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I discuss the calculation of the heavy generation masses in the superstring derived standard-like models. The top quark Yukawa coupling is obtained from a cubic level mass term while the bottom quark and tau lepton mass terms are obtained…

High Energy Physics - Phenomenology · Physics 2011-01-27 Alon E. Faraggi

We consider the renormalisation group flow of gauge couplings within the so-called exceptional supersymmetric standard model (E$_6$SSM) based on the low energy matter content of 27 dimensional representations of the gauge group $E_6$,…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. F. King , S. Moretti , R. Nevzorov

We briefly review the issues of proton decay and fermion masses and mixings in minimal supersymmetric grand unified theories. We argue that minimal SU(5), although tightly constrained by proton decay data, is still not ruled out. However,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Borut Bajc , Alejandra Melfo , Goran Senjanovic

We make a complete analysis of the Yukawa coupling unification in SU(5) extensions of the MSSM in the framework of the radiative symmetry breaking scenario. Both logarithmic and finite threshold corrections of sparticles have been included…

High Energy Physics - Phenomenology · Physics 2009-10-30 A. Dedes , K. Tamvakis

Contrary to commonly held belief, we show that one can obtain a low value for $M_R$, the $SU(2)_R$ breaking scale, in grand unification theories based on $SO(10)$. This possibility emerges in the supersymmetric version of $SO(10)$ with a…

High Energy Physics - Phenomenology · Physics 2009-10-22 N. G Deshpande , E. Keith , T. G. Rizzo

Third family Yukawa unification, as suggested by minimal SO(10) unification, is revisited in light of recent experimental measurements and theoretical progress. We characterize unification in a semi-model-independent fashion, and conclude…

High Energy Physics - Phenomenology · Physics 2010-04-05 Kazuhiro Tobe , James D. Wells

We present an updated assessment of the viability of t-b-tau Yukawa coupling unification in supersymmetric models. For the superpotential Higgs mass parameter mu>0, we find unification to less than 1% is possible, but only for GUT scale…

High Energy Physics - Phenomenology · Physics 2014-11-17 D. Auto , H. Baer , C. Balazs , A. Belyaev , J. Ferrandis , X. Tata

Recently realization of TeV scale inverse seesaw mechanism in supersymmetric SO(10) framework has led to a number of experimentally verifiable predictions including low-mass W_R and Z' gauge bosons and nonunitarity effects. Using…

High Energy Physics - Phenomenology · Physics 2015-06-03 Ram Lal Awasthi , Mina K. Parida

We perform numerical fits of Grand Unified Models based on SO(10), using various combinations of 10-, 120- and 126-dimensional Higgs representations. Both the supersymmetric and non-supersymmetric versions are fitted, as well as both…

High Energy Physics - Phenomenology · Physics 2013-09-17 Alexander Dueck , Werner Rodejohann

We discuss some testable predictions of a non-supersymmetric $SO(10)$ model supplemented by a Peccei-Quinn symmetry. We utilize a symmetry breaking pattern of $SO(10)$ that yields unification of the Standard Model gauge couplings, with the…

High Energy Physics - Phenomenology · Physics 2022-12-09 George Lazarides , Rinku Maji , Rishav Roshan , Qaisar Shafi

We make a comprehensive analysis of an extended supersymmetric model(ESSM) obtained by adding a pair of vector-like families to the minimal supersymmetric standard model and having specific forms of 5 x 5 fermion mass matrices. The singlet…

High Energy Physics - Phenomenology · Physics 2009-10-31 Mar Bastero-Gil , Biswajoy Brahmachari

We consider the scenario in which the mass matrices of the charged fermions in the SO(10) Grand Unified Theory are generated exclusively by renormalizable Yukawa couplings to one $\mathbf{10} \oplus \mathbf{120}$ representation of scalars.…

High Energy Physics - Phenomenology · Physics 2011-01-27 L. Lavoura , H. Kuhbock , W. Grimus

Supersymmetric $SO(10)$ models with Yukawa coupling matrices involving only a $10_H$ and a $\overline{126}_H$ of Higgs fields can lead to a predictive and consistent scenario for fermion masses and mixings, including the neutrino sector.…

High Energy Physics - Phenomenology · Physics 2018-10-30 K. S. Babu , Borut Bajc , Shaikh Saad

We present phenomenological aspects of the simplest realistic SU(5) grand unified theory--the theory with the 5, 15, and 24 dimensional representations in the Higgs sector. We show that a successful gauge coupling unification sets…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ilja Dorsner

We compute the one-loop radiative corrections to the masses of the top quark, the stop squarks and the gluino in the Minimal Supersymmetric Standard Model. We include the loops controlled by the strong coupling constant and the top Yukawa…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. Donini

The top-Yukawa-coupling enhanced two-loop corrections to the charged Higgs-boson mass in the real MSSM are presented. The contributing two-loop self-energies are calculated in the Feynman- diagrammatic approach in the gaugeless limit with…

High Energy Physics - Phenomenology · Physics 2015-07-10 Wolfgang Hollik , Sebastian Paßehr

We apply the full one-loop corrections to the masses, gauge couplings, and Yukawa couplings in the minimal supersymmetric standard model. We focus on predictions for the strong coupling and the bottom-quark pole mass in the context of SU(5)…

High Energy Physics - Phenomenology · Physics 2007-05-23 Damien Pierce

We propose an $SU(3)_C\times SU(2)_L \times SU(2)_N \times U(1)_Y$ model arising from $E_6$ grand unified theory. We show that the tiny neutrino masses in this model can be generated at the three-loop involving the $SU(2)_N$ gauge bosons.…

High Energy Physics - Phenomenology · Physics 2019-06-13 Bhaskar Dutta , Sumit Ghosh , Ilia Gogoladze , Tianjun Li

We construct lists of supersymmetric models with extended gauge groups at intermediate steps, all of which are based on SO(10) unification. We consider three different kinds of setups: (i) The model has exactly one additional intermediate…

High Energy Physics - Phenomenology · Physics 2013-04-17 C. Arbelaez , R. M. Fonseca , M. Hirsch , J. C. Romao

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
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