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Related papers: B-L-violating Masses in Softly Broken Supersymmetr…

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A simple model of the Majorana neutrino with the see-saw mechanism is studied, assuming that two light neutrinos are the hot dark matters with equal mass of 2.4 eV in the cold plus hot dark matter model of cosmology. We find that the heavy…

High Energy Physics - Phenomenology · Physics 2009-10-28 Noriaki Kitazawa , Nobuchika Okada , Shin Sasaki

In the conventional gauged ${B-L}$ extension of the standard model, the $B-L$ charge of the singlet scalar $\chi$, responsible for the breaking of $U(1)_{B-L}$ symmetry, is taken to be 2 such that it can anchor type-I seesaw by giving…

High Energy Physics - Phenomenology · Physics 2026-01-12 Ernest Ma , Partha Kumar Paul , Narendra Sahu

We show that Dirac neutrino masses of the right size can arise from the Kahler potential of supergravity. They are proportional to the supersymmetry and the electroweak breaking scales. We find that they have the experimentally observed…

High Energy Physics - Phenomenology · Physics 2009-11-10 Steven Abel , Athanasios Dedes , Kyriakos Tamvakis

It is shown that a certain sum rule for soft supersymmetry-breaking scalar masses, which has been recently found in a certain class of superstring models, is universal for gauge-Yukawa unified models. To explain this coincidence, we argue…

High Energy Physics - Phenomenology · Physics 2009-10-30 Yoshiharu Kawamura , Tatsuo Kobayashi , Jisuke Kubo

There are strong indications for neutrino masses and mixings in the data on solar neutrinos as well as in the observed deficit of muon neutrinos from the atmosphere. The COBE data and other analysis of the large scale structure in the…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. N. Mohapatra

Majorana masses of the neutrino implies lepton number violation and is intimately related to the lepton asymmetry of the universe, which gets related to the baryon asymmetry of the universe in the presence of the sphalerons during the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Utpal Sarkar

If the present or upcoming searches for neutrinoless double beta decay give a positive result, the Majorana nature of massive neutrinos will be established. From the determination of the value of the effective Majorana mass parameter |<m>|,…

High Energy Physics - Phenomenology · Physics 2015-06-25 S. Pascoli , S. T. Petcov

Theories in which neutrino masses are generated by a conventional see-saw mechanism generically yield masses which are O(v^2) in units where M_{Pl}=1, which is naively too small to explain the results from SuperKamiokande. In supersymmetric…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nima Arkani-Hamed , Lawrence Hall , Hitoshi Murayama , David Smith , Neal Weiner

Neutrinoless double beta decay is a promising test for lepton number violating physics beyond the standard model of particle physics. There is a deep connection between this decay and the phenomenon of neutrino masses. In particular, we…

High Energy Physics - Phenomenology · Physics 2012-07-30 Michael Duerr

We show that a recently proposed extension of the MSSM can provide a scenario where both the cold and hot dark matter of the universe owe their origin to a single scale connected with the breakdown of the global B-L symmetry. The susy…

High Energy Physics - Phenomenology · Physics 2009-10-28 R. N. Mohapatra , A. Riotto

R-parity-violating supersymmetry (with a conserved baryon number B) provides a framework for particle physics with lepton number (L) violating interactions. We examine in detail the structure of the most general R-parity-violating…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yuval Grossman , Howard E. Haber

It is often said that neutrino mass is a window to a new physics beyond the standard model (SM). This is certainly true if neutrinos are Majorana particles since the SM with Majorana neutrino mass is not a complete theory. The classical…

High Energy Physics - Phenomenology · Physics 2010-03-25 Goran Senjanovic

We show that Majorana neutrinos convert into antineutrinos in a background of ultralight vector dark matter coupled to lepton number, such as the gauge boson of $\text{U}(1)_{B-L}$ or $\text{U}(1)_{L_i - L_j}$ with $i, j = e , \mu, \tau$.…

High Energy Physics - Phenomenology · Physics 2026-05-11 Asher Berlin , Rodolfo Capdevilla , Ting Cheng , Matheus Hostert , Pedro A. N. Machado

Renormalizable lepton number violating interactions that break R-parity can induce a Majorana mass for neutrinos. Based on this, we show that it is possible to obtain a phenomenologically viable neutrino mass matrix that can accommodate…

High Energy Physics - Phenomenology · Physics 2009-12-30 M. Drees , S. Pakvasa , X. Tata , T. ter Veldhuis

We point out a connection between R symmetry and \susy\ breaking. We show that the existence of an R symmetry is a necessary condition for \susy\ breaking and a spontaneously broken R symmetry is a sufficient condition provided two…

High Energy Physics - Phenomenology · Physics 2009-09-15 Ann E. Nelson , Nathan Seiberg

Bilinear R-parity violating supersymmetric model is a viable model which can explain the smallness of neutrino masses and the mixing pattern in the lepton sector. In this model, there is a common set of parameters which determine the…

High Energy Physics - Phenomenology · Physics 2011-07-08 R. S. Hundi

A natural extension of the standard $SU(2)_{\rm L} \times U(1)_{\rm Y}$ gauge model to accommodate massive neutrinos is to introduce one Higgs triplet and three right-handed Majorana neutrinos, leading to a $6\times 6$ neutrino mass matrix…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei Chao , Shu Luo , Zhi-zhong Xing , Shun Zhou

We study the phenomenology of supersymmetric models that explain neutrino masses through the spontaneous breaking of R-parity, finding strong correlations between the decays of the lightest neutralino and the neutrino mixing angles. In…

High Energy Physics - Phenomenology · Physics 2009-07-22 A. Vicente

We consider an Supersymmetric extension of the Standard Model with some extra Higgs doublets and a global $(B - L)$, where $B$ and $L$ are the usual baryonic and lepton number respectivelly, and ${\cal Z}_{3} \otimes {\cal Z}^{\prime}_{3}$…

High Energy Physics - Phenomenology · Physics 2021-02-24 M. C. Rodriguez

In the relation between the linear (L) supersymmetry (SUSY) representation and the nonlinear (NL) SUSY representation we discuss the role of the Wess-Zumino gauge. We show in two dimensional spacetime that a spontaneously broken LSUSY…

High Energy Physics - Theory · Physics 2008-11-26 Kazunari Shima , Motomu Tsuda