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Dynamical Supersymmetry Breaking with T_N Theory
High Energy Physics - Theory · Submitted 31 Jul 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We demonstrate that the supersymmetry is dynamically broken in the four-dimensional SU(N) gauge theory coupled to a strongly-coupled superconformal theory T_N.
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The abstract, sentence by sentence
We demonstrate that the supersymmetry is dynamically broken in the four-dimensional SU(N) gauge theory coupled to a strongly-coupled superconformal theory T_N. This is a direct generalization of the model of supersymmetry breaking on deformed moduli space in supersymmetric QCD with an SU(2) gauge group.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We demonstrate that the supersymmetry is dynamically broken in the four-dimensional SU(N) gauge theory coupled to a strongly-coupled superconformal theory T_N. | result 0.91 | 0.93 | 0.94 | asserted 1.00 |
| s1 | This is a direct generalization of the model of supersymmetry breaking on deformed moduli space in supersymmetric QCD with an SU(2) gauge group. | interpretation 0.41 | 0.33 | 0.06 | asserted 1.00 |
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The paper
Original abstract
We demonstrate that the supersymmetry is dynamically broken in the four-dimensional SU(N) gauge theory coupled to a strongly-coupled superconformal theory T_N. This is a direct generalization of the model of supersymmetry breaking on deformed moduli space in supersymmetric QCD with an SU(2) gauge group.
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References
How the literature uses it
4 arXiv papers cite this in 5 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 2 papers
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The field theory dynamics of $=1$ class $$ theories or similar theories are discussed in [ref] .
Supersymmetric gauge theory, (2,0) theory and twisted 5d Super-Yang-Mills · Introduction and summary · 0.97
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Recently, there has been a lot of work on $=1$ dualities coming from wrapped $M5$-branes [ref] .
New N=1 dualities from orientifold transitions - Part I: Field Theory · Introduction · 0.80
What it cites · 5 sentences without a confident label
Builds on 2 papers
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When $N=2$, this effective superpotential is exactly the one considered in [ref] and our supersymmetry breaking mechanism is a direct generalization of the one in [ref] to $(N)$.
Dynamical Supersymmetry Breaking in Vector-like Gauge Theories · The model of supersymmetry breaking · 0.99
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When $N=2$, this effective superpotential is exactly the one considered in [ref] and our supersymmetry breaking mechanism is a direct generalization of the one in [ref] to $(N)$.
Dynamical Supersymmetry Breaking on Quantum Moduli Spaces · The model of supersymmetry breaking · 0.99
Uses the method or tool of 1 paper
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For $N ≥3$, we use an $=2$ duality of the $T_N$ theory [ref] .
N=2 dualities · More on Eq. [ref] · 0.93
Compares with 3 papers
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When $N=2$, this superpotential is exactly the one used in [ref] .
Dynamical Supersymmetry Breaking in Vector-like Gauge Theories · The model of supersymmetry breaking · 0.92
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When $N=2$, this superpotential is exactly the one used in [ref] .
Dynamical Supersymmetry Breaking on Quantum Moduli Spaces · The model of supersymmetry breaking · 0.92
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In the case of $N=2$ where $(μ_A)_i_A^j_A=Q_i_A i_B i_C Q^j_A i_B i_C$ and $(μ_B)_i_B^j_B=Q_i_A i_B i_C Q^i_A j_B i_C$, one can check that [ref] is just a rewriting of the more familiar deformed moduli constraint $M -B B̃=Λ^4$ of $N_f=N=2$ SUSY QCD [ref] .
Exact Results on the Space of Vacua of Four Dimensional SUSY Gauge Theories · The model of supersymmetry breaking · 0.91
Cites as support 1 paper
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As shown in [ref] , the operators of the $T_N$ theory neutral under $(N)_C$ are polynomials of $μ_A$ and $μ_B$.
N=1 dynamics with T_N theory · The model of supersymmetry breaking · 0.96
Cites as background 1 paper
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One of them is the $T_N$ theory [ref] which was discovered in the study of dualities of $=2$ supersymmetric theories.
N=2 dualities · Introduction · 0.99
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