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Related papers: Constraints on fourth generation Majorana neutrino…

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A novel method to differentiate the effects of Dirac and Majorana (D-M) neutrinos in four-body decays has been discussed in arXiv:2106.11785. There, it is concluded that the back-to-back kinematic scenario seems to avoid the constraint…

High Energy Physics - Phenomenology · Physics 2024-02-09 Juan Manuel Márquez , Diego Portillo-Sánchez , Pablo Roig

In the event of an observation of neutrinoless double beta decay, a relevant question would be: what lepton number violating physics is responsible for the decay? The exchange of Majorana neutrinos and/or supersymmetric particles may…

High Energy Physics - Phenomenology · Physics 2010-07-20 B. C. Allanach , C. H. Kom , H. Päs

We revisit the current experimental bounds on fourth-generation Majorana neutrino masses, including the effects of right handed neutrinos. Current bounds from LEPII are significantly altered by a global analysis. We show that the current…

High Energy Physics - Phenomenology · Physics 2011-01-17 Linda M. Carpenter , Arvind Rajaraman

In supersymmetric models, the CP asymmetry produced in the decay of the lightest right-handed neutrino, $\equiv epsilon$, can be written as a function of weak scale parameters. We introduce a way of separating epsilon into contributions…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sacha Davidson , Alejandro Ibarra

Any theory that have a global spontaneously broken symmetry will imply the existence of very light neutral bosons or massless bosons (sometimes called Majorons). For most of these models we have neutrino-Majoron couplings, that appear as…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. P. Lessa , O. L. G. Peres

Neutrinos in the Standard Model (SM) are considered to be massless which is in contradiction with the evidence from the neutrino oscillation data. These experiments established that at least two SM neutrinos have non-zero masses and that…

High Energy Physics - Phenomenology · Physics 2019-06-11 Rachik Soualah , Salah Nasri , Safa Naseem

We analyze the structure of quark and lepton mass matrices under the hypothesis that they are determined from a minimum principle applied to a generic potential invariant under the $\left[SU(3)\right]^5\otimes \mathcal O(3)$ flavor…

High Energy Physics - Phenomenology · Physics 2015-06-16 R. Alonso , M. B. Gavela , G. Isidori , L. Maiani

The scenario of baryogenesis through leptogenesis is reviewed in models involving heavy Majorana neutrinos. The various mechanisms of CP violation occurring in the out-of-equilibrium lepton-number-violating decays of heavy Majorana…

High Energy Physics - Phenomenology · Physics 2011-08-17 Apostolos Pilaftsis

Recent considerations by these authors pointed out the attractive features which a search for the exchange of heavy Majorana neutrinos could have for solving the mass and the lepton number puzzles for all neutrinos, in TeV-level…

High Energy Physics - Phenomenology · Physics 2007-05-23 Clemens A. Heusch , Peter Minkowski

Possible existence of "hot-sector generations" above the well known 3 generation bound is investigated on the basis of a model of leptons and quarks, which is based on the Harari and Shupe's one. Our model predicts the existence of {\bf3 +…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kazuo Koike

The Majorana neutrino in type-I seesaw and the pseudo-Dirac neutrinos in the inverse seesaw can have sizable mixings with the light neutrinos in the standard model (SM), through which the heavy neutrinos can be produced at the Large Hadron…

High Energy Physics - Phenomenology · Physics 2016-02-24 Arindam Das , Nobuchika Okada

The seesaw mechanism explains the exclusive smallness of neutrino masses by the presence of very heavy Majorana masses and leads to the appearance of Majorana particles and to the direct lepton number violation. The author proposes a seesaw…

High Energy Physics - Phenomenology · Physics 2020-04-07 Igor T. Dyatlov

We revisit the recent limits from LHCb on a Majorana neutrino N in the mass range 250 - 5000 MeV. These limits are among the best currently available, and they will be improved soon by the addition of data from Run 2 of the LHC. LHCb…

High Energy Physics - Phenomenology · Physics 2017-04-10 Brian Shuve , Michael E. Peskin

The history of research associated with the fundamental problem of the nature of massive neutrinos, which can be Dirac particles or Majorana fermions, and the related processes of neutrinoless double beta decay, $(A,Z)\rightarrow (A,Z+2) +…

High Energy Physics - Phenomenology · Physics 2019-10-22 S. T. Petcov

The predictions for the effective Majorana mass |<m>| in neutrinoless double-beta decay in the case of 3-neutrino mixing and massive Majorana neutrinos are reviewed. The physics potential of the experiments, searching for neutrinoless…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Pascoli , S. T. Petcov

We describe current and future hadron collider limits on new vector-like leptons with exotic decays. We consider the possibility that, besides standard decays, the new leptons can also decay into a Standard Model charged lepton and a stable…

High Energy Physics - Phenomenology · Physics 2022-02-09 Guilherme Guedes , José Santiago

The general Lagrangian containing the couplings of the Higgs scalars to Majorana neutrinos is presented in the context of singlet Majoron models with intergenerational mixings. The analytical expressions for the coupling of the Majoron…

High Energy Physics - Phenomenology · Physics 2008-11-26 Apostolos Pilaftsis

The scale of neutrino mass generation may be too large to explore directly, but useful information may still be extracted from independent experimental channels. Here I survey various model independent probes of Majorana neutrino mass…

High Energy Physics - Phenomenology · Physics 2008-05-05 James Jenkins

Considering the scheme with mixing of three neutrinos and a mass hierarchy that can accommodate the results of solar and atmospheric neutrino experiments, it is shown that the results of solar neutrino experiments imply a lower bound for…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. Giunti

Assuming 3-$\nu$ mixing, massive Majorana neutrinos and neutrinoless double-beta (\betabeta-) decay generated only by the (V-A) charged current weak interaction via the exchange of the three Majorana neutrinos, we briefly review the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Pascoli , S. T. Petcov , T. Schwetz