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Changes between Version 148 and Version 149 of ALRM

v148	v149
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22		As any other left-right symmetric model, ALRM is a QFT gauged by the gauge symmetry group ''SU(3),,C,,×SU(2),,L,,×SU(2),,R,,×U(1),,B-L,,'' XXX $~~[SU(3)_{C}\times SU(2)_{L}\times SU(2)_{R}\times U(1)_{B-L}]~~$. The latter ''B'' and ''L'' being the baryon and lepton numbers. An extra discrete symmetry ''S'' is imposed to distinguish between Higgs fields and their dual fields and hence their interactions.
	22	As any other left-right symmetric model, ALRM is a QFT gauged by the gauge symmetry group ''SU(3),,C,,×SU(2),,L,,×SU(2),,R,,×U(1),,B-L,,'' XXX $$[SU(3)_{C}\times SU(2)_{L}\times SU(2)_{R}\times U(1)_{B-L}]$$. The latter ''B'' and ''L'' being the baryon and lepton numbers. An extra discrete symmetry ''S'' is imposed to distinguish between Higgs fields and their dual fields and hence their interactions.
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24	24	As in the SM, left fermions compose ''SU(2),,L,,'' doublets. Right charged leptons are accommodated in ''SU(2),,R,,'' doublets with corresponding extra particles (scotinos) and right up-quarks in ''SU(2),,R,,'' doublets with corresponding extra down-type exotic quarks. Right neutrinos and down-quarks are ''SU(2),,L,R,,'' singlets. The Higgs sector composes of an ''SU(2),,L,,''-doublet, an ''SU(2),,R,,''-doublet and a bidoublet.