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Four-Dimensional Superconformal Theories with Interacting Boundaries or Defects
High Energy Physics - Theory · Submitted 3 Mar 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Moreover we derive Callan-Symanzik equations for these models using their superconformal transformation properties and show that the beta functions vanish to all orders in perturbation theory, such that the models remain superconformal upon quantization.
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We study four-dimensional superconformal field theories coupled to three-dimensional superconformal boundary or defect degrees of freedom. Starting with bulk N=2, d=4 theories, we construct abelian models preserving N=2, d=3 supersymmetry and the conformal symmetries under which the boundary/defect is invariant. We write the action, including the bulk terms, in N=2, d=3 superspace. Moreover we derive Callan-Symanzik equations for these models using their superconformal transformation properties and show that the beta functions vanish to all orders in perturbation theory, such that the models remain superconformal upon quantization. Furthermore we study a model with N=4 SU(N) Yang-Mills theory in the bulk coupled to a N=4, d=3 hypermultiplet on a defect. This model was constructed by DeWolfe, Freedman and Ooguri, and conjectured to be conformal based on its relation to an AdS configuration studied by Karch and Randall. We write this model in N=2, d=3 superspace, which has the distinct advantage that non-renormalization theorems become transparent. Using N=4, d=3 supersymmetry, we argue that the model is conformal.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study four-dimensional superconformal field theories coupled to three-dimensional superconformal boundary or defect degrees of freedom. | contribution 0.90 | 0.86 | 0.06 | asserted 0.94 |
| s1 | Starting with bulk N=2, d=4 theories, we construct abelian models preserving N=2, d=3 supersymmetry and the conformal symmetries under which the boundary/defect is invariant. | contribution 0.60 | 0.94 | 0.07 | asserted 1.00 |
| s2 | We write the action, including the bulk terms, in N=2, d=3 superspace. | method 0.83 | 0.95 | 0.03 | asserted 1.00 |
| s3 | Moreover we derive Callan-Symanzik equations for these models using their superconformal transformation properties and show that the beta functions vanish to all orders in perturbation theory, such that the models remain superconformal upon quantization. | result 0.92 | 0.95 | 0.49 | asserted 1.00 |
| s4 | Furthermore we study a model with N=4 SU(N) Yang-Mills theory in the bulk coupled to a N=4, d=3 hypermultiplet on a defect. | contribution 0.99 | 0.78 | 0.04 | asserted 0.98 |
| s5 | This model was constructed by DeWolfe, Freedman and Ooguri, and conjectured to be conformal based on its relation to an AdS configuration studied by Karch and Randall. | background 0.98 | 0.04 | 0.05 | speculative 0.48 |
| s6 | We write this model in N=2, d=3 superspace, which has the distinct advantage that non-renormalization theorems become transparent. | method 0.83 | 0.91 | 0.05 | asserted 0.99 |
| s7 | Using N=4, d=3 supersymmetry, we argue that the model is conformal. | result 0.71 | 0.90 | 0.30 | asserted 0.74 |
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The paper
Original abstract
We study four-dimensional superconformal field theories coupled to three-dimensional superconformal boundary or defect degrees of freedom. Starting with bulk N=2, d=4 theories, we construct abelian models preserving N=2, d=3 supersymmetry and the conformal symmetries under which the boundary/defect is invariant. We write the action, including the bulk terms, in N=2, d=3 superspace. Moreover we derive Callan-Symanzik equations for these models using their superconformal transformation properties and show that the beta functions vanish to all orders in perturbation theory, such that the models remain superconformal upon quantization. Furthermore we study a model with N=4 SU(N) Yang-Mills theory in the bulk coupled to a N=4, d=3 hypermultiplet on a defect. This model was constructed by DeWolfe, Freedman and Ooguri, and conjectured to be conformal based on its relation to an AdS configuration studied by Karch and Randall. We write this model in N=2, d=3 superspace, which has the distinct advantage that non-renormalization theorems become transparent. Using N=4, d=3 supersymmetry, we argue that the model is conformal.
