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Related papers: Proton stability from a fourth family

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Within supersymmetric SU(5) GUT we suggest mechanisms for suppression of baryon number violating dimension five and six operators. The mechanism is based on the idea of split multiplets (i.e. quarks and leptons are not coming from a single…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zurab Tavartkiladze

For a large set of flavor symmetries, the lowest-dimensional baryon- or lepton-number violating operators in the Standard Model effective field theory (SMEFT) with flavor symmetry are of mass dimension 9. As a consequence, baryon- and…

High Energy Physics - Phenomenology · Physics 2019-12-04 Andreas Helset , Andrew Kobach

In most supersymmetric models the stability of the proton is ensured by invoking R-parity. A necessary ingredient to enforce R-parity is the possibility of distinguishing the lepton superfields from the Higgs ones. This is generally…

High Energy Physics - Phenomenology · Physics 2016-08-24 Zurab Berezhiani , Enrico Nardi

The straightforward supersymmetrization of the Standard Model (SM) results in a phenomenologically inconsistent theory in which Baryon number ($B$) and Lepton number ($L$) are violated by dimension 4 operators, inducing fast proton decay.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Diego Restrepo

Proton stability is guaranteed in the MSSM by assuming a discrete symmetry, R-parity. However, there are additional R-parity conserving higher dimensional operators which violate lepton and baryon numbers and induce fast proton decay. Here…

High Energy Physics - Phenomenology · Physics 2013-07-12 S. Morisi , E. Peinado , A. Vicente

One of the most puzzling questions in particle physics concerns the status of the baryon (B) and lepton (L) quantum numbers. On the theoretical side, most new physics scenarios naturally lead to their non-conservation and some amount of…

High Energy Physics - Phenomenology · Physics 2013-03-12 Gauthier Durieux , Jean-Marc Gérard , Fabio Maltoni , Christopher Smith

If the present baryon-asymmetry is due to a Planck or GUT-scale matter asymmetry then baryon- or lepton-number violating processes are constrained by the condition that they do not subsequently erase this asymmetry. We present a revision of…

High Energy Physics - Phenomenology · Physics 2009-10-22 Herbert Dreiner , Graham G. Ross

The first part of this talk presents the general complexion of baryon and lepton number non-conservation that may arise in the context of quark-lepton unification. The second part presents the status of grand unification with and without…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jogesh C. Pati

The smallness of the quark and lepton parameters and the hierarchy between them could be the result of selection rules due to a horizontal symmetry broken by a small parameter. The same selection rules apply to baryon number violating…

High Energy Physics - Phenomenology · Physics 2011-04-08 Valerie Ben-Hamo , Yosef Nir

A simple extension of the minimal supersymmetric standard model in which baryon and lepton numbers are local gauge symmetries spontaneously broken at the supersymmetry scale is reported. This theory provides a natural explanation for proton…

High Energy Physics - Phenomenology · Physics 2015-07-09 Bartosz Fornal

In supersymmetric standard models R-parity violating couplings are severely constrained, since otherwise they would erase the existing baryon asymmetry before the electroweak transition. It is often claimed that this cosmological constraint…

High Energy Physics - Phenomenology · Physics 2014-11-20 Motoi Endo , Koichi Hamaguchi , Sho Iwamoto

The Standard Model has three generations of fermions and although it does not contain any explicit reason for this, the existence of additional generations is now very constrained by experiment. Present measurements are saturating…

High Energy Physics - Phenomenology · Physics 2014-12-17 Alfredo Aranda , Jose A. R. Cembranos

We study the flavor structure of the lepton and baryon number--conserving dimension-6 operators in the Standard Model effective field theory (SMEFT). Building on the work of [1], we define several well-motivated flavor symmetries and…

High Energy Physics - Phenomenology · Physics 2023-05-26 Admir Greljo , Ajdin Palavrić , Anders Eller Thomsen

We recall the obstacles which seemed, long ago, to prevent one from viewing supersymmetry as a possible fundamental symmetry of Nature. Is spontaneous supersymmetry breaking possible ? Where is the spin-1/2 Goldstone fermion of…

High Energy Physics - Phenomenology · Physics 2016-11-23 Pierre Fayet

We compile information from low-energy observables sensitive to flavor-conserving 4-fermion operators with two or four leptons. Our analysis includes data from e+e- colliders, neutrino scattering on electron or nucleon targets, atomic…

High Energy Physics - Phenomenology · Physics 2017-09-13 Adam Falkowski , Martín González-Alonso , Kin Mimouni

We present here arguments in favor of the existence of the lightest lepton and its neutrino. This new family with a fourth lepton flavor uncovered so far unobserved universal properties of matter. The unity of the laws of their nature…

General Physics · Physics 2017-11-08 Rasulkhozha S. Sharafiddinov

Recently it was pointed out that in the TeV-scale brane world there is a logical possibility where the electroweak Higgs can be identified with a fourth generation slepton. In this paper we address various issues in this four-generation…

High Energy Physics - Theory · Physics 2009-10-31 Zurab Kakushadze

Baryon triality (B3) is a Z3 discrete symmetry that can protect the proton from decay. Although its realization does not require supersymmetry, it is particularly appealing in the supersymmetry as an alternative to the popular R-parity. We…

High Energy Physics - Phenomenology · Physics 2015-05-19 Hye-Sung Lee

A review of baryon and lepton conservation in supersymmetric grand unified theories is given. Proton stability is discussed in the minimal SU(5) supergravity grand unification and in several non-minimal extensions such as the $SU(3)^3$,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pran Nath , R. Arnowitt

The absence so far of any supersymmetric signals at the LHC pushes towards a rethinking of the assumptions underlying the MSSM. Because the large missing $E_T$ searches are inadequate to detect a LSP decaying within the detector, R-parity…

High Energy Physics - Phenomenology · Physics 2013-08-30 Angelo Monteux
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