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Related papers: Dynamical SUSY Breaking with a Hybrid Messenger Se…

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We address intermediate scales within a class of string models. The intermediate scales occur due to the SM singlets S_i acquiring non-zero VEVs due to radiative breaking; the mass-square (m_i)^2 of S_i is driven negative at mu_{RAD} due to…

High Energy Physics - Phenomenology · Physics 2009-09-17 G. Cleaver , M. Cvetic , J. R. Espinosa , L. Everett , P. Langacker

Supersymmetry (SUSY) breaking without messenger fields is proposed. We assume that our world is on a wall and SUSY is broken only by the coexistence of another wall with some distance from our wall. The Nambu-Goldstone (NG) fermion is…

High Energy Physics - Theory · Physics 2007-05-23 Nobuhito Maru

We study dark gauge-mediated supersymmetry breaking (dark GMSB) in a theory with a new unbroken $U(1)_{D}$ local symmetry and massless dark photon. Messenger fields charged under both Standard Model and dark gauge symmetries produce new…

High Energy Physics - Phenomenology · Physics 2025-05-16 Brian Batell , Yechan Kim , Hye-Sung Lee , Jiheon Lee

We investigate a large class of supersymmetric SO(10) grand unified theories within the framework of gauge-mediated supersymmetry breaking. We start with the most general messenger sector and imbedd the standard model gauge group into…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Frank , H. Hamidian , K. Puolamaki

We present a model in which the same modulus field breaks both SUSY and a simple GUT gauge group down to the SM gauge group. The modulus is stabilized by the inverted hierarchy mechanism in a perturbative region so that the model is…

High Energy Physics - Phenomenology · Physics 2014-11-17 Kaustubh Agashe

We construct an extension of the recently proposed dynamical model for the breaking of SU(5)$_{\rm GUT}$ gauge symmetry, in which a pair of massless chiral supermultiplets for Higgs doublets are naturally obtained. We point out that a model…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Hisano , T. Yanagida

In the multiverse the scale of SUSY breaking, \tilde{m} = F_X/M_*, may scan and environmental constraints on the dark matter density may exclude a large range of \tilde{m} from the reheating temperature after inflation down to values that…

High Energy Physics - Phenomenology · Physics 2015-06-03 Lawrence J. Hall , Yasunori Nomura

Models like the Supersymmetric Standard Model (SSM) possess simple, but well-hidden, `Outfields'. These Outfields are composite operators that violate superspace invariance, but in a special way. A new mechanism for SUSY breaking arises…

High Energy Physics - Theory · Physics 2010-12-23 John A. Dixon

The gauge coupling unification is one of main motivations in the split-SUSY scenario, and the existence of the grand unified theories (GUTs) is assumed. We examine how to realize split-SUSY mass spectrum in the context of GUTs and find that…

High Energy Physics - Phenomenology · Physics 2016-09-06 Naoyuki Haba , Nobuchika Okada

Tree-level gauge mediation (TGM) is a scenario of SUSY breaking in which the tree-level exchange of heavy (possibly GUT) vector fields generates flavor-universal sfermion masses. In this work we extend this framework to the case of E_6 that…

High Energy Physics - Phenomenology · Physics 2015-05-30 Maurizio Monaco , Marco Nardecchia , Andrea Romanino , Robert Ziegler

We consider explicit models of dynamical supersymmetry breaking where dark matter is a 10 -- 100 TeV strongly-interacting composite state carrying no standard model quantum numbers. These constructions are simple variants of well-known…

High Energy Physics - Phenomenology · Physics 2014-11-20 JiJi Fan , Jesse Thaler , Lian-Tao Wang

Supersymmetric models with a strongly interacting superconformal hidden sector (HS) may drive soft SUSY breaking scalar masses, bilinear soft term B\mu and Higgs combinations m_{H_{u,d}}^2+\mu^2 to small values at some intermediate scale,…

High Energy Physics - Phenomenology · Physics 2024-01-30 Howard Baer , Vernon Barger , Dakotah Martinez

A simple mechanism for SUSY breaking is proposed due to the coexistence of BPS domain walls. It requires no messenger fields nor complicated SUSY breaking sector on any of the walls. We assumed that our world is on a BPS domain wall and…

High Energy Physics - Theory · Physics 2007-05-23 Nobuhito Maru , Norisuke Sakai , Yutaka Sakamura , Ryo Sugisaka

In direct gauge mediation, the gaugino masses are anomalously small, giving rise to a split SUSY spectrum. Here we investigate the superpartner spectrum in a minimal version of "direct gaugino mediation." We find that the sfermion masses…

High Energy Physics - Phenomenology · Physics 2015-03-19 Roberto Auzzi , Amit Giveon , Sven Bjarke Gudnason , Tomer Shacham

An earlier paper showed that it is possible to write down new SUSY Actions in which it is not possible to define a Supersymmetry Charge. SUSY is defined in these new Actions by the fact that they satisfy Master Equations. The new SUSY…

High Energy Physics - Theory · Physics 2024-07-25 John Dixon

We consider gauge messenger models in which X and Y gauge bosons and gauginos are messengers of supersymmetry breaking. In simple gauge messenger models, all the soft parameters except mu and Bmu are calculated in terms of a single scale…

High Energy Physics - Phenomenology · Physics 2009-09-29 Hyung Do Kim

We present a complete, viable model of gravity-mediated supersymmetry breaking that is safe from all flavor constraints. The central new idea is to employ a supersymmetry breaking sector without singlets, but with D-terms comparable to…

High Energy Physics - Phenomenology · Physics 2010-12-24 Graham D. Kribs , Takemichi Okui , Tuhin S. Roy

Within the MSSM framework and with purely anomaly mediated supersymmetry breaking the slepton masses turn out to be tachyonic. We resolve this problem by introducing an anomaly free U(1) gauge symmetry which provides positive $D$-term…

High Energy Physics - Phenomenology · Physics 2007-05-23 Qaisar Shafi , Zurab Tavartkiladze

A general framework is presented for supersymmetric theories that do not suffer from fine-tuning in electroweak symmetry breaking. Supersymmetry is dynamically broken at a scale \Lambda \approx (10 - 100) TeV, which is transmitted to the…

High Energy Physics - Phenomenology · Physics 2009-09-29 Yasunori Nomura , Brock Tweedie

Many extensions of the Standard Model include a new $U(1)$ gauge group that is broken spontaneously at a scale much above TeV. If a $U(1)$-breaking phase transition occurs at nucleation temperature of $O(100)$-$O(1000)$~TeV, it can generate…

High Energy Physics - Phenomenology · Physics 2020-04-22 Naoyuki Haba , Toshifumi Yamada