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Related papers: Three lepton decay modes of the proton

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An extension of the left--right symmetric model has been constructed which gives in a natural way the three lepton decay modes of the proton which have been suggested as an explanation for the atmospheric neutrino anomaly. We write down the…

High Energy Physics - Phenomenology · Physics 2009-09-25 Biswajoy Brahmachari , Patrick J. O'Donnell , Utpal Sarkar

We show that in supersymmetric unified theories such as SO(10), implementation of the see-saw mechanism for neutrino masses introduces a new set of color triplet fields and thereby a new source of d=5 proton decay operators. For neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-30 K. S. Babu , J. C. Pati , F. Wilczek

We discuss proton and neutron decays involving three leptons in the final state. Some of these modes could constitute the dominant decay channel because they conserve lepton-flavor symmetries that are broken in all usually considered…

High Energy Physics - Phenomenology · Physics 2018-04-25 Thomas Hambye , Julian Heeck

The proton decay modes $p\to K^0 e^+$ and $p\to K^0 \mu^+$ may be visible in certain supersymmetric theories, and if seen would provide evidence for new flavor physics at extremely short distances. These decay modes can arise from the…

High Energy Physics - Phenomenology · Physics 2009-09-29 Hitoshi Murayama , D. B. Kaplan

Issues of proton decay are examined in supersymmetric standard model with U(1) flavor symmetry. Dimension five proton-decay operators which arise generically are controlled by the flavor symmetry. We show that unlike the minimal…

High Energy Physics - Phenomenology · Physics 2009-11-07 Mitsuru Kakizaki , Masahiro Yamaguchi

We propose a mechanism for sufficient suppression of dimension-5 operators for proton decay in a supersymmetric SO(10) model. This mechanism is analogue to the double seesaw mechanism in studying neutrino masses. Only an intermediate VEV…

High Energy Physics - Phenomenology · Physics 2015-06-22 Xiaojia Li , Da-Xin Zhang

It is shown that in realistic SUSY GUT models of quark and lepton masses both the proton decay rate and branching ratios differ in general from those predicted in the minimal $SU(5)$ supersymmetric model. The observation of proton decay,…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr

In supersymmetric Grand Unified Theories, proton decay mediated by the color--triplet higgsino is generally problematic and requires some fine--tuning of parameters. We present a mechanism which naturally suppresses such dimension 5…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr

We present a study of proton decay in a supersymmetric $ SO(10)$ gauge theory in six dimensions compactified on an orbifold. The dimension 5 proton decay operators are absent, but the dimension 6 are enhanced due to the presence of KK…

High Energy Physics - Phenomenology · Physics 2007-05-23 Laura Covi

We explore proton decay in a class of realistic supersymmetric flipped $SU(5)$ models supplemented by a $U(1)_R$ symmetry which plays an essential role in implementing hybrid inflation. Two distinct neutrino mass models, based on inverse…

High Energy Physics - Phenomenology · Physics 2021-02-23 Maria Mehmood , Mansoor Ur Rehman , Qaisar Shafi

We discuss proton decay in a recently proposed model of supersymmetric hybrid inflation based on the gauge symmetry $SU(4)_c \times SU(2)_L \times SU(2)_R$. A $U(1)\, R$ symmetry plays an essential role in realizing inflation as well as in…

High Energy Physics - Phenomenology · Physics 2020-10-15 George Lazarides , Mansoor Ur Rehman , Qaisar Shafi

Within a chiral $SU(15)$ gauge theory in which the Standard Model fermions are bound states of massless preons, we show that proton-decay operators are likely induced at the compositeness scale, $\Lambda_{\rm pre}$. Our estimate of the…

High Energy Physics - Phenomenology · Physics 2023-01-18 Benoît Assi , Bogdan A. Dobrescu

I review the theoretical and experimental status of proton decay theory and experiment. Regarding theory, I focus mostly, but not only, on grand unification. I discuss only the minimal, well established SU(5) and SO(10) models, both…

High Energy Physics - Phenomenology · Physics 2010-04-22 Goran Senjanovic

Non-renormalizable operators both account for the failure of down quark and charged lepton Yukawa couplings to unify and reduce the proton decay rate via dimension-five operators in minimal SUSY SU(5) GUT. We extend the analysis to SUSY…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Wiesenfeldt

It has been shown recently that the problem of rapid proton decay induced by dimension five operators arising from the exchange of colored Higgsinos can be simply avoided in grand unified models where a fifth spatial dimension is…

High Energy Physics - Phenomenology · Physics 2011-05-12 Carl H. Albright , S. M. Barr

We study proton decay in a supersymmetric {\sf SO(10)} gauge theory in six dimensions compactified on an orbifold. The dimension-5 proton decay operators are forbidden by R-symmetry, whereas the dimension-6 operators are enhanced due to the…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Buchmuller , L. Covi , D. Emmanuel-Costa , S. Wiesenfeldt

Proton decay is usually discussed in the context of grand unified theories. However, as is well-known, in the standard model effective theory proton decay appears in the form of higher dimensional non-renormalizable operators. Here, we…

High Energy Physics - Phenomenology · Physics 2019-05-29 Juan Carlos Helo , Martin Hirsch , Toshihiko Ota

A minimal renormalizable SUSY SO(10) model with B-L symmetry broken by {\bf 126} Higgs field has recently been shown to predict all neutrino mixings and the ratio $\Delta m^2_{\odot}/\Delta m^2_A$ in agreement with observations. Unlike…

High Energy Physics - Phenomenology · Physics 2009-11-10 H. S. Goh , R. N. Mohapatra , S. Nasri , Siew-Phang Ng

Realistic models based on the renormalizable grand unified theories have varieties of scalars, many of which are capable of mediating baryon ($B$) and lepton ($L$) number non-conserving processes. We identify all such scalar fields residing…

High Energy Physics - Phenomenology · Physics 2022-08-05 Ketan M. Patel , Saurabh K. Shukla

We study the simplest renormalizable scalar leptoquark models where the standard model is augmented only by one additional scalar representation of SU(3) x SU(2) x U(1). The requirement that there be no proton decay from renormalizable…

High Energy Physics - Phenomenology · Physics 2013-08-26 Jonathan M. Arnold , Bartosz Fornal , Mark B. Wise
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