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Left-right symmetry

In theoretical physics, the electroweak model breaks parity maximally. All its fermions are chiral Weyl fermions. Some theorists found this objectionable, and so proposed a GUT extension of the electroweak group

{[SU(2)_W\times U(1)_Y]\over \mathbb{Z}_2}

to

{SU(2)_L\times SU(2)_R\times U(1)_{B-L}\over \mathbb{Z}_2}.

Here, SU(2)_L (pronounced SU(2) left) is none other than SU(2)W and B-L is the baryon number minus the lepton number.

There is also the chromodynamic SU(3)C. The idea was to restore parity by introducing a left-right symmetry. This is a group extension of Z2 (the left-right symmetry) by

{SU(3)_C\times SU(2)_L \times SU(2)_R \times U(1)_{B-L}\over \mathbb{Z}_6}

to the semidirect product

{SU(3)_C\times SU(2)_L \times SU(2)_R \times U(1)_{B-L}\over \mathbb{Z}_6}Image:rtimes2.pngZ2.

This has two connected components where Z2 acts as an automorphism, which is the composition of an involutive outer automorphism of SU(3)C with the interchange of the left and right copies of SU(2) with the reversal of U(1)B-L. This left-right symmetry is spontaneously broken to give a chiral low energy theory.

In this setting the chiral quarks

(3,2,1)1/3

and

(\bar{3},1,2)_{-{1\over 3}}

are unified into an irrep

(3,2,1)_{1\over 3}\oplus(\bar{3},1,2)_{-{1\over 3}}.

The leptons are also unified into an irrep

(1,2,1)_{-1}\oplus(1,1,2)_1.

This then predicts three sterile neutrinos , which is perfectly consistent with current neutrino oscillation data.

Because the left-right symmetry is spontaneously broken, left-right models predict domain walls.

Later, this left-right symmetry idea was used in the Pati-Salam model and trinification.

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