Changes between Version 45 and Version 46 of ALRM


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Timestamp:
Apr 25, 2016, 2:42:21 PM (9 years ago)
Author:
Mustafa Ashry
Comment:

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  • ALRM

    v45 v46  
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    28 As any other left-right symmetric model, ALRM is a QFT gauged by SU(2)_L×SU(2)_R×U(1)_B-L. B and L being the baryon and lepton numbers. An extra discrete S symmetry is imposed to differentiate between both the left and right fields and interactions of the Higgs sector. 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 exotic down-type 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.
     28As any other left-right symmetric model, ALRM is a QFT gauged by SU(2)_L×SU(2)_R×U(1)_B-L. B and L being the baryon and lepton numbers. An extra discrete S symmetry is imposed to differentiate between both the left and right fields and interactions of the Higgs sector. 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 exotic down-type 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. The physical gauge sector of the model contains the electroweak gauge bosons (photon, W and Z bosons) and two extra gauge bosons (W' and Z') correspond to the SU(2)_R group.
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    3030'''References'''