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We construct supersymmetric (SUSY) grand unification (GUT) models in the six dimensional space-time where the GUT symmetry is broken down to the standard-model gauge group by a simple orbifolding T^2/Z_4 or T^2/Z_6 and a pair of massless…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. Watari , T. Yanagida

We investigate the possibility to generate neutrino masses in the context of Split supersymmetric scenarios where all sfermions are very heavy. All relevant contributions coming from the R-parity violating terms to the neutrino mass matrix…

High Energy Physics - Phenomenology · Physics 2009-01-15 Marco Aurelio Diaz , Pavel Fileviez Perez , Clemencia Mora

We consider an MSSM extension with anomaly mediation as the source of supersymmetry-breaking, and a U(1) symmetry which solves the tachyonic slepton problem, and introduces both the see-saw mechanism for neutrino masses, and the Higgs…

High Energy Physics - Phenomenology · Physics 2015-06-04 Mark Hindmarsh , D. R. Timothy Jones

It is often argued that the minimal supersymmetric standard model has O(100) free parameters and the generic parameter region is already excluded by the null observation of the flavor and CP violating processes as well as the constraints…

High Energy Physics - Phenomenology · Physics 2016-12-21 Ryuichiro Kitano , Ryuji Motono , Minoru Nagai

We consider the possibility to observationally differentiate the Standard Model (SM) Higgs driven inflation with non-minimal couplingto gravity from other variants of SM Higgs inflation based on the scalar field theories with non-canonical…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-28 L. A. Popa

In the Minimal Supersymmetric Standard Model (MSSM), a Higgs boson mass of 125 GeV can be obtained with moderately heavy scalar top superpartners provided they are highly mixed. The source of this mixing, a soft trilinear stop-stop-Higgs…

High Energy Physics - Phenomenology · Physics 2014-03-25 Nikita Blinov , David E. Morrissey

We propose the Supersymmetric Standard Models (SSMs) with a pseudo-Dirac gluino from hybrid $F-$ and $D-$term supersymmetry (SUSY) breakings. Similar to the SSMs before the LHC, all the supersymmetric particles in the Minimal SSM (MSSM)…

High Energy Physics - Phenomenology · Physics 2015-07-16 Ran Ding , Tianjun Li , Florian Staub , Chi Tian , Bin Zhu

We study SU(N) supersymmetric Yang-Mills theory with massless adjoint matter defined on $M^3\otimes S^1$. The SU(N) gauge symmetry is broken maximally to $U(1)^{N-1}$, independent of the number of flavor and the boundary conditions of the…

High Energy Physics - Theory · Physics 2009-11-07 K. Takenaga

The Higgs boson mass problem is considered in the next-to-minimal supersymmetric standard model for the case of the spontaneous CP violation. The renormalization group equations for the gauge, Yukawa and scalar coupling constants, the…

High Energy Physics - Phenomenology · Physics 2009-10-28 H. M. Asatrian , G. K. Yeghiyan

A non-universal $U(1)_{X}$ extension to the Standard Model composed of two scalar doublets and two scalar singlets together with three additional quark singlets and two lepton singlets and three generations of right-handed and Majorana…

High Energy Physics - Phenomenology · Physics 2020-10-07 J. S. Alvarado , M. A. Bulla , D. G. Martinez , R. Martinez

We propose a supersymmetric extension of the standard model which is a realistic alternative to the MSSM, and which has several advantages. No ``mu'' supersymmetric Higgs/Higgsino mass parameter is needed for sufficiently heavy charginos.…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ann E. Nelson , Nuria Rius , Veronica Sanz , Mithat Unsal

The discovery of the Higgs boson is both a milestone achievement for the Standard Model and an exciting probe of new physics beyond the SM. One of the most important properties of the Higgs is its mass, a number that has proven to be highly…

High Energy Physics - Phenomenology · Physics 2017-02-23 Patrick Draper , Heidi Rzehak

We argue that with the discovery of neutrino mass effects at Super-Kamiokande there is a clear logical chain leading from the Standard Model through the MSSM and the recently developed Minimal Left Right Supersymmetric models with a…

High Energy Physics - Phenomenology · Physics 2011-02-09 Charanjit Singh Aulakh

Assuming grand unified theory (GUT) and supersymmetry, we propose a simple model which can consistently accommodate the masses and mixings for quarks and leptons. The grand unified group is SO(10), and $\bf 10$, $\bf 120$, and $\bar {\bf…

High Energy Physics - Phenomenology · Physics 2009-11-10 Noriyuki Oshimo

The electroweak (EW) symmetry breaking in the simplest supersymmetric (SUSY) extensions of the standard model (SM), i.e. minimal and next-to-minimal supersymmetric standard models (MSSM and NMSSM), is considered. The spectrum of the Higgs…

High Energy Physics - Phenomenology · Physics 2011-05-13 R. Nevzorov

In supersymmetric models where the superpotential mu term is generated with mu<< m_{soft} (e.g. from radiative Peccei-Quinn symmetry breaking or compactified string models with sequestration and stabilized moduli), and where the string…

High Energy Physics - Phenomenology · Physics 2016-06-22 Howard Baer , Vernon Barger , Michael Savoy , Hasan Serce

A new economical model for neutrino masses is proposed in the context of brane bulk scenarios for particle physics, where global B-L symmetry of the standard model is broken spontaneously by a gauge singlet Higgs field in the bulk. This…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. N. Mohapatra , A. Perez-Lorenzana , C. A. de S. Pires

On the basis of the universal seesaw mass matrix model, which is a promising model of the unified description of the quark and lepton mass matrices, the behaviors of the gauge coupling constants and intermediate energy scales in the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yoshio Koide

A noncommutative version of the usual electro-weak theory is constructed. We discuss how to overcome the two major problems: 1) although we can have noncommutative U(n) (which we denote by $U_{\star}(n)$) gauge theory we cannot have…

High Energy Physics - Theory · Physics 2010-05-28 M. Chaichian , P. Presnajder , M. M. Sheikh-Jabbari , A. Tureanu

The structure of the quark and lepton masses and mixing angles provides one of the few windows we have on the underlying physics generating the \sm. In an attempt to identify the underlying symmetry group we look for the simplest gauge…

High Energy Physics - Phenomenology · Physics 2011-07-19 Luis E. Ibanez , G. G. Ross
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