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We revisit minimal non-supersymmetric models of SU(5) Grand Unification with the type II seesaw mechanism as the origin of neutrino masses. Imposing the requirement of gauge coupling unification and the proton lifetime bounds, we perform a…

High Energy Physics - Phenomenology · Physics 2022-12-02 Lorenzo Calibbi , Xiyuan Gao

The left-right symmetric model with doublet and bi-doublet Higgs scalars can accommodate linear, inverse or double seesaw for generating small neutrino masses in the presence of three singlet fermions. If the singlet fermions have small…

High Energy Physics - Phenomenology · Physics 2010-10-29 Pei-Hong Gu , Utpal Sarkar

The minimal Type I see-saw model cannot explain the observed neutrino masses and the baryon asymmetry of the Universe via hierarchical thermal leptogenesis without ceding naturalness. We show that this conclusion can be avoided by adding a…

High Energy Physics - Phenomenology · Physics 2015-08-26 Jackson D. Clarke , Robert Foot , Raymond R. Volkas

We consider the minimal 3-3-1 model with a heavy scalar sextet and realize, at the tree level, an effective dimension-five interaction that contributes to the mass of the charged leptons. In this case the charged leptons masses arise from a…

High Energy Physics - Phenomenology · Physics 2015-10-22 G. De Conto , A. C. B. Machado , V. Pleitez

Type-I seesaw provides a natural explanation for the tiny neutrino masses. The right-handed neutrino masses it requires are, however, too large to keep the Higgs boson mass at its measured value. Here we show that vector-spinors, singlet…

High Energy Physics - Phenomenology · Physics 2021-12-07 Durmus Demir , Canan Karahan , Ozan Sargın

We construct a model realizing the inverse seesaw mechanism. The model has two types of gauge singlet fermions in addition to right-handed neutrinos. A required Majorana mass scale (keV scale) for generating the light active neutrino mass…

High Energy Physics - Phenomenology · Physics 2015-11-30 Mayumi Aoki , Naoyuki Haba , Ryo Takahashi

Anomaly mediated supersymmetry breaking (AMSB), when implemented in MSSM is known to suffer from the problem of negative slepton mass squared leading to breakdown of electric charge conservation. We show however that when MSSM is extended…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. N. Mohapatra , Nobuchika Okada , Hai-Bo Yu

Baryon and lepton number are excellent low-energy symmetries of the Standard Model (SM) that tightly constrain the form of its extensions. In this paper we investigate the possibility that these accidental symmetries are violated in the…

High Energy Physics - Phenomenology · Physics 2025-12-18 Arnau Bas i Beneito , John Gargalionis , Juan Herrero-Garcia , Michael A. Schmidt

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

We propose an SU(5) GUT model extended with two additional pairs of $\mathbf{10}$ representation vector-like fermions. The CDF collaboration $W$ boson mass anomaly is explained by using the VEV of a real $\mathrm{SU(2)_L}$ triplet scalar…

High Energy Physics - Phenomenology · Physics 2023-08-09 Yusuke Shimizu , Shonosuke Takeshita

There exists a generic minimal tree-level diagram, with two external scalars and a heavy intermediate fermion, that can generate naturally small neutrino masses via a seesaw. This diagram has a mass insertion on the internal fermion line,…

High Energy Physics - Phenomenology · Physics 2013-07-30 Kristian L. McDonald

In this doctoral thesis, we study both low- and high-energy observables related to massive neutrinos. Neutrino oscillations have provided indisputable evidence in favour of non-zero neutrino masses and mixings. However, the original…

High Energy Physics - Phenomenology · Physics 2013-11-25 Cédric Weiland

We extend the $SU(3)_c \times SU(2)_L \times U(1)_Y$ standard model by a $U(1)_{Y'}$ gauge symmetry. Three right-handed neutrinos are introduced to cancel the gauge anomaly. One Higgs singlet is responsible for spontaneously breaking the…

High Energy Physics - Phenomenology · Physics 2023-01-11 Su-Ping Chen , Pei-Hong Gu

We discuss the phenomenology of type-II seesaw by extending the Standard Model with additional Higgs doublets and scalar triplets additionally invoked with $\Delta(27)$ flavor symmetry for the explanation of non-zero neutrino masses and…

High Energy Physics - Phenomenology · Physics 2019-09-05 Itishree Sethi , Sudhanwa Patra

For understanding the hierarchies of fermion masses and mixing, we extend the Standard Model gauge group with \( U(1)_X \) and \( Z_2 \) symmetry. The field content of the Standard Model is augmented by three heavy right-handed neutrinos,…

High Energy Physics - Phenomenology · Physics 2025-02-14 Abdul Rahaman Shaikh , Rathin Adhikari

In a recent re-analysis of the Standard Model (SM) beta-function for the effective neutrino mass operator, we found that the previous results were not entirely correct. Therefore, we consider the analogous dimension five operators in a…

High Energy Physics - Phenomenology · Physics 2009-11-07 Stefan Antusch , Manuel Drees , Joern Kersten , Manfred Lindner , Michael Ratz

In the framework of non-holomorphic modular invariance approach, we have systematically constructed all minimal lepton models based on the non-holomorphic $A^{\prime}_{5}$ modular symmetry from a bottom-up approach. In these models, the…

High Energy Physics - Phenomenology · Physics 2025-09-19 Cai-Chang Li , Gui-Jun Ding

We implement type-II seesaw dominance for neutrino mass and baryogenesis through heavy scalar triplet leptogenesis in a class of minimal non-supersymmetric SO(10) models where matter parity as stabilising discrete symmetry as well as WIMP…

High Energy Physics - Phenomenology · Physics 2020-01-27 Mainak Chakraborty , M. K. Parida , Biswonath Sahoo

We propose a new seesaw model based on fermionic hypercharge zero weak quintuplet in conjunction with additional scalar quadruplet which attains an induced vev. The model provides both tree-level seesaw ~ v^6/M^5 and a loop-suppressed…

High Energy Physics - Phenomenology · Physics 2012-07-26 Kresimir Kumericki , Ivica Picek , Branimir Radovcic

We point out that the minimal seesaw model can provide a natural framework to accommodate tiny neutrino masses, while its experimental testability and notable predictiveness are still maintained. This possibility is based on the observation…

High Energy Physics - Phenomenology · Physics 2010-05-12 He Zhang , Shun Zhou
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