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On Domain Walls of N=1 Supersymmetric Yang-Mills in Four Dimensions
High Energy Physics - Theory · Submitted 1 Mar 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This leads to a counting of BPS degeneracies of domain walls in agreement with expected results.
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The abstract, sentence by sentence
We study the BPS domain walls of supersymmetric Yang-Mills for arbitrary gauge group. We describe the degeneracies of domain walls interpolating between arbitrary pairs of vacua. A recently proposed large N duality sheds light on various aspects of such domain walls. In particular, for the case of G = SU(N) the domain walls correspond to wrapped D-branes giving rise to a 2+1 dimensional U(k) gauge theory on the domain wall with a Chern-Simons term of level N. This leads to a counting of BPS degeneracies of domain walls in agreement with expected results.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the BPS domain walls of supersymmetric Yang-Mills for arbitrary gauge group. | contribution 1.00 | 0.91 | 0.09 | asserted 0.95 |
| s1 | We describe the degeneracies of domain walls interpolating between arbitrary pairs of vacua. | contribution 0.90 | 0.88 | 0.13 | asserted 0.99 |
| s2 | A recently proposed large N duality sheds light on various aspects of such domain walls. | background 0.91 | 0.10 | 0.07 | asserted 0.77 |
| s3 | In particular, for the case of G = SU(N) the domain walls correspond to wrapped D-branes giving rise to a 2+1 dimensional U(k) gauge theory on the domain wall with a Chern-Simons term of level N. | result 0.58 | 0.30 | 0.40 | asserted 1.00 |
| s4 | This leads to a counting of BPS degeneracies of domain walls in agreement with expected results. | result 0.85 | 0.69 | 0.44 | asserted 0.95 |
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The paper
Original abstract
We study the BPS domain walls of supersymmetric Yang-Mills for arbitrary gauge group. We describe the degeneracies of domain walls interpolating between arbitrary pairs of vacua. A recently proposed large N duality sheds light on various aspects of such domain walls. In particular, for the case of G = SU(N) the domain walls correspond to wrapped D-branes giving rise to a 2+1 dimensional U(k) gauge theory on the domain wall with a Chern-Simons term of level N. This leads to a counting of BPS degeneracies of domain walls in agreement with expected results.
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References
How the literature uses it
42 arXiv papers cite this in 80 sentences
Papers citing it · 51 sentences without a confident label
Builds on it 2 papers
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In this section we will derive a full generalization of the Acharya-Vafa formula [ref] while staying in field theory framework.
Degenerate Domain Walls in Supersymmetric Theories · SYM on a cylinder: Moduli and symmetries · 1.00
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In particular, starting with a known $𝒩=2$ enhancement point of the $T_𝒩=1[L(p,1)]$ theory [ref] , we propose a quiver description for the $T_𝒩=1[L(p,q)]$ theory.
Higher-Form Symmetries, Bethe Vacua, and the 3d-3d Correspondence · 3d $𝒩=1$ · 0.80
Uses its method or tool 1 paper
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Indices for such theories are computed in [ref] , following [ref] .[Deforming to $𝒩=3$ Yang-Mills theory might be physically more natural, considering the origin of M2-brane theories from $𝒩=3$ D-brane systems.
Supersymmetric vacua of mass-deformed M2-brane theory · Introduction and discussions · 0.82
Uses its data or values 2 papers
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Indeed, for the AV CS theory the Witten index was computed in [ref] and was found to be proportional to $1/(N-k)!$.
Brane Dynamics and 3D Seiberg Duality on the Domain Walls of 4D N=1 SYM · Pseudo-moduli, the s-rule and brane creation · 0.86
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For these 3d $𝒩 = 1$ Chern-Simons theories $T_𝒩 = 1[L(p,q)]$ the Witten index was computed in [ref] to be I_T^3(T_𝒩 = 1[L(p,q),U(N)]) = p N .
An $\mathcal{N}=1$ 3d-3d Correspondence · Specializing $M_3$: $T_𝒩 = 1[L(p,q), U(N)]$ · 0.96
Compares with it 6 papers
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After T-duality this setup bears many similarities with the large-$N$ dual string theory background of [ref] but is not identical to it.
Brane Dynamics and 3D Seiberg Duality on the Domain Walls of 4D N=1 SYM · Introduction · 0.91
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As we have already mentioned in the Introduction, for $k=1$ the obtained action is level/rank dual [ref] to the Acharya-Vafa [ref] worldvolume theory of the $k=1$ domain wall, but differs from the latter for $k>1$.
Supermembranes and domain walls in $\mathcal N=1$, $D=4$ SYM · Membrane coupled to SYM · 0.98
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The effective theory in this vacuum agrees with the theory that Acharya and Vafa (AV) discovered to govern the dynamics on domain walls in $SU(N)$ SYM [ref] .
Living on the walls of super-QCD · Introduction and summary of results · 0.85
Cites it as support 2 papers
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Assuming that this is the case, the rest of the anomaly corresponding to $ν'=ν-1=G-1$ is accounted for by the TQFT living on the domain wall.[It requires some computation to determine that the goldstino corresponds to $ν=1$ rather than $ν=-1$. ] In fact, it was argued that some TQFT does live on the domain wall [ref] .
On time-reversal anomaly of 2+1d topological phases · Semion-fermion theory on a SYM domain wall · 0.98
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However, from various indirect field theory arguments in [ref] as well as successful applications of Yang-Mills Chern-Simons index on $T^2$ to D-branes living on uncompactified $ℝ^2+1$ [ref] , we believe that our calculation also provides the vacuum counting for M2-branes living on $ℝ^2+1$.
Supersymmetric vacua of mass-deformed M2-brane theory · Introduction and discussions · 1.00
Cites it as background 12 papers
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Nevertheless, in the recent years our understanding of these theories has overcome a new twist [ref] (see also [ref] for earlier considerations).
Phases of $\mathcal{N}=1$ Quivers in $2+1$ Dimensions · Introduction · 0.83
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This question has been analyzed in great detail by Acharya and Vafa [ref] .
Living on the walls of super-QCD · Domain walls of SYM: a review · 0.95
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Holographically, domain walls are described by 5-branes wrapping compact 3-cycles of the internal geometry, with the other three directions being along $ℝ^1,3$ [ref] (see also [ref] for a construction within the KS model).
Confinement in a finite duality cascade · Domain walls - holographic description · 0.83
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