Conditions for suppressing dimension-five proton decay in renormalizable SUSY SO(10) GUT
Naoyuki Haba, Toshifumi Yamada
Abstract
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Naoyuki Haba, Toshifumi Yamada
Abstract
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Abstract The SUSY SO(10) GUT is in severe tension with the experimental bounds on proton partial lifetimes because proton decay mediated by colored Higgsinos (dimension-five proton decay) is too rapid. In this paper, we pursue the possibility that a texture of the Yukawa coupling matrices in a renormalizable SUSY SO(10) GUT model suppresses dimension-five proton decay. We focus on a general renormalizable SUSY SO(10) GUT model which contains 10 + 126 + $$ \overline{\textbf{126}} $$ 126 ¯ + 120 representation fields and where the Yukawa coupling matrices of the 16 matter fields with the 10, $$ \overline{\textbf{126}} $$ 126 ¯ , 120 fields, Y10, Y126, Y120, provide the quark and lepton Yukawa couplings and Majorana mass of the singlet neutrinos. We find that if components in certain flavor bases, $$ {\left({Y}_{10}\right)}_{u_R{d}_R} $$ Y 10 u R d R , $$ {\left({Y}_{126}\right)}_{u_R{d}_R} $$ Y 126 u R d R , $$ {\left({Y}_{10}\right)}_{u_R{s}_R} $$ Y 10 u R s R , $$ {\left({Y}_{126}\right)}_{u_R{s}_R} $$ Y 126 u R s R , $$ {\left({Y}_{10}\right)}_{u_L{d}_L} $$ Y 10 u L d L , $$ {\left({Y}_{126}\right)}_{u_L{d}_L} $$ Y 126 u L d L , $$ {\left({Y}_{10}\right)}_{u_L{s}_L} $$ Y 10 u L s L , $$ {\left({Y}_{126}\right)}_{u_L{s}_L} $$ Y 126 u L s L , $$ {\left({Y}_{10}\right)}_{u_L{u}_L} $$ Y 10 u L u L , $$ {\left({Y}_{126}\right)}_{u_L{u}_L} $$
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Abstract The SUSY SO(10) GUT is in severe tension with the experimental bounds on proton partial lifetimes because proton decay mediated by colored Higgsinos (dimension-five proton decay) is too rapid. In this paper, we pursue the possibility that a texture of the Yukawa coupling matrices in a renormalizable SUSY SO(10) GUT model suppresses dimension-five proton decay. We focus on a general renormalizable SUSY SO(10) GUT model which contains 10 + 126 + $$ \overline{\textbf{126}} $$ 126 ¯ + 120 representation fields and where the Yukawa coupling matrices of the 16 matter fields with the 10, $$ \overline{\textbf{126}} $$ 126 ¯ , 120 fields, Y10, Y126, Y120, provide the quark and lepton Yukawa couplings and Majorana mass of the singlet neutrinos. We find that if components in certain flavor bases, $$ {\left({Y}_{10}\right)}_{u_R{d}_R} $$ Y 10 u R d R , $$ {\left({Y}_{126}\right)}_{u_R{d}_R} $$ Y 126 u R d R , $$ {\left({Y}_{10}\right)}_{u_R{s}_R} $$ Y 10 u R s R , $$ {\left({Y}_{126}\right)}_{u_R{s}_R} $$ Y 126 u R s R , $$ {\left({Y}_{10}\right)}_{u_L{d}_L} $$ Y 10 u L d L , $$ {\left({Y}_{126}\right)}_{u_L{d}_L} $$ Y 126 u L d L , $$ {\left({Y}_{10}\right)}_{u_L{s}_L} $$ Y 10 u L s L , $$ {\left({Y}_{126}\right)}_{u_L{s}_L} $$ Y 126 u L s L , $$ {\left({Y}_{10}\right)}_{u_L{u}_L} $$ Y 10 u L u L , $$ {\left({Y}_{126}\right)}_{u_L{u}_L} $$
Key concepts: Yukawa potential, Physics, Proton decay, Particle physics, Supersymmetry, Lepton, SO(10), Muon