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We analyze the connection between electric dipole moment of the electron and the soft leptogenesis in supersymmetric $B-L$ extension of the standard model. In this model, the $B-L$ symmetry is radiatively broken at TeV scale. Therefore, it…

High Energy Physics - Phenomenology · Physics 2010-04-15 Yuji Kajiyama , Shaaban Khalil , Martti Raidal

An attractive explanation for non-zero neutrino masses and small matter antimatter asymmetry of the present Universe lies in "leptogenesis". At present the {\it size} of the lepton asymmetry is precisely known, while the {\it sign} is not…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kaushik Bhattacharya , Narendra Sahu , Utpal Sarkar , Santosh K. Singh

If new sequential leptons $E^\pm$ and $N^0$ exist, the LEP bound implies $m_E$, $m_N > M_Z/2$. The heaviness of the neutral lepton breaks away from the pattern of the first three generations. The minimal model is to have 4 left-handed…

High Energy Physics - Phenomenology · Physics 2009-10-22 Wei-Shu Hou , Gwo-Guang Wong

A typical problem of the leptogenesis scenario is the mismatch between the maximum reheat temperature implied by gravitino overproduction bound and the minimum temperature required to create thermally the lightest right-handed neutrino. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 Lotfi Boubekeur

Leptogenesis is studied within the seesaw neutrino mass model in a regime where all sterile neutrinos have prompt rather than delayed decays. It is shown that during neutrino thermal production lepton asymmetries are generated in both…

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

Minimal gauged U(1)$_{L_{\mu}-L_{\tau}}$ models can provide for an additional source for the muon anomalous magnetic moment however it is difficult to accommodate the discrepancy in the electron magnetic moment in tandem. Owing to the…

High Energy Physics - Phenomenology · Physics 2021-04-07 Heerak Banerjee , Bhaskar Dutta , Sourov Roy

We revisit the Affleck-Dine leptogenesis via the $L H_u$ flat direction with a light slepton field. Although the light slepton field is favored in low-energy SUSY phenomenologies, such as the muon $g-2$ anomaly and bino-slepton…

High Energy Physics - Phenomenology · Physics 2023-07-12 Kazuki Enomoto , Koichi Hamaguchi , Kohei Kamada , Juntaro Wada

An anomaly-free U(1) charge $Q'$ has recently been identified within the group E$_6$ for which the familiar leptons (the left- and right-handed electron and the left-handed neutrino) have $Q' = 0$. It is pointed out that the $Q'$ charges of…

High Energy Physics - Phenomenology · Physics 2009-10-28 Jonathan L. Rosner

We consider a gauge model based on $SU(3)\otimes U(1)$ symmetry in which the lepton number is violated explicitly by charged scalar and gauge bosons, including a vector field with double electric charge. Although there exist in the…

High Energy Physics - Phenomenology · Physics 2009-07-28 F. Pisano , V. Pleitez

We argue that fast interactions of the lightest singlet neutrino $N_1$ would project part of a preexisting lepton asymmetry $L_p$ onto a direction that is protected from $N_1$ washout effects, thus preventing it from being erased. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 Guy Engelhard , Yuval Grossman , Enrico Nardi , Yosef Nir

We apply a model-independent, agnostic approach to the collider phenomenology of supersymmetry (SUSY), in which all mass parameters are taken as free inputs at the weak scale. We consider the gauginos, higgsinos, and the first two…

High Energy Physics - Phenomenology · Physics 2010-12-03 Partha Konar , Konstantin T. Matchev , Myeonghun Park , Gaurab K. Sarangi

In split-family SUSY, one can use a U(2)^3 symmetry to protect flavour observables in the quark sector from SUSY contributions. However, attempts to extend this procedure to the lepton sector by using an analogous U(2)^5 symmetry fail to…

High Energy Physics - Phenomenology · Physics 2015-06-17 Joel Jones-Perez

Within low scale theories traditional see-saw and scalar triplet mechanisms, for neutrino mass suppression, do not work out anymore and for realistic model building some new ideas are needed. In this paper we suggest mechanism, different…

High Energy Physics - Phenomenology · Physics 2016-09-06 Zurab Tavartkiladze

Some versions of the electroweak SU(3)$_L\otimesU(1)_X$ models cannot be treated within perturbation theory at energies of few TeV. An extended version for these models is proposed which is perturbative even at TeV scale posing no…

High Energy Physics - Phenomenology · Physics 2009-11-10 Alex G. Dias

A detailed analytic and numerical study of baryogenesis through leptogenesis is performed in the framework of the standard model of electroweak interactions extended by the addition of three right-handed neutrinos, leading to the seesaw…

High Energy Physics - Phenomenology · Physics 2011-07-19 G. C. Branco , R. Gonzalez Felipe , F. R. Joaquim , M. N. Rebelo

Lepton generation universality holds very well in Z decays, but appears to be violated in recent LEP data of W leptonic decay branching fractions. If this trend persists, a consistent and natural explanation is a model of generation…

High Energy Physics - Phenomenology · Physics 2007-05-23 Xiao-Yuan Li , Ernest Ma

An extension of the Standard Model to the local gauge group SU(3)_c X SU(3)_L X U(1)_X as a family independent model is presented. The mass scales, the gauge boson masses and the masses for the spin 1/2 particles in the model are studied.…

High Energy Physics - Phenomenology · Physics 2011-03-23 R. Martinez , William A. Ponce , Luis A. Sanchez

We investigate the possibility that a minimal realization of left-right supersymmetry can be reachable at a high-energy upgrade of the LHC, expected to operate at a center-of-mass energy of 27 TeV. This minimal scenario has a relatively…

High Energy Physics - Phenomenology · Physics 2020-07-01 Mariana Frank , Benjamin Fuks , Katri Huitu , Subhadeep Mondal , Santosh Kumar Rai , Harri Waltari

In this letter we consider that assuming: a) that the only left-handed neutral fermions are the active neutrinos, b) that $B-L$ is a gauge symmetry, and c) that the $L$ assignment is restricted to the integer numbers, the anomaly…

High Energy Physics - Phenomenology · Physics 2009-05-29 J. C. Montero , V. Pleitez

In the context of the minimal supersymmetric seesaw model, the CP-violating neutrino Yukawa couplings might induce an electron EDM. The same interactions may also be responsible for the generation of the observed baryon asymmetry of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. R. Joaquim , I. Masina , A. Riotto