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Related papers: Heavy Majorana neutrinos in e^-e^- collisions

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The cross section for the reaction $e^{-}e^{-} \to \ell^-\ell^-$ ($\ell=\mu,\tau$) is calculated in models with heavy Majorana neutrinos mediating lepton number violating amplitudes at the loop level. The contributing four-point functions…

High Energy Physics - Phenomenology · Physics 2011-09-13 M. Cannoni , St. Kolb , O. Panella

We study the process $e^+e^- \to W^+W^-$ with the aim of estimating the prospects for observing heavy neutrinos contributions at future $e^+e^-$-colliders. In this work, we consider two implementations of heavy-light neutrino mixing: a…

High Energy Physics - Phenomenology · Physics 2026-04-07 G. A. Chachava , S. I. Godunov

We examine two processes, the neutrino production process e^+e^- ---> N\nu and the inverse neutrinoless double-beta decay process e^-e^- --->W^-W^- as possible places for discovering heavy neutrinos in future lepton linear colliders. The…

High Energy Physics - Phenomenology · Physics 2009-10-28 J. Gluza , M. Zralek

Right-handed (RH) Majorana neutrinos play a crucial role in understanding the origin of neutrino mass, the nature of dark matter and the mechanism of matter-antimatter asymmetry. In this work, we investigate the observability of heavy…

High Energy Physics - Phenomenology · Physics 2020-05-11 Ning Liu , Zong-guo Si , Lei Wu , Hang Zhou , Bin Zhu

In the framework of the left-right symmetric model the CP-parity violation has been studied in heavy Majorana neutrino decays $N\rightarrow e^{\mp} \mu^{\pm} n$. The numerical estimates of CP-asymmetry for different masses of neutrino and…

High Energy Physics - Phenomenology · Physics 2010-11-01 R. A. Alanakyan , H. M. Asatrian , A. N. Ioannisian , S. A. Chatrchyan

We examine the e-e- -> W-W- lepton number violating process in the frame of the Standard Model with additional right-handed neutrino singlets. We give results in the framework of the `see-saw' as well as other models, where there is no…

High Energy Physics - Phenomenology · Physics 2009-10-28 J. Gluza , M. Zralek

Whether in nature exists Majorana neutrino is one of the most fundamental questions in physics. It is directly related to the violation of accidental $U(1)$-lepton number symmetry(LNV). Enormous efforts had been put into such test and among…

High Energy Physics - Phenomenology · Physics 2017-04-19 Kai Wang , Tao Xu , Liangliang Zhang

We study potential contribution of the heavy right-handed neutrino exchange in the process $e^{+}e^{-} \rightarrow W^{+}W^{-}$. This process is sensitive to heavy neutrinos with masses larger than $\sqrt{s}$. The Monte Carlo simulation of…

High Energy Physics - Phenomenology · Physics 2025-01-28 A. Drutskoy , E. Vasenin

We revisit the sensitivity to non-resonant, heavy Majorana neutrinos $N$ in same-sign $W^\pm W^\pm$ scattering at the $\sqrt{s}=13$ TeV LHC and its high-luminosity upgrade. As a benchmark scenario, we work in the context of the…

High Energy Physics - Phenomenology · Physics 2021-03-11 Benjamin Fuks , Jonas Neundorf , Krisztian Peters , Richard Ruiz , Matthias Saimpert

A search is performed for a heavy Majorana neutrino (N), produced by leptonic decay of a W boson propagator and decaying into a W boson and a lepton, with the CMS detector at the LHC. The signature used in this search consists of two…

High Energy Physics - Experiment · Physics 2019-01-25 CMS Collaboration

Vector boson fusion processes become increasingly more important at higher collider energies and for probing larger mass scales due to collinear logarithmic enhancements of the cross section. In this context, we revisit the production of a…

High Energy Physics - Phenomenology · Physics 2015-02-27 Daniel Alva , Tao Han , Richard Ruiz

A search is performed for heavy Majorana neutrinos (N) using an event signature defined by two same-sign charged leptons of the same flavour and two jets. The data correspond to an integrated luminosity of 4.98 inverse femtobarns of pp…

High Energy Physics - Experiment · Physics 2013-03-13 CMS Collaboration

We consider the reaction ee -> q,q,qbar,qbar as a test of lepton number non-conservation in the framework of the left-right-symmetric electroweak model. The main contributions to this process are due to Majorana neutrino exchange in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jukka Maalampi , Nikolai Romanenko

The determination of CP violating phases in the Majorana neutrino mixing matrix using phenomenological constraints from neutrino oscillations, neutrinoless double beta decay, ($\mu^-, e^+$) conversion and few other processes is discussed.…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. K. Samal

We have studied mixing and masses of three left handed Majorana neutrinos in the model, which assumes exactly degenerate neutrino masses at some "neutrino unification" scale. Such a simple theoretical ansatz naturally leads to…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. N. Ioannisian , N. A. Kazarian

A charged Higgs pair can be produced at an ee collider through a t-channel exchange of a heavy neutrino (N) via e^+ e^- -> H^+ H^- and, if N is a Majorana particle, also via the lepton number violating (LNV) like-sign reaction e^\pm e^\pm…

High Energy Physics - Phenomenology · Physics 2008-11-26 David Atwood , Shaouly Bar-Shalom , Amarjit Soni

In the minimal extension of the standard electroweak theory with ultra massive Majorana neutrinos, the process e- + e- -> mu- + mu- could be observable, in sharp contrast with the reaction e- + e- -> W- + W- which is entirely controlled by…

High Energy Physics - Phenomenology · Physics 2009-10-31 X. Y. Pham

Majorana CP violating phases coming from heavy right-handed Majorana mass matrices ($M_{RR}$) are considered to estimate the masses of neutrinos.The effects of phases on quasi-degenerate neutrinos mass matrix obeying $\mu$-$\tau$ symmetry…

High Energy Physics - Phenomenology · Physics 2023-11-28 Ng. K. Francis

The Standard Model of particle physics is still lacking an understanding of the generation and nature of neutrino masses. A favorite theoretical scenario (the see-saw mechanism) is that both Dirac and Majorana mass terms are present,…

High Energy Physics - Experiment · Physics 2019-08-14 Alain Blondel , E. Graverini , N. Serra , M. Shaposhnikov

We consider the Standard Model with right-handed neutrinos to explain the masses of active neutrinos by the seesaw mechanism. Since active neutrinos as well as heavy neutral leptons are Majorana fermions in this case, the lepton number…

High Energy Physics - Phenomenology · Physics 2016-01-15 Takehiko Asaka , Takanao Tsuyuki