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Bounds on R-parity violating couplings in the supersymmetric standard model are reviewed, and some new bounds arising from non-observation of certain rare B-decays (such as $B \rightarrow K^+K^-$) are presented. The focus is on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marc Sher

We discuss the role of heavy scalar fields in mediating neutrinoless double beta decay $(0\nu\beta\beta)$ within the $SU(5)$ Grand Unified Theory framework, extended suitably to include neutrino mass. In such a minimal realistic $SU(5)$…

High Energy Physics - Phenomenology · Physics 2026-01-16 P. S. Bhupal Dev , Srubabati Goswami , Debashis Pachhar , Saurabh K. Shukla

We consider the proton decay involving a light gravitino or axino in gauge-mediated supersymmetry breaking models to derive constraints on the $R$ parity and baryon number violating Yukawa couplings. Bounds on all nine coupling constants…

High Energy Physics - Phenomenology · Physics 2009-10-31 Kiwoon Choi , Kyuwan Hwang , Jae Sik Lee

Neutrinoless double beta decay, lepton number violating collider processes and the Baryon Asymmetry of the Universe (BAU) are intimately related. In particular lepton number violating processes at low energies in combination with sphaleron…

High Energy Physics - Phenomenology · Physics 2015-05-29 Julia Harz , Wei-Chih Huang , Heinrich Päs

Proton decay, although unobserved so far, is a natural expectation when attempting to explain the baryon asymmetry of the universe. $p\to K^+\bar{\nu}$ or $p\to K^+\tilde{\chi}_1^0$, with $\tilde{\chi}_1^0$ a light exotic neutral particle,…

High Energy Physics - Phenomenology · Physics 2024-03-28 Florian Domingo , Herbi K. Dreiner , Dominik Köhler , Saurabh Nangia , Apoorva Shah

Using data collected with the OPAL detector at LEP, we have searched for the processes e+e- -> Z0 -> p e-, p mu- and the charge conjugate final-states. These would violate the conservation of the baryon-number B, lepton-number L and the…

High Energy Physics - Experiment · Physics 2008-11-26 The OPAL Collaboration , G. Abbiendi et al

Dimension-five operators for nucleon decays are suppressed in the modified missing doublet (MMD) model in the supersymmetric SU(5) grand unification. We show that nonrenormalizable interactions decrease the unification scale in the MMD…

High Energy Physics - Phenomenology · Physics 2009-09-29 J. Hisano , Yasunori Nomura , T. Yanagida

We have searched for the violation of baryon number B and lepton number L in the (B-L)-conserving modes tau- -> anti-Lambda0 pi- and tau- -> anti-Lambda0 K- as well as the (B-L)-violating modes tau- -> Lambda0 pi- and tau- -> Lambda0 K-…

High Energy Physics - Experiment · Physics 2007-05-23 The BABAR Collaboration , B. Aubert

Below the electroweak scale, new physics that violates lepton number in two units ($\Delta L = 2$) and is mediated by heavy particle exchange can be parameterized by a dimension-9 low-energy effective Lagrangian. Operators in this…

High Energy Physics - Phenomenology · Physics 2025-03-11 Marcela González , Nicolás A. Neill

We discuss the relation between lepton number violation at high and low energies, particularly, the constraints on baryogenesis models, which would be implied by an observation of neutrinoless double beta decay. The primordial baryon…

High Energy Physics - Phenomenology · Physics 2016-05-05 Lukas Graf

Using the freedom in SO(10) GUT's one can generalize the existing models without changing the mass spectrum of fermions to obtain a significant suppression of proton decay resulting from the baryon number violating operators of dimension 5.…

High Energy Physics - Phenomenology · Physics 2009-11-07 Krzysztof Turzynski

We point out that if the baryon number violating neutron-antineutron oscillation is discovered, it would impose strong limits on the departure from Einstein's equivalence principle at a level of one part in $10^{19}$. If this departure owes…

High Energy Physics - Phenomenology · Physics 2016-10-05 K. S. Babu , Rabindra N. Mohapatra

Many extensions of the Standard Model have to face the problem of new unsuppressed baryon-number violating interactions. In supersymmetry, the simplest way to solve this problem is to assume R-parity conservation. As a result, the lightest…

High Energy Physics - Phenomenology · Physics 2011-05-05 Kaustubh Agashe , Geraldine Servant

Nucleon decays put extremely stringent bounds on baryon-number-violating interactions. However, in case the corresponding operators involve only $\tau$ leptons, the direct two-body decays, e.g., $p\to\pi^0 \tau^+$, are kinematically not…

High Energy Physics - Phenomenology · Physics 2023-09-18 Andreas Crivellin , Martin Hoferichter

The strongly interacting sector in the E6 inspired composite Higgs model (E6CHM) with baryon number violation possesses SU(6)\times U(1)_L global symmetry. In the weakly-coupled sector of this model the U(1)_L symmetry associated with…

High Energy Physics - Phenomenology · Physics 2018-08-07 R. Nevzorov , A. W. Thomas

The observed matter-antimatter asymmetry in the universe is a serious challenge to our understanding of nature. Baryon/lepton number violation (BNV/LNV) decays have been searched for in many experiments to understand this large-scale…

High Energy Physics - Experiment · Physics 2025-11-04 Xudong Yu

In models with a low quantum gravity scale, one might expect that all operators consistent with gauge symmetries are present in the low-energy effective theory. If this is the case, some mechanism must be present to adequately suppress…

High Energy Physics - Phenomenology · Physics 2011-03-23 Alfredo Aranda , Christopher D. Carone

With a goal toward explaining the observed baryon asymmetry of the Universe, we extend the standard model (SM) by adding a vector-vector dimension-six effective operator coupling a new Dirac fermion $\chi$, uncharged under the SM gauge…

High Energy Physics - Phenomenology · Physics 2023-08-22 Shrihari Gopalakrishna , Rakesh Tibrewala

We enumerate the simplest models that have baryon number violation at the classical level but do not give rise to proton decay. These models have scalar fields in two representations of SU(3) x SU(2) x U(1) and violate baryon number by two…

High Energy Physics - Phenomenology · Physics 2013-04-22 Jonathan M. Arnold , Bartosz Fornal , Mark B. Wise

The lepton number violating process can be induced by introducing a fourth generation heavy Majorana neutrino, which is coupled to the charged leptons of Standard Model. There have been many previous studies on the leptonic number violating…

High Energy Physics - Phenomenology · Physics 2013-07-23 Hai-Rong Dong , Feng Feng , Hai-Bo Li
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