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Related papers: Gauge Mediation with D-term SUSY Breaking

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Anomaly-mediated supersymmetry breaking in the context of 4D conformally sequestered models is combined with Poppitz-Trivedi D-type gauge-mediation. The implementation of the two mediation mechanisms naturally leads to visible soft masses…

High Energy Physics - Theory · Physics 2009-09-15 Raman Sundrum

We give a general definition of gauge mediated supersymmetry breaking which encompasses all the known gauge mediation models. In particular, it includes both models with messengers as well as direct mediation models. A formalism for…

High Energy Physics - Phenomenology · Physics 2009-09-15 Patrick Meade , Nathan Seiberg , David Shih

We propose a new class of gauge mediated supersymmetry breaking models where the standard model gauge group is embedded into the gauge group $SU(2)_L\times U(1)_{I_{3R}}\times U(1)_{B-L}$ [or $SU(2)_L\times SU(2)_R\times U(1)_{B-L}$] at the…

High Energy Physics - Phenomenology · Physics 2009-10-30 R. N. Mohapatra , S. Nandi

We propose a simple class of nonrenormalizable models of gauge mediated dynamical supersymmetry breaking. The models do not have gauge singlet fields. The Standard Model gauge group is embedded in the global symmetry of the SUSY breaking…

High Energy Physics - Phenomenology · Physics 2009-10-30 Yuri Shirman

In the supersymmetric models with low scale supersymmetry (SUSY) breaking where the gravitino mass is around keV, we show that the 3.5 keV $X-$ray lines can be explained naturally through several different mechanisms: (I) A keV scale dark…

High Energy Physics - Phenomenology · Physics 2015-06-19 Zhaofeng Kang , P. Ko , Tianjun Li , Yandong Liu

A consistent theory of supersymmetry breaking must have a hidden sector, an observable sector, and must be embedded in a locally supersymmetric theory which arises from string theory. For phenomenological reasons it must also transmit…

High Energy Physics - Theory · Physics 2009-03-27 S. P. de Alwis

We consider theories with one or more compact dimensions with size r > 1/M, where M is the fundamental Planck scale, with the visible and hidden sectors localized on spatially separated "3-branes." We show that a bulk U(1) gauge field…

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

We study phenomenological features in an extended gauge mediation SUSY breaking model which has non-universal gaugino masses and CP phases. We show that large CP phases in soft SUSY breaking parameters can be consistent with the constraints…

High Energy Physics - Phenomenology · Physics 2008-11-26 Daijiro Suematsu

We present a model of supersymmetry breaking mediated through a small extra dimension. Standard model matter multiplets and a supersymmetry-breaking (or ``hidden'') sector are confined to opposite four-dimensional boundaries while gauge…

High Energy Physics - Phenomenology · Physics 2009-10-31 David Elazzar Kaplan , Graham D. Kribs

Strongly coupled semi-direct gauge mediation models of supersymmetry breaking through massive mediators with standard model charges are investigated by means of composite degrees of freedom. Sizable mediation is realized to generate the…

High Energy Physics - Phenomenology · Physics 2010-05-12 M. Ibe , K. -I. Izawa , Y. Nakai

We examine the infra-red structure of soft supersymmetry breaking masses of the squarks and sleptons in supersymmetric (SUSY) strong unification schemes where $\alpha_{GUT}\sim 0.2-1$. We show that combinations of soft masses approach fixed…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. F. King , G. G. Ross

We argue that supersymmetry breaking by gaugino condensation in the strongly coupled heterotic string can be described by an analogue of Scherk-Schwarz compactification on the eleventh dimension in M-theory. The M-theory scale is identified…

High Energy Physics - Theory · Physics 2009-10-30 I. Antoniadis , M. Quiros

We propose a new framework for the next-to-minimal supersymmetric standard model (NMSSM) in gauge mediation, where in general the correct electroweak symmetry breaking (EWSB) is difficult to be explained. The difficulty is caused by the…

High Energy Physics - Phenomenology · Physics 2016-02-17 Masaki Asano , Yuichiro Nakai , Norimi Yokozaki

We present a new, simple supersymmetry breaking model with direct gauge mediation. Supersymmetry breaking sector is based on the model with an Affine quantum moduli space. The model has no gauge messengers and no light scalars charged under…

High Energy Physics - Phenomenology · Physics 2016-09-06 Nobuhito Maru

Most phenomenologically acceptable supersymmetric models imply breaking of supersymmetry in a separate sector of fields introduced just for this purpose. Supersymmetry breaking is transferred to the Standard Model due to a certain…

High Energy Physics - Phenomenology · Physics 2010-12-17 S. L. Dubovsky , D. S. Gorbunov , S. V. Troitsky

We present a class of models in the framework of gauge mediation supersymmetry breaking where the messenger fields transform in the adjoint representation of the Standard Model gauge symmetry. To avoid unacceptably light right-handed…

High Energy Physics - Phenomenology · Physics 2016-11-02 Ilia Gogoladze , Azar Mustafayev , Qaisar Shafi , Cem Salih Un

We generalize the General Gauge Mediation formalism to allow for the possibility of gauge messengers. Gauge messengers occur when charged matter fields of the susy-breaking sector have non-zero F-terms, which leads to tree-level,…

High Energy Physics - Phenomenology · Physics 2014-11-20 Kenneth Intriligator , Matthew Sudano

In theories in which SUSY is broken on a brane separated from the MSSM matter fields, supersymmetry breaking is naturally mediated in a variety of ways. Absent other light fields in the theory, gravity will mediate supersymmetry breaking…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ann E. Nelson , Neal Weiner

We present a SUSY breaking scenario based on Abelian gaugino kinetic term mixings between hidden and observable sectors. If an extra U(1) gaugino in the observable sector obtains a large mass through this mixing effect based on SUSY…

High Energy Physics - Phenomenology · Physics 2009-11-11 Daijiro Suematsu

The most general Lagrangian for a model with two U(1) gauge symmetries contains a renormalizable operator which mixes their gauge kinetic terms. Such kinetic mixing can be generated at arbitrarily high scales but will not be suppressed by…

High Energy Physics - Phenomenology · Physics 2009-07-09 Keith R. Dienes , Christopher Kolda , John March-Russell
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