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Related papers: High-dimensional neutrino masses

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M-theory compactified on a $G_2$ manifold with resolved $E_8$ singularity is a promising candidate for a unified theory. The experimentally observed masses of quarks and charged leptons put a restriction on the moduli of the $G_2$ manifold.…

High Energy Physics - Theory · Physics 2022-03-14 Eric Gonzalez , Gordon Kane , Khoa Nguyen

We obtain the complete and independent bases of effective operators at mass dimension 5, 6, 7, 8, 9 in both standard model effective field theory with light sterile right-handed neutrinos ($\nu$SMEFT) and low energy effective field theory…

High Energy Physics - Phenomenology · Physics 2021-11-24 Hao-Lin Li , Zhe Ren , Ming-Lei Xiao , Jiang-Hao Yu , Yu-Hui Zheng

We study a mechanism where tiny neutrino masses arise only from radiative contribution in a supersymmetric model. In each generation, the tree-level light neutrino mass is rotated away by introducing a second SM singlet $s_{L}$ that forms a…

High Energy Physics - Phenomenology · Physics 2011-06-28 Seong Chan Park , Kai Wang

The implications of a large value of the effective Majorana neutrino mass for a class of two texture zero neutrino mass matrices have been studied in the flavor basis. It is found that these textures predict near maximal atmospheric…

High Energy Physics - Phenomenology · Physics 2014-08-06 S. Dev , Radha Raman Gautam , Lal Singh , Manmohan Gupta

We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upper bound is $4\pi v^2/\sqrt 3 m_\nu$, where $v \simeq 246$ GeV is the weak scale and $m_\nu$ is the Majorana neutrino mass. For neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. M. Niczyporuk

We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upper bound is $4\pi v^2/\sqrt 3 m_\nu$, where $v \simeq 246$ GeV is the weak scale and $m_\nu$ is the Majorana neutrino mass. For neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. Maltoni , J. M. Niczyporuk , S. Willenbrock

If the neutrino is Majorana type and the electroweak phase transition is second or weak first order, neutrino-induced interactions together with sphaleron transitions have the potential to erase a previously generated baryon asymmetry of…

High Energy Physics - Phenomenology · Physics 2009-10-31 H. V. Klapdor-Kleingrothaus , St. Kolb , U. Sarkar

Recently, Majorana's spirit returns to modern condensed matter physics -- in the context of topological Majorana zero mode that represents a local half degree of freedom carrying non-Abelian statistics.In this paper, we investigate the…

High Energy Physics - Phenomenology · Physics 2014-04-08 Zheng-Cheng Gu

Starting from a complete set of possible parametrisations of the quark-mass matrices that have the maximum number of texture zeros at the grand unification scale, and the Georgi-Jarlskog mass relations, we classify the neutrino spectra with…

High Energy Physics - Phenomenology · Physics 2015-06-25 E. Papageorgiu

A simple extension of the Standard Model providing TeV scale seesaw mechanism is presented. Beside the Standard Model particles and right-handed Majorana neutrinos, the model contains a singly charged scalar, an extra Higgs doublet and…

High Energy Physics - Phenomenology · Physics 2010-11-03 Wei Chao

One puzzle of neutrino masses and mixings is that they do not exhibit the kind of strong "hierarchy" that is found for the quarks and charged leptons. Neutrino mass ratios and mixing angles are not small. A possible reason for this is…

High Energy Physics - Phenomenology · Physics 2011-05-12 S. M. Barr

We consider a class of models in which the neutrinos acquire Majorana masses through mixing with singlet neutrinos that emerge as composite states of a strongly coupled hidden sector. In this framework, the light neutrinos are partially…

High Energy Physics - Phenomenology · Physics 2021-03-16 Zackaria Chacko , Patrick J. Fox , Roni Harnik , Zhen Liu

We study neutrino masses and mixing in R-parity violating supersymmetric models with generic soft supersymmetry breaking terms. Neutrinos acquire masses from various sources: Tree level neutrino--neutralino mixing and loop effects…

High Energy Physics - Phenomenology · Physics 2009-11-10 Yuval Grossman , Subhendu Rakshit

The possibility of generating neutrino mass through see-saw mechanism involving U(1) chiral Peccei-Quinn and scale symmetries breakdown is discussed. We consider a generic scale invariant model which has three Majorana fermions and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alex Gomes Dias

Theories beyond the Standard Model must necessarily respect its gauge symmetry. This implies strict constraints on the possible models of non-standard neutrino interactions, which we analyze. The focus is set on the effective low-energy…

High Energy Physics - Phenomenology · Physics 2009-10-23 M. B. Gavela , D. Hernandez , T. Ota , W. Winter

In this work, we explore the proposed mechanism in which the gravitational $\theta$ anomaly generates neutrino masses. We highlight that the leading renormalizable interactions of the neutrino condensate forbid the possibility of generating…

High Energy Physics - Phenomenology · Physics 2023-05-10 Carlos Henrique de Lima , Daniel Stolarski

A minimal and predictive neutrino mass matrix texture for Majorana neutrino is proposed. The texture favours the normal hierarchy of neutrino mass eigenvalues. It further predicts the octant of $\theta_{23}$, constraints $\delta$, gives…

High Energy Physics - Phenomenology · Physics 2026-05-19 Sagar Tirtha Goswami , Pralay Chakraborty , Subhankar Roy

We study neutrino physics in a 5D supersymmetric SO(10) GUT. We analyze several different choices for realizing the See-Saw mechanism. We find that the "natural" scale for the Majorana mass of right-handed neutrinos depends critically on…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hyung Do Kim , Stuart Raby

The strong CP problem can be solved in Parity symmetric theories with electroweak gauge group containing $SU(2)_L \times SU(2)_R$ broken by the minimal Higgs content. Neutrino masses may be explained by adding the same number of gauge…

High Energy Physics - Phenomenology · Physics 2023-11-20 Lawrence J. Hall , Keisuke Harigaya , Yogev Shpilman

A new mechanism for generating neutrino masses without a high-energy mass scale is proposed. The mechanism needs a fundamental mass scale M in the 100-1000 TeV region and a minimal field content beyond the Standard Model one containing a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Emilian Dudas , Carlos A. Savoy