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Related papers: One-loop neutrino mass model with $SU(2)_L$ multip…

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We extend the standard model by three types of inert fields including Majorana fermion singlets/triplets, real Higgs singlets/triplets and leptonic Higgs doublets. In the presence of a softly broken lepton number and an exactly conserved…

High Energy Physics - Phenomenology · Physics 2016-09-07 Wen-Bin Lu , Pei-Hong Gu

We propose an extension of the Standard Model by extending the EW symmetry to SU(2)_L x U(1) x Z_2 and introducing three SU(2)_L x U(1) singlet right handed neutrinos, N_R, and an additional Higgs doublet, phi. While the SM gauge bosons and…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Gabriel , S. Nandi

We investigate an one loop radiative neutrino mass model, where the loop particles, notably a singlet fermion ($\chi$), a doublet fermion ($\Psi$) and three generations of singlet scalars ($\phi_i, i=\{1,2,3\}$) are assumed to be odd under…

High Energy Physics - Phenomenology · Physics 2025-11-25 Ujjal Kumar Dey , Santu Kumar Manna , Partha Kumar Paul , Sujit Kumar Sahoo , Narendra Sahu

A new idea for neutrino mass was proposed recently, where its smallness is not due to the seesaw mechanism, i.e. not inversely proportional to some large mass scale. It comes from a one-loop mechanism with dark matter in the loop consisting…

High Energy Physics - Phenomenology · Physics 2013-06-06 Subhaditya Bhattacharya , Ernest Ma , Alexander Natale , Ahmed Rashed

We propose a model where neutrino masses are generated at three loop order but neutrinoless double beta decay occurs at one loop. Thus we can have large neutrinoless double beta decay observable in the future experiments even when the…

High Energy Physics - Phenomenology · Physics 2018-06-21 Julien Alcaide , Dipankar Das , Arcadi Santamaria

We studied a left-right symmetric model that can accommodate the neutrino dark energy (\nd) proposal. Type III seesaw mechanism is implemented to give masses to the neutrinos. After explaining the model, we study the consistency of the…

High Energy Physics - Phenomenology · Physics 2010-04-21 Jitesh R. Bhatt , Pei-Hong Gu , Utpal Sarkar , Santosh K. Singh

In this work, we report on recent analyses of a class of models that generate neutrino mass at the three-loop level. We argue that these models offer a viable solution to both the neutrino mass and dark matter problems, without being in…

High Energy Physics - Phenomenology · Physics 2015-05-19 Amine Ahriche , Kristian L. McDonald , Salah Nasri

We extend the recently proposed gluino axion model to include neutrino masses. We discuss how the canonical seesaw model and the Higgs triplet model may be realized in this framework. In the former case, the heavy singlet neutrinos are…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. A. Demir , Ernest Ma , Utpal Sarkar

In the simplest model of horizontal U(1) symmetry with one singlet added to the supersymmetric standard model, we systematically reconstruct quark mass matrices from the low-energy data to prove that there are only two mass matrices found…

High Energy Physics - Phenomenology · Physics 2015-06-25 E. J. Chun , A. Lukas

We propose the $SU(3)_C\times SU(3)_L\times U(1)_X$ model arising from $SU(6)$ breaking. One family of the Standard Model (SM) fermions arises from two $\bar{6}$ representations and one $15$ representation of $SU(6)$ gauge symmetry. To…

High Energy Physics - Phenomenology · Physics 2020-11-23 Tianjun Li , Junle Pei , Fangzhou Xu , Wenxing Zhang

We present the general form of the unitary matrices keeping invariant the Majorana neutrino mass matrix of specific texture suitable for explaining oscillation data. In the case of the Tri-bimaximal pattern with two degenerate masses we…

High Energy Physics - Phenomenology · Physics 2011-02-01 E. I. Lashin , S. Nasri , E. Malkawi , N. Chamoun

We present a three-loop model of neutrino mass whose most-general Lagrangian possesses a softly-broken accidental $Z_2$ symmetry. In the limit that a single parameter vanishes, $\lambda\rightarrow0$, the $Z_2$ symmetry becomes exact and the…

High Energy Physics - Phenomenology · Physics 2014-11-04 Amine Ahriche , Kristian L. McDonald , Salah Nasri

We discuss a new class of neutrino mass models generated in two loops, and explore specifically three new physics scenarios: (A) doubly charged scalar, (B) dark matter, and (C) leptoquark and diquark, which are verifiable at the 14 TeV LHC…

High Energy Physics - Phenomenology · Physics 2018-04-04 Qing-Hong Cao , Shao-Long Chen , Ernest Ma , Bin Yan , Dong-Ming Zhang

Planck scale lepton number violation is an interesting and natural possibility to explain non-zero neutrino masses. We consider such operators in the context of Randall-Sundrum (RS1) scenarios. Implementation of this scenario with a single…

High Energy Physics - Phenomenology · Physics 2014-06-18 Abhishek M Iyer

We propose a simple $SU(5)$ model that connects the neutrino mass generation mechanism to the observed disparity between the masses of charged leptons and down-type quarks. The model is built out of $5$-, $10$-, $15$-, $24$-, and…

High Energy Physics - Phenomenology · Physics 2020-01-22 Ilja Doršner , Shaikh Saad

We present a class of models with radiative neutrino mass and stable dark-matter candidates. Neutrino mass is generated by a one-loop diagram with the same topography as Ma's 2006 proposal (which used an inert scalar-doublet and singlet…

High Energy Physics - Phenomenology · Physics 2015-06-16 Sandy S. C. Law , Kristian L. McDonald

We propose an extension of the standard model of quarks and leptons to include gauge $B-L$ symmetry with an exotic array of neutral fermion singlets for anomaly cancellation. With the addition of suitable scalars also transforming under…

High Energy Physics - Phenomenology · Physics 2016-09-21 Ernest Ma , Nicholas Pollard , Oleg Popov , Mohammadreza Zakeri

We propose a model with radiatively induced neutrino mass at two-loop level, applying modular $A_4$ symmetry. The neutrino mass matrix is formulated where the structure of associated couplings are restricted by the symmetry. Then we show…

High Energy Physics - Phenomenology · Physics 2021-03-09 Takaaki Nomura , Hiroshi Okada

If there exist only three light neutrinos below the weak scale, the neutrino masses can arise by breaking the lepton number L. One example is the Zee mechanism for the neutrino masses. We study phenomenological implications of neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jihn E. Kim , Jae Sik Lee

When the singlet-doublet fermion dark matter model is extended with additional $Z_2$--odd real singlet scalars, neutrino masses and mixings can be generated at one-loop level. In this work, we discuss the salient features arising from the…

High Energy Physics - Phenomenology · Physics 2015-07-15 Diego Restrepo , Andrés Rivera , Marta Sánchez-Peláez , Oscar Zapata , Walter Tangarife
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