In physics, the Pati–Salam model is a Grand Unified Theory (GUT) proposed in 1974 by Jogesh Pati and Abdus Salam. Like other GUTs, its goal is to explain the seeming arbitrariness and complexity of the Standard Model in terms of a simpler, more fundamental theory that unifies, what are in the Standard Model, disparate particles and forces. The Pati–Salam unification is based on there being four quark color charges, dubbed red, green, blue and violet (or originally lilac), instead of the conventional three, with the new "violet" quark being identified with the leptons. The model also has left–right symmetry and predicts the existence of a high energy right handed weak interaction with heavy W' and Z' bosons and right-handed neutrinos. Originally the fourth color was labelled "lilac" to alliterate with "lepton". Pati–Salam is an alternative to the Georgi–Glashow SU(5) unification also proposed in 1974. Both can be embedded within an SO(10) unification model.
Core theory The Pati–Salam model states that the gauge group is either SU(4) × SU(2)L × SU(2)R or (SU(4) × SU(2)L × SU(2)R)/Z2 and the fermions form three families, each consisting of the representations (4, 2, 1) and (4, 1, 2). This needs some explanation. The center of SU(4) × SU(2)L × SU(2)R is Z4 × Z2L × Z2R. The Z2 in the quotient refers to the two element subgroup generated by the element of the center corresponding to the two element of Z4 and the 1 elements of Z2L and Z2R. This includes the right-handed neutrino. See neutrino oscillations. There is also a (4, 1, 2) and/or a (4, 1, 2) scalar field called the Higgs field which acquires a non-zero vacuum expectation value (VEV). This results in a spontaneous symmetry breaking from SU(4) × SU(2)L × SU(2)R to (SU(3) × SU(2) × U(1)Y)/Z3 or from (SU(4) × SU(2)L × SU(2)R)/Z2 to (SU(3) × SU(2) × U(1)Y)/Z6 and also,
(4, 2, 1) → (3, 2)1/6 ⊕ (1, 2)− 1/2 (q & l) (4, 1, 2) → (3, 1)1/3 ⊕ (3, 1)− 2/3 ⊕ (1, 1)1 ⊕ (1, 1)0 (d c, uc, ec & νc) (6, 1, 1) → (3, 1)− 1/3 ⊕ (3, 1)1/3 (1, 3, 1) → (1, 3)0 (1, 1, 3) → (1, 1)1 ⊕ (1, 1)0 ⊕ (1, 1)−1 See restricted representation. Calling the representations things like (4, 1, 2) and (6, 1, 1) is purely a physicist's convention, not a mathematician's convention, where representations are either labelled by Young diagrams or by Dynkin diagrams with numbers on their vertices, but still, it is standard among GUT theorists. The weak hypercharge, Y, is the sum of the two matrices:
( 1 3 0 0 0 0 1 3 0 0 0 0 1 3 0 0 0 0 − 1 ) ∈ SU ( 4 ) , ( 1 0 0 − 1 ) ∈ SU ( 2 ) R {\displaystyle {\begin{pmatrix}{\frac {1}{3}}&0&0&0\\0&{\frac {1}{3}}&0&0\\0&0&{\frac {1}{3}}&0\\0&0&0&-1\end{pmatrix}}\in {\text{SU}}(4),\qquad {\begin{pmatrix}1&0\\0&-1\end{pmatrix}}\in {\text{SU}}(2)_{\text{R}}}
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