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Proposed symmetry relations, e.g., quark-lepton complementarity (QLC) or tribimaximal mixing (TBM), need to be imposed at a high scale $\wedge \sim 10^{12}$ GeV characterising the large masses of right-handed neutrinos required to implement…

High Energy Physics - Phenomenology · Physics 2008-11-26 Probir Roy

Short-baseline neutrino anomalies suggest the existence of low-mass ( m \sim O(1)~eV) sterile neutrinos \nu_s. These would be efficiently produced in the early universe by oscillations with active neutrino species, leading to a thermal…

Cosmology and Nongalactic Astrophysics · Physics 2014-12-24 Ninetta Saviano , Ofelia Pisanti , Gianpiero Mangano , Alessandro Mirizzi

We study the impact for leptogenesis of new U(1) gauge bosons coupled to the heavy Majorana neutrinos. They can significantly enhance the efficiency of thermal scenarios in the weak washout regime as long as the Z' masses are not much…

High Energy Physics - Phenomenology · Physics 2014-11-18 J. Racker , E. Roulet

We study sterile neutrino dark matter in a minimal Type-I Dirac seesaw framework where the states responsible for generating Dirac neutrino masses at tree level can be viable dark matter candidates. A $\mathcal{Z}_6$ symmetry, spontaneously…

High Energy Physics - Phenomenology · Physics 2026-03-23 J. Adhikary , A. Batra , K. Deka , F. R. Joaquim

We study a type I see-saw scenario where the right-handed (RH) neutrinos, responsible for the light neutrino mass generation, lie at the electroweak scale. Under certain conditions, the strength of the charged and neutral current weak…

High Energy Physics - Phenomenology · Physics 2011-08-08 A. Ibarra , E. Molinaro , S. T. Petcov

Extending the Standard Model with right-handed neutrinos provides a minimal explanation for both light neutrino masses (through the type-I seesaw mechanism) and the baryon asymmetry of our universe (through leptogenesis). We map here for…

High Energy Physics - Phenomenology · Physics 2023-05-12 Yannis Georis

The existence of prolonged radiation domination prior to the Big Bang Nucleosynthesis (BBN), starting just after the inflationary epoch, is not yet established unanimously. If instead, the universe undergoes a non-standard cosmological…

High Energy Physics - Phenomenology · Physics 2022-10-05 Anirban Biswas , Dilip Kumar Ghosh , Dibyendu Nanda

We study constraints on additional $Z'$ bosons predicted in the supersymmetric (SUSY) $E_6$ models by using the updated results of electroweak experiments -- $Z$-pole experiments, $m_W$ measurements and low-energy neutral current (LENC)…

High Energy Physics - Phenomenology · Physics 2009-10-31 Gi-Chol Cho , Kaoru Hagiwara , Yoshiaki Umeda

We consider theories where the Standard Model (SM) neutrinos acquire masses through the seesaw mechanism at the weak scale. We show that in such a scenario, the requirement that any pre-existing baryon asymmetry, regardless of its origin,…

High Energy Physics - Phenomenology · Physics 2010-04-14 Steve Blanchet , Z. Chacko , Rabindra N. Mohapatra

In the context of the Type I seesaw mechanism, we carry out a systematic study of the constraints that result from zeros in both the Dirac and right-handed Majorana neutrino mass matrices. We find that most constraints can be expressed in…

High Energy Physics - Phenomenology · Physics 2015-10-08 Jiajun Liao , D. Marfatia , K. Whisnant

We study the collider phenomenology of the $B$-$L$ extension of the Standard Model (BLSM), focusing on the production and decay of a heavy neutral gauge boson (\( Z' \)) at the Large Hadron Collider (LHC). In this framework, the \( Z' \)…

High Energy Physics - Phenomenology · Physics 2025-08-13 Nidal Chamoun , Kareem Ezzat , Shaaban Khalil , Rhitaja Sengupta

We consider phenomenological constraints on the mass $M_{Z^{\prime}}$ and the two mixing angles $\theta_R$ and $\xi$ of the neutral sector in a very general class of $SU(2)_L \times SU(2)_R \times U(1)$ models using electroweak data. We do…

High Energy Physics - Phenomenology · Physics 2008-11-26 Junegone Chay , Kang Young Lee , Soo-hyeon Nam

A beautiful understanding of the smallness of the neutrino masses may be obtained via the seesaw mechanism, whereby one takes advantage of the key qualitative distinction between the neutrinos and the other fermions: right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2015-06-03 Brian Feldstein , William Klemm

Unlike the standard model where neutrino masses can be made arbitrarily small, we find in the minimal left-right symmetric model that Dirac type Yukawa coupling $h_D \sim 10^{-4.2}$ for $\nu_\tau$ is generated from charged fermion Yukawa…

High Energy Physics - Phenomenology · Physics 2017-04-26 Ravi Kuchimanchi

If future neutrino oscillation experiments show that the neutrino mass spectrum is with normal ordering, m1 < m2 < m3, and the searches for neutrinoless double beta-decay with sensitivity to values of the effective Majorana mass |<m>| >…

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

We investigate the pair production of right-handed neutrinos from the decay of an additional neutral $Z^{\prime}$ boson in the gauged $B-L$ model. Taking into account current constraints on the $Z^{\prime}$ mass and the associated gauge…

High Energy Physics - Phenomenology · Physics 2019-08-14 Frank F. Deppisch , Suchita Kulkarni , Wei Liu

In the type-I seesaw mechanism, both the light Majorana neutrinos (\nu_1, \nu_2, \nu_3) and the heavy Majorana neutrinos (N_1, ..., N_n) can mediate the neutrinoless double-beta (0\nu\beta\beta) decay. We point out that the contribution of…

High Energy Physics - Phenomenology · Physics 2009-09-28 Zhi-zhong Xing

We present the Large Hadron Collider (LHC) discovery potential in the Z' sector of a U(1)_{B-L} enlarged Standard Model also encompassing three heavy Majorana neutrinos, for \sqrt{s}=7 centre-of-mass energy, considering both the…

High Energy Physics - Phenomenology · Physics 2013-05-29 Lorenzo Basso , Alexander Belyaev , Stefano Moretti , Giovanni Marco Pruna , Claire H. Shepherd-Themistocleous

We consider the minimal seesaw model in which two gauge singlet right handed neutrinos with opposite lepton numbers are added to the Standard Model. In this model, the smallness of the neutrino mass is explained by the tiny lepton number…

High Energy Physics - Phenomenology · Physics 2014-05-07 Subrata Khan , Srubabati Goswami , Sourov Roy

We tested several models in which the Standard Model (SM) gauge group is extended by an additional U(1) gauge symmetry, against available electroweak precision data to impose limits on the mass of the neutral Z' boson, M_Z', predicted in…

High Energy Physics - Phenomenology · Physics 2015-05-14 J. Erler , P. Langacker , S. Munir , E. Rojas