standard Model gauge bosons plus 12 leptoquark bosons that carry both color and weak charge.
Symmetry breaking: an adjoint Higgs breaks SU(5) to SU(3) x SU(2) x U(1) at the unification scale, and a Higgs in the 5 breaks the electroweak symmetry. The color-triplet partner of the electroweak doublet in that 5 must be superheavy, because its exchange also mediates proton decay through dimension-six operators.
Running couplings: Georgi, Quinn and Weinberg (1974) set up the renormalization-group calculation that explains why the strong force is strong at low energy. In SU(5) it gives superheavy gauge bosons with masses perhaps as large as 10^17 GeV, close to the Planck mass. The same running fixes the prediction for sin^2 theta_W.
Monopoles: 't Hooft (1974) showed that any gauge theory in which electromagnetic U(1) sits inside a larger compact group contains magnetic monopoles as regular solutions. Preskill (1979) estimated that a grand unified phase transition would produce them in unacceptable numbers.
▸§5 · Who built it, and when(6 sources, 6 established)
- EstablishedGeorgi & Glashow (1974). 'Unity of All Elementary Particle Forces.' Phys. Rev. Lett. 32, 438
- EstablishedGeorgi, Quinn & Weinberg (1974). 'Hierarchy of Interactions in Unified Gauge Theories.' Phys. Rev. Lett. 33, 451
- EstablishedEllis, Gaillard, Nanopoulos & Rudaz (1980). 'Uncertainties in the Proton Lifetime.' Nucl. Phys. B 176, 61
- EstablishedPreskill (1979). 'Cosmological Production of Superheavy Magnetic Monopoles.' Phys. Rev. Lett. 43, 1365
- EstablishedAmaldi, de Boer & Furstenau (1991). 'Comparison of grand unified theories with electroweak and strong coupling constants measured at LEP.' Phys. Lett. B 260, 447
- EstablishedSuper-Kamiokande Collaboration, Takenaka et al. (2020). 'Search for proton decay via p to e+ pi0 and p to mu+ pi0 with an enlarged fiducial volume in Super-Kamiokande I-IV.' Phys. Rev. D 102, 112011
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