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Related papers: MSSM and Large $tan\beta$ from SUSY Trinification

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In the context of the standard SUSY GUT scenario, we present a detailed analysis of the softly broken finite supersymmetric grand unified theory. The model, albeit non-minimal, remains very rigid due to the requirement of finiteness. It is…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. I. Kazakov , M. Yu. Kalmykov , I. N. Kondrashuk , A. V. Gladyshev

We present the simplest, string-derivable, supergravity model and discuss its experimental consequences. This model is a new string-inspired flipped $SU(5)$ which unifies at the string scale $M_U=10^{18}\GeV$ due to the introduction of an…

High Energy Physics - Phenomenology · Physics 2009-08-25 J. Lopez , D. Nanopoulos , A. Zichichi

We introduce the supersymmetric version of YM-like theories with infinitely many spin fields in 4 dimension. The construction is carried out via the superfield method. The surprising feature of these models is that they describe in…

High Energy Physics - Theory · Physics 2020-12-18 Loriano Bonora , Stefano Giaccari

We explore in a model independent way the possibility of achieving the non supersymmetric gauge coupling unification within left-right symmetric models, with the minimal particle content at the left-right mass scale which could be as low as…

High Energy Physics - Phenomenology · Physics 2009-10-31 Abdel Pérez--Lorenzana , William A. Ponce , Arnulfo Zepeda

The purpose of this paper is threefold: a) Check if the rather poor Standard Model (SM) fit to all electroweak data can be improved in its minimal supersymmetric extension (MSSM); b) Check what constraints present electroweak data has on…

High Energy Physics - Phenomenology · Physics 2009-11-10 Wim de Boer , Christian Sander

A new supersymmetric grand unified model based on the gauge group $SU(5)\times SU(5)$ is discussed. The model has the feature that the conventional seesaw mechanism for neutrino masses is implemented using the $(15, 1)+(1,\bar{15)}$…

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

The Coulomb branch of $N=2$ supersymmetric gauge theories in four dimensions is described in general by an integrable Hamiltonian system in the holomorphic sense. A natural construction of such systems comes from two-dimensional gauge…

High Energy Physics - Theory · Physics 2010-04-07 Ron Donagi , Edward Witten

We introduce an explicit supersymmetric unification model where grand unified gauge symmetry breaking and supersymmetry (SUSY) breaking are caused by the same field. Besides, the SM-charged particles are also predicted by the symmetry…

High Energy Physics - Phenomenology · Physics 2015-04-28 Yuji Omura

We construct a supersymmetric standard model in the context of the $Z_{12-I}$ orbifold compactification of the heterotic string theory. The gauge group is $SU(3)_c\times SU(2)_L\times U(1)_Y\times U(1)^4\times[SO(10)\times U(1)^3]'$. We…

High Energy Physics - Phenomenology · Physics 2010-10-27 Jihn E. Kim , Ji-Hun Kim , Bumseok Kyae

What does third family ($t$-$b$-$\tau$) Yukawa unification, a typical prediction from embedding the Standard Model (SM) fermions in 16-plets of a $\mathrm{SO}(10)$ GUT, imply for the scale of the supersymmetric (SUSY) partners? Which…

High Energy Physics - Phenomenology · Physics 2025-09-18 Stefan Antusch , Shaikh Saad , Vasja Susič

The MSSM distinguishes itself from other GUT's by a successful prediction of many unrelated phenomena with a minimum number of parameters. Among them: a) Unification of the couplings constants; b)Unification of the masses; c) Proton decay;…

High Energy Physics - Phenomenology · Physics 2012-01-11 W. de Boer , R. Ehret , D. I. Kazakov

Supersymmetry is one of the best motivated possibilities for new physics at the TeV scale. However, both concrete string constructions and phenomenological considerations suggest the possibility that the physics at the TeV scale could be…

High Energy Physics - Phenomenology · Physics 2009-01-06 Vernon Barger , Paul Langacker , Gabe Shaughnessy

If N=2 supersymmetry breaks to N=1 supersymmetry at an intermediate scale $m_2$ and then, later on, N=1 supersymmetry breaks and produces standard model at a scale $m_{susy}$ such that $m_2 > m_{susy}$, renormalization group evolution of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Biswajoy Brahmachari

In the generalized minimal supergravity (GmSUGRA) scenario, we systematically study the supersymmetry breaking scalar masses, Standard Model fermion Yukawa coupling terms, and trilinear soft terms in SU(5) models with the Higgs fields in…

High Energy Physics - Phenomenology · Physics 2014-11-21 Csaba Balazs , Tianjun Li , Dimitri V. Nanopoulos , Fei Wang

Recent advances in the calculation of the $b\to s\gamma$ decay branching ratio are presented in the context of supersymmetric theories. Theoretical accuracy increased by inclusion of the next-to-leading order QCD corrections makes it…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michal Brhlik

The minimal supersymmetric SO(10) model, in which not only the gauge but also the third generation fermion Yukawa couplings are unified, provides a simple and highly predictive theoretical scenario for the understanding of the origin of the…

High Energy Physics - Phenomenology · Physics 2009-09-25 M. Carena , C. E. M. Wagner

After a brief review of the motivations for grand unification, I discuss the main challenges facing realistic SUSY GUT model building. Achieving doublet-triplet splitting without fine--tuning is chief among them. Symmetry breaking should…

High Energy Physics - Phenomenology · Physics 2011-11-10 K. S. Babu

It is shown how an $SU(3)^{N}$ nonsupersymmetric quiver gauge theory can accommodate the standard model with three chiral families and unify all of $SU(3)_C$, $SU(2)_L$ and $U(1)_Y$ couplings with high accuracy at one unique scale estimated…

High Energy Physics - Phenomenology · Physics 2009-11-07 Paul H. Frampton

We construct a supersymmetric standard model in the context of the Z_{12-I} orbifold compactification of the E_8 x E_8' heterotic string theory. The gauge group is SU(3)_c x SU(2)_L x U(1)_Y x U(1)^4 x [SO(10) x U(1)^3]' with sin^2\theta_W…

High Energy Physics - Theory · Physics 2007-11-01 Jihn E. Kim , Ji-Hun Kim , Bumseok Kyae

We describe a simple class of supersymmetric gauge theories that can act as supersymmetry-breaking sectors for gauge-mediated supersymmetry breaking. The models have a local supersymmetry-breaking minimum along a direction in field space…

High Energy Physics - Phenomenology · Physics 2009-10-30 Markus A. Luty