A Conformal Gauge Mediation and Dark Matter with Only One Parameter

Kazuya Yonekura; Tsutomu T. Yanagida

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A Conformal Gauge Mediation and Dark Matter with Only One Parameter

Tsutomu T. Yanagida, Kazuya Yonekura

High Energy Physics - Phenomenology · Submitted 11 Jun 2010

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We show that there is a low-scale conformal gauge mediation model which contains all necessary ingredients, i.e. not only a SUSY-breaking dynamics and a gauge mediation mechanism, but also a candidate for the dark matter.

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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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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,439 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.34 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.97 · compares with prior results 0.11 · mentions code or data availability 0.01.

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arXiv listing abstract v1. Results and the main claim are underlined; show every role.

If the supersymmetry (SUSY) is a solution to the hierarchy problem, it is puzzling that any SUSY particle has not been discovered yet. We show that there is a low-scale conformal gauge mediation model which contains all necessary ingredients, i.e. not only a SUSY-breaking dynamics and a gauge mediation mechanism, but also a candidate for the dark matter. The model has only one free parameter, that is, the mass for messengers. In this model, the dark matter is provided by a composite particle in the SUSY-breaking sector, and the observed value of the dark matter density uniquely fixes the mass of messengers at the order of 10^2 TeV. Then, the sfermion and gaugino masses are fixed to be of order 10^2~10^3 GEV without any arbitrariness, thus the SUSY particles are expected not to be discovered at the Tevatron or LEP, while having a discovery possibility at the LHC.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#	sentence	role	the authors' own work	states the main conclusion	strength
s0	If the supersymmetry (SUSY) is a solution to the hierarchy problem, it is puzzling that any SUSY particle has not been discovered yet.	background 0.98	0.04	0.02	asserted 0.82
s1	We show that there is a low-scale conformal gauge mediation model which contains all necessary ingredients, i.e. not only a SUSY-breaking dynamics and a gauge mediation mechanism, but also a candidate for the dark matter.	contribution 0.98	0.92	0.53	asserted 1.00
s2	The model has only one free parameter, that is, the mass for messengers.	contribution 0.70	0.76	0.14	asserted 1.00
s3	In this model, the dark matter is provided by a composite particle in the SUSY-breaking sector, and the observed value of the dark matter density uniquely fixes the mass of messengers at the order of 10^2 TeV.	result 0.99	0.86	0.48	asserted 1.00
s4	Then, the sfermion and gaugino masses are fixed to be of order 10^2~10^3 GEV without any arbitrariness, thus the SUSY particles are expected not to be discovered at the Tevatron or LEP, while having a discovery possibility at the LHC.	interpretation 0.77	0.79	0.39	hedged possibility 0.76

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.74.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper

Original abstract

If the supersymmetry (SUSY) is a solution to the hierarchy problem, it is puzzling that any SUSY particle has not been discovered yet. We show that there is a low-scale conformal gauge mediation model which contains all necessary ingredients, i.e. not only a SUSY-breaking dynamics and a gauge mediation mechanism, but also a candidate for the dark matter. The model has only one free parameter, that is, the mass for messengers. In this model, the dark matter is provided by a composite particle in the SUSY-breaking sector, and the observed value of the dark matter density uniquely fixes the mass of messengers at the order of 10^2 TeV. Then, the sfermion and gaugino masses are fixed to be of order 10^2~10^3 GEV without any arbitrariness, thus the SUSY particles are expected not to be discovered at the Tevatron or LEP, while having a discovery possibility at the LHC.

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How the literature uses it

11 arXiv papers cite this in 21 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 19 sentences without a confident label

Cites it as background 2 papers

Bearing these merits of GMSB models, in this paper, we give our special attention to a class of GMSB models dubbed “conformal gauge mediation (CGM)” [ref] (see also the follow-up works in [ref] ).

Charms of Strongly Interacting Conformal Gauge Mediation · Introduction · 0.83
See e.g. Refs. [ref] for a detailed discussion of such scenarios in different contexts.

Cosmic strings from pure Yang-Mills theory · Properties of cosmic strings · 0.98

What it cites · 49 sentences without a confident label

Uses the method or tool of 3 papers

Because of the strong dynamics, the calculation of mass spectrum of the MSSM particles is very difficult, so we use an effective operator analysis [ref] .

Conformal Gauge Mediation · Conformal gauge mediation · 0.98
[Whatever the value of $ℓ$ is, one may write down a planar diagram so as to avoid $1/N$ suppressions.] The model is very strongly coupled [ref] , then using the rules of naive dimensional analysis [ref] with factors of $N$'s included (and assuming $N_C, N_Q$ and $N_P$ are all of the same order, say $N$), we may have $|m_P| ∼Ł$, $N_C g_h^2/16π^2 ∼1$, and $łS^j̃_ i ∼(Ł+Ł^2 ^2) ^̣j̃_ i$.

Naive Dimensional Analysis and Supersymmetry · Conformal gauge mediation · 0.82
[Whatever the value of $ℓ$ is, one may write down a planar diagram so as to avoid $1/N$ suppressions.] The model is very strongly coupled [ref] , then using the rules of naive dimensional analysis [ref] with factors of $N$'s included (and assuming $N_C, N_Q$ and $N_P$ are all of the same order, say $N$), we may have $|m_P| ∼Ł$, $N_C g_h^2/16π^2 ∼1$, and $łS^j̃_ i ∼(Ł+Ł^2 ^2) ^̣j̃_ i$.

Semi-direct Gauge Mediation in Conformal Windows of Vector-like Gauge Theories · Conformal gauge mediation · 0.82

Uses data or values from 1 paper

The values of the anomalous dimensions are given by $_S ≃0.70,_Q ≃-0.35,_P ≃-0.59$ as shown in Ref. [ref] .

Semi-direct Gauge Mediation in Conformal Windows of Vector-like Gauge Theories · $μ$-$B_μ$ · 0.99

Compares with 1 paper

First, colored particles are most likely lighter in the present model compared with in the minimal gauge mediation [ref] .

Conformal Gauge Mediation · Mass spectrum and LHC signature · 0.93

Cites as support 4 papers

In this region, the model becomes non-calculable, but the SUSY breaking has been established [ref] .

Semi-direct Gauge Mediation in Conformal Windows of Vector-like Gauge Theories · Conformal gauge mediation · 0.98
In this region, the model becomes non-calculable, but the SUSY breaking has been established [ref] .

Conformal Supersymmetry Breaking in Vector-like Gauge Theories · Conformal gauge mediation · 0.98
The above arguments suggest that the next-to-lightest SUSY particle (NLSP) is perhaps the Bino or the gluino [ref] .

Strongly Interacting Gauge Mediation at the LHC · Mass spectrum and LHC signature · 0.96

Cites as background 12 papers

In this subsection, we review the strongly coupled conformal gauge mediation model [ref] which is based on the recently discovered dynamical SUSY-breaking mechanism [ref] .

Semi-direct Gauge Mediation in Conformal Windows of Vector-like Gauge Theories · Conformal gauge mediation · 0.89
In this subsection, we review the strongly coupled conformal gauge mediation model [ref] which is based on the recently discovered dynamical SUSY-breaking mechanism [ref] .

Conformal Supersymmetry Breaking in Vector-like Gauge Theories · Conformal gauge mediation · 0.89
Interestingly, however, there is a class of gauge mediation models, called as conformal gauge mediation [ref] , where the SUSY-breaking scale is strongly linked to the messenger masses.

Conformal Gauge Mediation · Introduction · 0.80

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