In physics, the trinification model is a Grand Unified Theory proposed by Alvaro De Rújula, Howard Georgi and Sheldon Glashow in 1984.
Details It states that the gauge group is either
S U ( 3 ) C × S U ( 3 ) L × S U ( 3 ) R {\displaystyle SU(3)_{C}\times SU(3)_{L}\times SU(3)_{R}}
or
[ S U ( 3 ) C × S U ( 3 ) L × S U ( 3 ) R ] / Z 3 {\displaystyle [SU(3)_{C}\times SU(3)_{L}\times SU(3)_{R}]/\mathbb {Z} _{3}} ; and that the fermions form three families, each consisting of the representations: Q = ( 3 , 3 ¯ , 1 ) {\displaystyle \mathbf {Q} =(3,{\bar {3}},1)} , Q c = ( 3 ¯ , 1 , 3 ) {\displaystyle \mathbf {Q} ^{c}=({\bar {3}},1,3)} , and L = ( 1 , 3 , 3 ¯ ) {\displaystyle \mathbf {L} =(1,3,{\bar {3}})} . The L includes a hypothetical right-handed neutrino, which may account for observed neutrino masses (see neutrino oscillations), and a similar sterile "flavon." There is also a ( 1 , 3 , 3 ¯ ) {\displaystyle (1,3,{\bar {3}})} and maybe also a ( 1 , 3 ¯ , 3 ) {\displaystyle (1,{\bar {3}},3)} scalar field called the Higgs field which acquires a vacuum expectation value. This results in a spontaneous symmetry breaking from
S U ( 3 ) L × S U ( 3 ) R {\displaystyle SU(3)_{L}\times SU(3)_{R}} to [ S U ( 2 ) × U ( 1 ) ] / Z 2 {\displaystyle [SU(2)\times U(1)]/\mathbb {Z} _{2}} . The fermions branch (see restricted representation) as
( 3 , 3 ¯ , 1 ) → ( 3 , 2 ) 1 6 ⊕ ( 3 , 1 ) − 1 3 {\displaystyle (3,{\bar {3}},1)\rightarrow (3,2)_{\frac {1}{6}}\oplus (3,1)_{-{\frac {1}{3}}}} ,
( 3 ¯ , 1 , 3 ) → 2 ( 3 ¯ , 1 ) 1 3 ⊕ ( 3 ¯ , 1 ) − 2 3 {\displaystyle ({\bar {3}},1,3)\rightarrow 2\,({\bar {3}},1)_{\frac {1}{3}}\oplus ({\bar {3}},1)_{-{\frac {2}{3}}}} ,
( 1 , 3 , 3 ¯ ) → 2 ( 1 , 2 ) − 1 2 ⊕ ( 1 , 2 ) 1 2 ⊕ 2 ( 1 , 1 ) 0 ⊕ ( 1 , 1 ) 1 {\displaystyle (1,3,{\bar {3}})\rightarrow 2\,(1,2)_{-{\frac {1}{2}}}\oplus (1,2)_{\frac {1}{2}}\oplus 2\,(1,1)_{0}\oplus (1,1)_{1}} , and the gauge bosons as
( 8 , 1 , 1 ) → ( 8 , 1 ) 0 {\displaystyle (8,1,1)\rightarrow (8,1)_{0}} ,
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