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The supersymmetric sector of minimal supersymmetric standard model (MSSM) possesses a U(1) R-symmetry which contains Z_2 matter parity. Non-zero neutrino masses, consistent with a 'redefined' R-symmetry, are possible through the see-saw…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. Lazarides , Q. Shafi

Supersymmetry solves the gauge hierarchy problem of the Standard Model if the masses of supersymmetric partners of the SM particles are close to the weak scale. In this thesis, we argue that the supersymmetric Standard Model, while avoiding…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kaustubh Agashe

To explain the dark matter and the baryon asymmetry of the Universe, the parameters of the $\nu$MSM (an extension of the Minimal Standard Model by three singlet neutrinos with masses smaller than the electroweak scale) must be fine-tuned:…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mikhail Shaposhnikov

Many extensions of the Standard Model have to face the problem of new unsuppressed baryon-number violating interactions. In supersymmetry, the simplest way to solve this problem is to assume R-parity conservation. As a result, the lightest…

High Energy Physics - Phenomenology · Physics 2011-05-05 Kaustubh Agashe , Geraldine Servant

In order that discrete symmetries should not be violated by gravitational effects, it is necessary to gauge them. In this paper we discuss the gauging of $\Z_N$ from the breaking of a high energy $SU(N)$ gauge symmetry, and derive…

High Energy Physics - Phenomenology · Physics 2009-10-22 P. L. White

Baryon number ($B$) conservation underlies the apparent stability of ordinary matter by forbidding the decay of nucleons, while lepton number ($L$) conservation plays a central role in the structure of lepton interactions and the possible…

High Energy Physics - Phenomenology · Physics 2026-02-11 Volodymyr Takhistov

We recall the obstacles which seemed, long ago, to prevent one from viewing supersymmetry as a possible fundamental symmetry of Nature. Is spontaneous supersymmetry breaking possible ? Where is the spin-1/2 Goldstone fermion of…

High Energy Physics - Phenomenology · Physics 2016-11-23 Pierre Fayet

We study two phases of a heterotic standard model, obtained from a Calabi-Yau compactification of the E8xE8 heterotic string, in the context of the associated four-dimensional effective theories. In the first phase we have a standard model…

High Energy Physics - Theory · Physics 2015-07-22 Evgeny I. Buchbinder , Andrei Constantin , Andre Lukas

We consider the most general generation-independent U(1) gauge symmetry consistent with the presence of Yukawa couplings for all quarks and leptons in the SUSY version of the Standard Model. This U(1) has generically mixed anomalies with SM…

High Energy Physics - Phenomenology · Physics 2009-10-31 Luis Ibanez , Fernando Quevedo

The Standard Model (SM) of the microcosm provides an excellent description of the phenomena of the microcosm, with the triumph of the discovery of the Higgs boson. There are many reasons, however, to believe that the SM is incomplete and…

High Energy Physics - Phenomenology · Physics 2019-06-06 Maurizio Spurio

We study the breaking of supersymmetry and its transmission to the light states in the context of the minimal SU(5) grand unified theory, with no additional singlets. This simple theory can be taken as a prototype for a program of breaking…

High Energy Physics - Phenomenology · Physics 2008-11-26 Borut Bajc , Goran Senjanovic

We show that in a self-consistent preon model, where Standard Model quarks and leptons are three-body composites confined at a metacolor scale Lambda_cr ~ 10^14 GeV, both leptoquarks and the Standard Model gauge group SU(3)_c x SU(2)_L x…

High Energy Physics - Phenomenology · Physics 2026-05-01 Risto Raitio

We point out that a class of non-supersymmetric models based on the gauge group $SU(3)_C \times SU(2)_L\times SU(2)_R\times U(1)_{Y_L}\times U(1)_{Y_R}$ possesses an automatic, exact $Z_{2 }$ symmetry under which the fermions in the…

High Energy Physics - Phenomenology · Physics 2016-11-16 P. S. Bhupal Dev , Rabindra N. Mohapatra , Yongchao Zhang

It is noted that, but for one missing piece -- proton decay -- the evidence in support of grand unification is now strong. It includes: (i) the observed family-structure, (ii) the meeting of the gauge couplings, (iii) neutrino-oscillations,…

High Energy Physics - Phenomenology · Physics 2014-11-17 Jogesh C. Pati

We recall the obstacles which seemed, long ago, to prevent supersymmetry from possibly being a fundamental symmetry of Nature. Which bosons and fermions could be related? Is spontaneous supersymmetry breaking possible? Where is the spin-1/2…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pierre Fayet

We propose a E_6 inspired supersymmetric model with a non-Abelian discrete flavor symmetry (S_4 group); that is, SU(3)_c x SU(2)_W x U(1)_Y x U(1)_X x S_4 x Z_2. In our scenario, the additional abelian gauge symmetry; U(1)_X, not only…

High Energy Physics - Phenomenology · Physics 2014-11-20 Y. Daikoku , H. Okada

Axion models generically suffer from a severe quality problem when coupled to gravity. In this article we provide a very simple model with a high quality axion. The axion is a pseudo-Nambu-Goldstone boson of the baryon number symmetry,…

High Energy Physics - Phenomenology · Physics 2025-10-10 Prateek Agrawal , Anson Hook , Vazha Loladze , Mario Reig

A simple extension of the Standard Model (SM), based on the gauge group $SU(3)_C\otimes SU(3)_L\otimes U(1)_Y$ with $Y$ being the hypercharge, is considered. We show that, by imposing an approximate global $SU(2)_L\times SU(2)_R$ custodial…

High Energy Physics - Phenomenology · Physics 2016-03-30 Le Tho Hue , Le Duc Ninh

Models of supersymmetric grand unified theories based on SU(5)_GUT \times U(N)_H gauge group (N = 2,3) have a symmetry that guarantees light Higgs doublets and absence of dimension-five proton decay operators. We analysed the proton decay…

High Energy Physics - Phenomenology · Physics 2009-11-10 Masahiro Ibe , T. Watari

We propose a new interpretation of Peccei-Quinn symmetry within the Standard Model, identifying it with the axial $B + L$ symmetry i.e. $U(1)_{PQ} \equiv U(1)_{\gamma_5(B+L)}$. This new interpretation retains all the attractive features of…

High Energy Physics - Phenomenology · Physics 2019-02-04 Mario Reig , Rahul Srivastava