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Direct-Transmission Models of Dynamical Supersymmetry Breaking
High Energy Physics - Phenomenology · Submitted 5 May 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We obtain a natural model with the gravitino mass $m_{3/2}$ smaller than 1 keV as required from the standard cosmology.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We systematically construct gauge-mediated supersymmetry(SUSY)-breaking models with direct transmission of SUSY-breaking effects to the standard-model sector. We obtain a natural model with the gravitino mass $m_{3/2}$ smaller than 1 keV as required from the standard cosmology. If all Yukawa coupling constants are of order one,the SUSY-breaking scale $m_{SUSY}$ transmitted into the standard-model sector is given by $m_{SUSY} \simeq 0.1 \alpha_i/(4\pi) \Lambda$ where $\Lambda$ is the original dynamical SUSY-breaking scale. Imposing $m_{SUSY} \simeq (10^2-10^3)$ GeV, we get $\Lambda \simeq (10^5-10^6)$ GeV, which yields the gravitino mass $m_{3/2}\simeq (10^{-2}-1)$ keV.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We systematically construct gauge-mediated supersymmetry(SUSY)-breaking models with direct transmission of SUSY-breaking effects to the standard-model sector. | contribution 0.96 | 0.94 | 0.19 | asserted 1.00 |
| s1 | We obtain a natural model with the gravitino mass $m_{3/2}$ smaller than 1 keV as required from the standard cosmology. | result 0.95 | 0.93 | 0.21 | asserted 1.00 |
| s2 | If all Yukawa coupling constants are of order one,the SUSY-breaking scale $m_{SUSY}$ transmitted into the standard-model sector is given by $m_{SUSY} \simeq 0.1 \alpha_i/(4\pi) \Lambda$ where $\Lambda$ is the original dynamical SUSY-breaking scale. | result 1.00 | 0.81 | 0.29 | asserted 0.96 |
| s3 | Imposing $m_{SUSY} \simeq (10^2-10^3)$ GeV, we get $\Lambda \simeq (10^5-10^6)$ GeV, which yields the gravitino mass $m_{3/2}\simeq (10^{-2}-1)$ keV. | result 0.98 | 0.88 | 0.27 | asserted 1.00 |
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The paper
Original abstract
We systematically construct gauge-mediated supersymmetry(SUSY)-breaking models with direct transmission of SUSY-breaking effects to the standard-model sector. We obtain a natural model with the gravitino mass $m_{3/2}$ smaller than 1 keV as required from the standard cosmology. If all Yukawa coupling constants are of order one,the SUSY-breaking scale $m_{SUSY}$ transmitted into the standard-model sector is given by $m_{SUSY} \simeq 0.1 \alpha_i/(4\pi) \Lambda$ where $\Lambda$ is the original dynamical SUSY-breaking scale. Imposing $m_{SUSY} \simeq (10^2-10^3)$ GeV, we get $\Lambda \simeq (10^5-10^6)$ GeV, which yields the gravitino mass $m_{3/2}\simeq (10^{-2}-1)$ keV.
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References
How the literature uses it
33 arXiv papers cite this in 49 sentences
Papers citing it · 36 sentences without a confident label
Builds on it 1 paper
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In this section, we generalize the model discussed in Refs. [ref] .
Low Scale Direct Gauge Mediation with Perturbatively Stable Vacuum · Classification of direct mediation models · 0.99
Compares with it 1 paper
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For a small $F$, expanding the gaugino mass in terms of $F/m^2_i$, we find that the leading non-vanishing term is proportional to $F^3$ which agrees with [ref] .
Higgs boson from the meta-stable SUSY breaking sector · Direct gauge mediation · 0.96
Cites it as background 10 papers
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First, we review the model [ref] based on the IYIT model [ref] as a SUSY breaking sector.
LHC Reach of Low Scale Gauge Mediation with Perturbatively Stable Vacuum · Model A (based on the IYIT model) · 0.82
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This model is based on the recent development of metastable SUSY breaking in supersymmetric QCD (SQCD) started from the work of Intriligator, Seiberg and Shih (ISS) [ref] and is classified as so-called direct gauge mediation models [ref] where the flavor symmetries of a hidden SUSY breaking sector are weakly gauged and identified with the standard model gauge symmetries.
Inflation in Gauge Mediation and Gravitino Dark Matter · Introduction · 0.80
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We begin by considering a simple example of the messenger sector[Low energy description of direct GMSB models is often given by superpotentials of this type [ref] .]: [equation] Where $S$ is a supersymmetry breaking field and $ψ$, $ψ̅$ are messenger fields.
Cascade supersymmetry breaking and low-scale gauge mediation · R-symmetry and the messenger sector · 0.86
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