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We construct supersymmetric theories in which the correct scale for electroweak symmetry breaking is obtained without significant fine-tuning. We calculate the fine-tuning parameter for these theories to be at the 20% level, which is…

High Energy Physics - Phenomenology · Physics 2009-09-29 Z. Chacko , Yasunori Nomura , David Tucker-Smith

We consider the Z'/Z mass hierarchy in a supersymmetric model in which the U(1)' is broken in a secluded sector coupled to the ordinary sector only by gauge and possibly soft terms. A large mass hierarchy can be achieved while maintaining…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jens Erler , Paul Langacker , Tianjun Li

We reconsider the idea of identifying the Higgs field as the internal component of a gauge field in the flat space R^4XS^1/Z_2, by relaxing the constraint of having unbroken SO(4,1) Lorentz symmetry in the bulk. In this way, we show that…

High Energy Physics - Phenomenology · Physics 2009-11-11 Giuliano Panico , Marco Serone , Andrea Wulzer

Gauge coupling unification and the stability of the Higgs vacuum are among two of the cherished features of low-energy supersymmetric models. Putting aside questions of naturalness, supersymmetry might only be realised in nature at very…

High Energy Physics - Phenomenology · Physics 2018-09-19 Sebastian A. R. Ellis , Tony Gherghetta , Kunio Kaneta , Keith A. Olive

An ${\rm SU}(8)$ theory was previously found to be the minimal simple gauge group where all three-generational Standard Model (SM) fermions can be nontrivially embedded. It is maximally broken into a subgroup of ${\rm SU}(8)\to {\cal…

High Energy Physics - Phenomenology · Physics 2025-06-30 Ning Chen , Zhiyuan Chen , Zhanpeng Hou , Zhaolong Teng , Bin Wang

Within a supersymmetric unified framework we explore the resolution of the gauge hierarchy problem taking account of the non-renormalizable terms in the superpotential. For $[SU(3)]^3$ supplemented by a discrete R parity, we find the…

High Energy Physics - Phenomenology · Physics 2011-05-12 G. Dvali , Q. Shafi

We construct a 5D SUSY SU(6) GUT on an $S^{(1)}/Z_2\tm Z_2'$ orbifold. The first stage of gauge symmetry breaking occurs through compactification and a specific selection of boundary conditions. Additional symmetries play a crucial role for…

High Energy Physics - Phenomenology · Physics 2008-11-26 Filipe Paccetti Correia , Michael G. Schmidt , Zurab Tavartkiladze

We study a class of nonsupersymmetric SO(10) grand unified scenarios where the first stage of the symmetry breaking is driven by the vacuum expectation values of the 45-dimensional adjoint representation. Three decade old results claim that…

High Energy Physics - Phenomenology · Physics 2014-11-20 Stefano Bertolini , Luca Di Luzio , Michal Malinsky

If supersymmetry (SUSY) is realized at the electroweak scale, its underlying structure and breaking mechanism may be explored with great precision by a future linear $e^+ e^-$ collider (LC) with a clean environment, tunable collision…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Y. Choi

A SU(3) \times SU(2) \times U(1) supersymmetric theory is constructed with a TeV sized extra dimension compactified on the orbifold S^1/(Z_2 \times Z_2'). The compactification breaks supersymmetry leaving a set of zero modes which…

High Energy Physics - Phenomenology · Physics 2009-09-29 Riccardo Barbieri , Lawrence J. Hall , Yasunori Nomura

We investigate quartification models in five dimensions, with the fifth dimension forming an $S^1/Z_2\times Z_2'$ orbifold. The orbifold construction is combined with a boundary Higgs sector to break the quartified gauge group directly to a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alison Demaria , Kristian L. McDonald

The supersymmetric flipped $SU(6)\times U(1)$ gauge symmetry can arise through compactification of the ten dimensional $E_8\times E_8$ superstring theory. We show how realistic phenomenology can emerge from this theory by supplementing it…

High Energy Physics - Phenomenology · Physics 2011-05-12 Qaisar Shafi , Zurab Tavartkiladze

Dynamical breaking of supersymmetry was long thought to be an exceptional phenomenon, but recent developments have altered this view. A question of great interest in the current framework is the value of the underlying scale of…

High Energy Physics - Phenomenology · Physics 2009-01-09 Michael Dine , John Mason

The current experimental lower bound on the Higgs mass significantly restricts the allowed parameter space in most realistic supersymmetric models, with the consequence that these models exhibit significant fine-tuning. We propose a…

High Energy Physics - Phenomenology · Physics 2014-11-17 Andreas Birkedal , Z. Chacko , Mary K. Gaillard

We review the gauge symmetry breaking mechanism due to orbifold projections in orbifold model building. We explicitly show the existence of a scale of breaking if such a symmetry breaking is due to freely-acting orbifold operators only,…

High Energy Physics - Theory · Physics 2008-11-26 Michele Trapletti

Supersymmetry broken geometrically in extra dimensions naturally leads to a nearly degenerate spectrum for superparticles, ameliorating the bounds from the current searches at the LHC. We present a minimal such model with a single extra…

High Energy Physics - Phenomenology · Physics 2015-03-20 Hitoshi Murayama , Yasunori Nomura , Satoshi Shirai , Kohsaku Tobioka

We consider supersymmetric theories where the standard-model quark and lepton fields are localized on a "3-brane" in extra dimensions, while the gauge and Higgs fields propagate in the bulk. If supersymmetry is broken on another 3-brane,…

High Energy Physics - Phenomenology · Physics 2009-10-31 Z. Chacko , Markus A. Luty , Ann E. Nelson , Eduardo Ponton

We study the interplay between the spontaneous breaking of a global symmetry of the Higgs sector and gauge-mediated supersymmetry breaking, in the framework of a supersymmetric model with global SU(3) symmetry. In addition to solving the…

High Energy Physics - Phenomenology · Physics 2015-05-19 Anna Kaminska , Stephane Lavignac

We describe a model for the scalar sector where all interactions occur either at an ultra-high scale L_U ~ 10^{16}-10^{19} GeV or at an intermediate scale L_I ~ 10^{9}-10^{11} GeV. The interaction of physics on these two scales results in…

High Energy Physics - Phenomenology · Physics 2009-01-07 David Atwood , Shaouly Bar-Shalom , Amarjit Soni

A $Z_2$ symmetry that extends the weak interaction, $SU(2)_L \rightarrow SU(2)_L \times SU(2)'$, and the Higgs sector, $H(2) \rightarrow H(2,1) + H'(1,2)$, yields a Standard Model quartic coupling that vanishes at scale $v' = <H'>~\gg~<H>$.…

High Energy Physics - Phenomenology · Physics 2018-11-14 Lawrence J. Hall , Keisuke Harigaya