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We present a Dirac mass model based on $A_{4}$ modular symmetry within Type-I seesaw framework. This extension of Standard Model requires three right-handed neutrinos and three heavy Dirac fermions superfields, all singlet under $SU(2)_{L}$…

High Energy Physics - Phenomenology · Physics 2024-08-28 Labh Singh , Monal Kashav , Surender Verma

In this paper, we construct a model with the help of modular symmetry in the framework of minimal inverse seesaw [ISS(2,3)]. We have used $\Gamma(3)$ modular group which is isomorphic to non-Abelian discrete symmetry group $A_4$. In this…

High Energy Physics - Phenomenology · Physics 2023-05-03 Jotin Gogoi , Nayana Gautam , Mrinal Kumar Das

We derive formulae for neutrino masses and mixing angles in a type I seesaw framework with an underlying A4 flavor symmetry. In particular, the Majorana neutrino mass matrix includes contributions from an A4 triplet, 1, 1', and 1" flavon…

High Energy Physics - Phenomenology · Physics 2013-02-22 Mu-Chun Chen , Jinrui Huang , Jon-Michael O'Bryan , Alexander M. Wijangco , Felix Yu

We introduce a lepton mass generation and flavor mixing model, realized through a (2,3) inverse seesaw structure based on modular \( S_4 \) symmetry. The model employs modular forms to construct the lepton Yukawa couplings, significantly…

High Energy Physics - Phenomenology · Physics 2025-09-23 Abhishek , V. Suryanarayana Mummidi

We propose a predictive model based on the $SU(3)_C\times SU(3)_L\times U(1)_X$ gauge symmetry, which is supplemented by the $D_4$ family symmetry and several auxiliary cyclic symmetries whose spontaneous breaking produces the observed SM…

High Energy Physics - Phenomenology · Physics 2022-09-02 A. E. Cárcamo Hernández , H. N. Long , M. L. Mora-Urrutia , N. H. Thao , V. V. Vien

We propose a lepton model under modular $A_4$ and gauged $U(1)_R$ symmetries, in which the neutrino masses are induced at one-loop level. Thanks to the modular $A_4$ symmetry, we have several predictions on the lepton sector, especially, on…

High Energy Physics - Phenomenology · Physics 2020-10-08 Keiko I. Nagao , Hiroshi Okada

We propose a flavour model based on an $A_4$ symmetry combined with a type-II seesaw mechanism for neutrino mass generation. The resulting neutrino mass matrix obeys a sum rule that, together with the measured mass-squared differences,…

High Energy Physics - Phenomenology · Physics 2026-03-16 Salvador Centelles Chuliá , Ranjeet Kumar

We combine $SO(10)$ Grand Unified Theories (GUTs) with $A_4$ modular symmetry and present a comprehensive analysis of the resulting quark and lepton mass matrices for all the simplest cases. We focus on the case where the three fermion…

High Energy Physics - Phenomenology · Physics 2021-11-24 Gui-Jun Ding , Stephen F. King , Jun-Nan Lu

We study flavor phenomenologies in a basis of a double covering of modular $A_4$ group with a hidden $SU(2)$ symmetry, in which we work on regions at nearby two fixed points and three special points. These special points of…

High Energy Physics - Phenomenology · Physics 2023-10-27 Keiya Ishiguro , Takaaki Nomura , Hiroshi Okada , Yuta Orikasa , Hajime Otsuka

After developing a general criterion for deciding which neutrino mass models belong to the category of inverse seesaw models, we apply it to obtain the Dirac analogue of the canonical Majorana inverse seesaw model. We then generalize the…

High Energy Physics - Phenomenology · Physics 2020-11-16 Salvador Centelles Chuliá , Rahul Srivastava , Avelino Vicente

Motivated by string constructions, we consider a variant on the Type II see-saw mechanism involving the exchange of triplet representations of SU(2)_L in which this group arises from a diagonal embedding into SU(2)_A x SU(2)_B. A natural…

High Energy Physics - Phenomenology · Physics 2009-11-11 Paul Langacker , Brent D. Nelson

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

We propose a new inverse seesaw model based on hidden local $U(1)$ symmetry framework where inverse seesaw mechanism is induced at one loop level. A Majorana mass term of singlet fermion is forbidden by the $U(1)$ symmetry and it is…

High Energy Physics - Phenomenology · Physics 2025-12-09 Takaaki Nomura , Hiroshi Okada

We propose a radiative seesaw model based on a modular $A_4$ symmetry, which has good predictability in the lepton sector. We execute a numerical analysis to search for parameters that satisfy the experimental constraints such as those from…

High Energy Physics - Phenomenology · Physics 2020-12-02 Hiroshi Okada , Yutaro Shoji

We proposed a viable and predictive model based on the $SU(3)_C \times SU(3)_L \times U(1)_X$ gauge symmetry, supplemented by the global $U(1)_{Lg}$ symmetry, the $S_4$ family symmetry and several auxiliary cyclic symmetries, which…

High Energy Physics - Phenomenology · Physics 2024-06-14 A. E. Cárcamo Hernández , Juan Marchant González , M. L. Mora-Urrutia , Daniel Salinas-Arizmendi

We propose an interesting assignment of positive modular wights for fields in a modular non-Abelian discrete flavor symmetry. By this assignment, we can construct inverse seesaw and linear seesaw models without any additional symmetries…

High Energy Physics - Phenomenology · Physics 2023-10-17 Tatsuo Kobayashi , Takaaki Nomura , Hiroshi Okada , Hajime Otsuka

We propose an A_4 flavor-symmetric SU(3)xSU(2)xU(1) seesaw model where lepton number is broken spontaneously. A consistent two-zero texture pattern of neutrino masses and mixing emerges from the interplay of type-I and type-II seesaw…

High Energy Physics - Phenomenology · Physics 2014-11-21 J. N. Esteves , F. R. Joaquim , A. S. Joshipura , J. C. Romao , M. A. Tortola , J. W. F. Valle

We extend the littlest modular seesaw to a Grand Unified scenario based on $SU(5)$ endowed with three modular $S_4$ symmetries. We leverage symmetry protected zeroes in the leptonic and down quark sectors to suppress deviations to the…

High Energy Physics - Phenomenology · Physics 2023-09-29 Ivo de Medeiros Varzielas , Steve F. King , Miguel Levy

A previous short analysis of the seesaw mechanism, based on quark-lepton symmetry, experimental data and hierarchical neutrino spectrum, is enlarged to include small but not zero U_{e3}, inverted mass hierarchy, and the qualitative effect…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Falcone

A new and novel idea for a predictive neutrino mass matrix is presented, using the non-Abelian discrete symmetry A(4) and the seesaw mechanism with only two heavy neutral fermion singlets. Given the components of the one necessarily…

High Energy Physics - Phenomenology · Physics 2015-06-11 Ernest Ma