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Changes between Version 235 and Version 236 of ALRM

v235	v236
20	20
21	21
22		The Alternative Left-Right Symmetric Model (ALRM) is gauged by the Left-Right symmetry group ''SU(3),,C,,×SU(2),,L,,×SU(2),,R,,×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; causing the absence of the tree-level flavor-changing neutral currents mediated by Higgs bosons.
	22	The Alternative Left-Right Symmetric Model (ALRM) is gauged by the Left-Right symmetry group ''SU(3),,C,,×SU(2),,L,,×SU(2),,R,,×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 interactions; causing the absence of the tree-level flavor-changing neutral currents mediated by Higgs bosons.
23	23
24	24	As in the SM, left-handed fermions compose ''SU(2),,L,,'' doublets. Right-handed charged leptons form ''SU(2),,R,,'' doublets with corresponding extra particles (scotinos) and right-handed up-quarks form ''SU(2),,R,,'' doublets with corresponding extra down-type exotic quarks. Right-handed 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.