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Related papers: The majoron coupling to charged leptons

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Fundamental mechanisms for Majoron emitting neutrinoless double beta decay in SU(3)_C x G_W x U(1) models, for electroweak flavor chiral extensions, G_W = SU(3)_L and SU(4)_L are pointed out. Both kinds of known Majoron emitting processes,…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. Pisano , S. Shelly Sharma

We discuss a scenario in which the supergravity induced soft terms, conventionally used for breaking supersymmetry, also lead to non-zero Majorana neutrino masses. The soft terms lead to the spontaneous violation of the lepton number at the…

High Energy Physics - Phenomenology · Physics 2024-01-26 Anjan S. Joshipura , Ketan M. Patel

The canonical type-I seesaw model with three heavy Majorana neutrinos is one of the most natural extensions of the standard model (SM) to accommodate tiny Majorana masses of three ordinary neutrinos. At low-energy scales, Majorana neutrino…

High Energy Physics - Phenomenology · Physics 2021-07-01 Di Zhang , Shun Zhou

A basis independent formulation of quark-lepton complementarity is implemented at a high scale for quasidegenerate Majorana neutrinos. It is shown that even with the renormalization group evolution in the minimal supersymmetric standard…

High Energy Physics - Phenomenology · Physics 2009-11-11 Amol Dighe , Srubabati Goswami , Probir Roy

It is proved that true Goldstone bosons develop coherent fields whenever the associated charges of the matter particles are not conserved in a macroscopic scale. The sources of the Goldstone fields are the time rates of quantum number…

High Energy Physics - Phenomenology · Physics 2009-10-30 Luis Bento

We propose a radiative neutrino-mass model by introducing 3 generations of fermion pairs $E^{-(N+1)/2} E^{+(N+1)/2}$ and a couple of multi-charged bosonic doublet fields $\Phi_{N/2}, \Phi_{N/2+1}$, where $N=1,3,5,7,9$. We show that the…

High Energy Physics - Phenomenology · Physics 2018-04-25 Kingman Cheung , Hiroshi Okada

Lepton number violation processes can be induced by the Majorana neutrino exchange, which provide evidence for the Majorana nature of neutrinos. In addition to the natural explanation of the small neutrino masses, Type-I seesaw mechanism…

High Energy Physics - Phenomenology · Physics 2019-01-14 Hong-lei Li , Peng-cheng Lu , Cong-feng Qiao , Zong-guo Si , Ying Wang

I review the origin of the lepton asymmetry which is converted to a baryon excess at the electroweak scale. This scenario becomes more attractive if we can relate it to other physical phenomena. For this reason I elaborate on the conditions…

High Energy Physics - Phenomenology · Physics 2009-11-07 E. A. Paschos

We discuss the phenomenology of a light U(1) gauge boson, $\gamma_B$, that couples only to baryon number. Gauging baryon number at high energies can prevent dangerous baryon-number violating operators that may be generated by Planck scale…

High Energy Physics - Phenomenology · Physics 2008-02-03 Christopher D. Carone , Hitoshi Murayama

Leptogenesis is considered in its natural context where Majorana neutrinos fit in a gauge unification scheme and therefore couple to some extra gauge bosons. The masses of some of these gauge bosons are expected to be similar to those of…

High Energy Physics - Phenomenology · Physics 2009-11-10 N. Cosme

It is shown that a true Nambu-Goldstone (NG) boson develops a coherent long-range field whenever the charge associated with it that is carried by the other particles is not conserved in a macroscopic scale. The source of a NG field is the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Luis Bento

The possible Majorana nature of neutrinos leads to lepton-number-violating effects such as neutrinoless double beta decay. The standard study of this process involves mass-dependent matrix elements which, although easy to use, might be…

High Energy Physics - Phenomenology · Physics 2025-05-26 Vaisakh Plakkot

Lepton-number violation (LNV), in general, implies nonzero Majorana masses for the Standard Model neutrinos. Since neutrino masses are very small, for generic candidate models of the physics responsible for LNV, the rates for almost all…

High Energy Physics - Phenomenology · Physics 2019-10-30 André de Gouvêa , Wei-Chih Huang , Johannes König , Manibrata Sen

Assuming Majorana nature of neutrinos, we re-investigate, in the light of the recent measurement of the reactor mixing angle, the allowed ranges for the absolute values of the elements of the neutrino mass matrix in the basis where the…

High Energy Physics - Phenomenology · Physics 2015-06-11 Walter Grimus , Patrick Otto Ludl

Scotogenic models constitute an appealing solution to the generation of neutrino masses and to the dark matter mystery. In this work we consider a version of the Scotogenic model that breaks lepton number spontaneously. At this scope, we…

High Energy Physics - Phenomenology · Physics 2023-12-21 Valentina De Romeri , Jacopo Nava , Miguel Puerta , Avelino Vicente

We recently showed that a new gauge boson $\gamma_B$ coupling only to baryon number is phenomenologically allowed, even if $m_B<m_Z$ and $\alpha_B \approx 0.2$. In our previous work we assumed that kinetic mixing between the baryon number…

High Energy Physics - Phenomenology · Physics 2016-09-01 Christopher D. Carone , Hitoshi Murayama

Instead of anchoring the seesaw mechanism with the conventional heavy right-handed neutrino singlet, a small Majorana neutrino mass may be obtained just as well with the addition of a heavy triplet of leptons per family to the minimal…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma

We explore the possibility of interpreting the solar and atmospheric neutrino data within the context of the Minimal Supersymmetric Standard Model augmented by a single U(1) anomalous family symmetry spontaneously broken by non-zero vacuum…

High Energy Physics - Phenomenology · Physics 2009-11-10 G. K. Leontaris , J. Rizos , A. Psallidas

We derive strong contraints on the Yukawa couplings and the vacuum expectation value in the singlet majoron model, taking into account the possibility of a small gravitationally induced mass for the majoron. If the present baryon asymmetry…

High Energy Physics - Phenomenology · Physics 2009-09-15 James M. Cline , Kimmo Kainulainen , Keith A. Olive

We derive expressions for the neutrino mixing parameters that result from complex perturbations on (1) the Majorana neutrino mass matrix (in the basis of charged lepton mass eigenstates) and on (2) the charged lepton mass matrix, for…

High Energy Physics - Phenomenology · Physics 2015-10-07 Jiajun Liao , D. Marfatia , K. Whisnant
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