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The large Nc limit of N=2 super Yang-Mills, fractional instantons and infrared divergences
High Energy Physics - Theory · Submitted 20 Jun 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our most interesting finding is that the 1/N expansion breaks down at singularities on the moduli space due to severe infrared divergencies, a fact that has remarkable consequences.
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We investigate the large Nc limit of pure N=2 supersymmetric gauge theory with gauge group SU(Nc) by using the exact low energy effective action. Typical one-complex dimensional sections of the moduli space parametrized by a global complex mass scale v display three qualitatively different regions depending on the ratio between |v| and the dynamically generated scale Lambda. At large |v|/Lambda, instantons are exponentially suppressed as N goes to infinity. When |v| is of order Lambda, singularities due to massless dyons occur. They are densely distributed in rings of calculable thicknesses in the v-plane. At small |v|/Lambda, instantons disintegrate into fractional instantons of charge 1/(2N). These fractional instantons give non-trivial contributions to all orders of 1/N, unlike a planar diagrams expansion which generates a series in 1/N^2, implying the presence of open strings. We have explicitly calculated the fractional instantons series in two representative examples, including the 1/N and 1/N^2 corrections. Our most interesting finding is that the 1/N expansion breaks down at singularities on the moduli space due to severe infrared divergencies, a fact that has remarkable consequences.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the large Nc limit of pure N=2 supersymmetric gauge theory with gauge group SU(Nc) by using the exact low energy effective action. | contribution 0.94 | 0.94 | 0.03 | asserted 0.97 |
| s1 | Typical one-complex dimensional sections of the moduli space parametrized by a global complex mass scale v display three qualitatively different regions depending on the ratio between |v| and the dynamically generated scale Lambda. | result 0.77 | 0.66 | 0.03 | asserted 1.00 |
| s2 | At large |v|/Lambda, instantons are exponentially suppressed as N goes to infinity. | result 1.00 | 0.73 | 0.04 | asserted 1.00 |
| s3 | When |v| is of order Lambda, singularities due to massless dyons occur. | result 1.00 | 0.61 | 0.03 | asserted 1.00 |
| s4 | They are densely distributed in rings of calculable thicknesses in the v-plane. | result 1.00 | 0.69 | 0.03 | asserted 1.00 |
| s5 | At small |v|/Lambda, instantons disintegrate into fractional instantons of charge 1/(2N). | result 1.00 | 0.67 | 0.05 | asserted 1.00 |
| s6 | These fractional instantons give non-trivial contributions to all orders of 1/N, unlike a planar diagrams expansion which generates a series in 1/N^2, implying the presence of open strings. | interpretation 0.84 | 0.71 | 0.11 | asserted 0.94 |
| s7 | We have explicitly calculated the fractional instantons series in two representative examples, including the 1/N and 1/N^2 corrections. | contribution 0.72 | 0.96 | 0.05 | asserted 1.00 |
| s8 | Our most interesting finding is that the 1/N expansion breaks down at singularities on the moduli space due to severe infrared divergencies, a fact that has remarkable consequences. | result 0.96 | 0.95 | 0.89 | asserted 1.00 |
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Original abstract
We investigate the large Nc limit of pure N=2 supersymmetric gauge theory with gauge group SU(Nc) by using the exact low energy effective action. Typical one-complex dimensional sections of the moduli space parametrized by a global complex mass scale v display three qualitatively different regions depending on the ratio between |v| and the dynamically generated scale Lambda. At large |v|/Lambda, instantons are exponentially suppressed as N goes to infinity. When |v| is of order Lambda, singularities due to massless dyons occur. They are densely distributed in rings of calculable thicknesses in the v-plane. At small |v|/Lambda, instantons disintegrate into fractional instantons of charge 1/(2N). These fractional instantons give non-trivial contributions to all orders of 1/N, unlike a planar diagrams expansion which generates a series in 1/N^2, implying the presence of open strings. We have explicitly calculated the fractional instantons series in two representative examples, including the 1/N and 1/N^2 corrections. Our most interesting finding is that the 1/N expansion breaks down at singularities on the moduli space due to severe infrared divergencies, a fact that has remarkable consequences.
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References
How the literature uses it
5 arXiv papers cite this in 9 sentences
Papers citing it · 3 sentences without a confident label
Builds on it 1 paper
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To find $μ$, we use the integrated form of ([ref]): [equation] Substituting the solution ([ref]) we obtain: [equation] This generalizes the solution of the pure $𝒩=2$ SYM in the 't Hooft limit [ref] $^3$ to the solution of $𝒩=2$ SQCD in the Veneziano limit.
Massive N=2 Gauge Theories at Large N · Super-QCD with $2N_f$ massive hypermultiplets · 0.97
Compares with it 2 papers
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Using the asymptotic form of the kernel: [equation] we can see that in the scaling limit the Hilbert kernel scales away, and we are left with the equation [equation] Differentiating this equation twice, we then get: [equation] This equation has a unique normalizable solution: [equation] This can be seen to agree with the eigenvalue density [ref] obtained from Seiberg-Witten theory directly in flat space.
Large N Limit of N=2 SU(N) Gauge Theories from Localization · Large radius · 0.97
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The saddle-point equations of the localization matrix model reproduce [ref] in this corner of the phase diagram the large-$N$ solution of $𝒩=2$ SYM, known from the Seiberg-Witten theory [ref] .
Localization and AdS/CFT Correspondence · Massive theory · 0.80
Cites it as background 2 papers
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Such a distribution has been considered several times in the literature and its properties have been discussed in various contexts, see for example [ref] .
Modular anomaly equations in N=2* theories and their large-N limit · Large-$N$ limit with a uniform distribution · 0.97
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The large-$N$ limit of the latter was investigated in [ref] for pure gauge $𝒩=2$ super-Yang-Mills (SYM).
Massive N=2 Gauge Theories at Large N · Introduction · 0.91
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