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Related papers: Light Stop from b-tau Yukawa Unification

200 papers

We show that in the Minimal Supersymmetric Standard Model, the mass of the lightest neutralino is experimentally unconstrained if the GUT relation between the gaugino mass parameters M_1 and M_2 is dropped. We discuss what the impact of…

High Energy Physics - Phenomenology · Physics 2009-02-16 H. K. Dreiner , S. Heinemeyer , O. Kittel , U. Langenfeld , A. M. Weber , G. Weiglein

We examine the prospects for testing SO(10) Yukawa-unified supersymmetric models during the first year of LHC running at \sqrt{s}= 7 TeV, assuming integrated luminosity values of 0.1 to 1 fb^-1. We consider two cases: the Higgs splitting…

High Energy Physics - Phenomenology · Physics 2010-04-23 Howard Baer , Sabine Kraml , Andre Lessa , Sezen Sekmen

A constraint from $b\rightarrow s\gamma$ process to the minimal supersymmetric standard model is derived in the light stop region where the coupling between the lighter stop and the $Z^0$ boson vanishes due to the left-right mixing of the…

High Energy Physics - Phenomenology · Physics 2009-10-22 Yasuhiro Okada

We study the prospects for the measurement of the stau - lightest neutralino mass difference (dM) and the gluino mass (Mg) in the supersymmetric co-annihilation region at the LHC using tau leptons. Recent WMAP measurements of the amount of…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Arnowitt , A. Aurisano , B. Dutta , T. Kamon , N. Kolev , P. Simeon , D. Toback , P. Wagner

We consider the constrained minimal supersymmetric standard model which emerges from one theory with a small deviation from Yukawa unification which is adequate for $\mu>0$. We show that this model possesses a wide and natural range of…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. E. Gomez , C. Pallis

A review of supersymmetric dark matter in minimal supergravity unification with R-parity invariance and with radiative breaking of the electro-weak symmetry is given. The analysis shows the lightest neutralino is the LSP over most of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pran Nath , R. Arnowitt

The Minimal Supersymmetric Standard Model opens the possibility of electroweak baryogenesis provided that the light scalar top quark (stop) is lighter than the top quark. In addition, the lightest neutralino is an ideal candidate to explain…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Carena , A. Finch , A. Freitas , C. Milstene , H. Nowak , A. Sopczak

The construction of a Supersymmetric Grand Unified Model based on the Pati-Salam gauge group is briefly reviewed and the low energy consequences of the derived asymptotic Yukawa quasi-unification conditions are examined. In the framework of…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. Pallis , M. E. Gomez

We review the phenomenology of gravitino dark matter within supergravity framework. Gravitino can be dark matter if it is the lightest supersymmetric particle, which is stable if R-parity is conserved. There are several distinct scenarios…

High Energy Physics - Phenomenology · Physics 2016-11-15 Yudi Santoso

In supersymmetric (SUSY) models with Dirac neutrino masses, a weak-scale trilinear A-term that is not proportional to the small neutrino Yukawa couplings can induce a sizable mixing between left and right-handed sneutrinos. The lighter…

High Energy Physics - Phenomenology · Physics 2015-03-19 Geneviève Bélanger , Sabine Kraml , Andre Lessa

We study the TeV scale partial mirage unification scenario, where the gluino and wino masses are degenerate around a TeV scale, but the bino mass is not degenerate. This scenario has phenomenologically interesting aspects. First, because of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hiroyuki Abe , Yeong Gyun Kim , Tatsuo Kobayashi , Yasuhiro Shimizu

There are several indications that the Majorana masses of the right-handed neutrino components, $M_R,$ are at the intermediate scale: $M_R\sim (10^{10}-10^{12})$ GeV or even lighter. The renormalization effects due to large Yukawa couplings…

High Energy Physics - Phenomenology · Physics 2009-10-28 F. Vissani , A. Yu. Smirnov

We study the prospects of detecting the signal in the stau neutralino co-annihilation region at the LHC using tau leptons. The co-annihilation signal is characterized by the stau and neutralino mass difference (dM) to be 5-15 GeV to be…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Arnowitt , A. Aurisano , B. Dutta , T. Kamon , N. Kolev , P. Simeon , D. Toback , P. Wagner

We study low-energy consequences of supersymmetric $SO(10)$ models with Yukawa unification $h_t = h_N$ and $h_b = h_\tau$. We find that it is difficult to reproduce the observed $m_b/m_\tau$ ratio when the third-generation right-handed…

High Energy Physics - Phenomenology · Physics 2009-09-29 Andrea Brignole , Hitoshi Murayama , Riccardo Rattazzi

The minimal supersymmetric (SUSY) standard model (MSSM) augmented by right chiral sneutrinos may lead to one such sneutrino serving as the lightest supersymmetric particle and a non-thermal dark matter candidate, especially if neutrinos…

High Energy Physics - Phenomenology · Physics 2018-09-27 Shankha Banerjee , Geneviève Bélanger , Avirup Ghosh , Biswarup Mukhopadhyaya

The consequences of Gauge-Yukawa Unification (GYU) in supersymmetric unified models on low energy physics are analyzed. We find that the observed top-bottom mass hierarchy can be explained by supersymmetric GYU and different models can be…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jisuke Kubo , Myriam Mondragon , Mark Olechowski , George Zoupanos

We discuss the scenario where the gravitino is the lightest supersymmetric particle and the long-lived next-to-lightest sparticle (NSP) is the neutralino or the stau, the charged partner of the tau lepton. In this case staus form bound…

High Energy Physics - Phenomenology · Physics 2007-10-30 Vassilis C. Spanos

We study the feasibility of detecting the stau neutralino (stau_1-neutralino_1)coannihilation region at the LHC using tau leptons. The signal is characterized by multiple low energy tau leptons from neutralino_2-->tau stau_1-->tau tau…

High Energy Physics - Phenomenology · Physics 2008-11-26 Richard Arnowitt , Bhaskar Dutta , Teruki Kamon , Nikolay Kolev , David Toback

The requirement of Yukawa coupling unification highly constrains the SUSY parameter space. In several SUSY breaking scenarios it is hard to reconcile Yukawa coupling unification with experimental constraints from B(b->s gamma) and the muon…

High Energy Physics - Phenomenology · Physics 2009-11-10 Csaba Balazs , Radovan Dermisek

The SU(5) unification-scale relation h_b=h_tau between the b and tau Yukawa couplings severely constrains tan beta and m_t (even more so if h_t=h_b= h_tau holds) in supersymmetric models. We examine the implications of these constraints for…

High Energy Physics - Phenomenology · Physics 2009-10-28 Paul Langacker , Nir Polonsky