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References
How later papers used it
63 later papers cite it
1 later paper by other authors is listed below: 1 used its method or tool.
Uses its method or tool 1 of 4 papers with this label
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Used the same embedding of three-dimensional N=2 superspace into four-dimensional N=2 superspace as this paper.
Super Yang-Mills Theory with Impurity Walls and Instanton Moduli Spaces (2011) · 0.99 · paraphrased: the licence does not allow quoting
How the literature uses it
60 arXiv papers cite this in 88 sentences
Papers citing it · 35 sentences without a confident label
Builds on it 3 papers
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In this paper we will study the dynamics of the theory on the world volume of a mixed D3 and D5 brane construction with a 2+1 dimensional intersection$^1$ , which has previously been studied at zero temperature in the absence of chemical potential in [ref] .
R-Charge Chemical Potential in a 2+1 Dimensional System · Introduction · 0.91
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In this paper we will study the dynamics of the theory on the world volume of a mixed D3 and D5 brane construction with a 2+1 dimensional intersection, which has previously been studied at zero temperature in the absence of chemical potential in [ref] .
Chemical Potential in the Gravity Dual of a 2+1 Dimensional System · Introduction · 0.89
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This is the nonabelian version of the map given in [ref] 's equations (2.18)-(2.21).
Supersymmetry of the D3/D5 Defect Field Theory · Mapping Between Superspace-Based Formulations · 0.97
Uses its method or tool 4 papers
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For this purpose we can write the fields of 4$d$ $𝒩=4$ SYM in terms of 3$d$ $𝒩=2$ superspace, following the formalism of [ref] .
Boundaries and Defects of N=4 SYM with 4 Supercharges, Part I: Boundary/Junction Conditions · D5-like Junction · 0.99
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We use the same embedding of $_3d=2$ superspace into $_4d=2$ superspace as in [ref] ; the details are provided in the appendix for completeness.
Super Yang-Mills Theory with Impurity Walls and Instanton Moduli Spaces · Field content · 0.99
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This was done in [ref] , by organizing the 4d fields in supermultiplets of the 3d SUSY.
The Virtue of Defects in 4D Gauge Theories and 2D CFTs · Janus Domain Wall · 0.80
Compares with it 3 papers
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Then the remaining symmetry is smaller than the case in [ref] which treats the boundary on the flat space.
Localization of four-dimensional super Yang-Mills theories compactified on Riemann surface · Introduction and Summary · 0.94
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A similar construction of the 4-dimensional Lagrangian is done in [ref] where they described the bulk 4-dimensional theory by 3-dimensional superfields.
Construction of 4d SYM compactified on open Riemann surfaces by the superfield formalism · Introduction and summary · 0.82
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The interface theories are different in character from the defect CFT discussed in the AdS/CFT context in [ref] .
Exact half-BPS Type IIB interface solutions I: Local solution and supersymmetric Janus · Interface Yang-Mills with maximal supersymmetry · 0.98
Cites it as support 1 paper
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This conformal invariance can also be shown directly by an analysis of the field theory [ref] .
Transport Properties of Holographic Defects · D5-branes · 0.96
Cites it as background 36 papers
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Holographic descriptions of $N=4$ super Yang-Mills theory [ref] with defect D5 probe branes [ref] (and other related systems [ref] ) provide a calculable system with similar gross properties - fermions on the defect interacting by higher dimension conformal gauge fields.
Holographic Graphene in a Cavity · Introduction · 0.91
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In the string-theory literature conformal interfaces were first studied as holographic duals [ref] to codimension-one anti-de Sitter branes [ref] .
On the Symmetries of Classical String Theory · Interfaces as spectrum-generating symmetries · 0.86
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We consider four-dimensional $𝒩=4$ SYM theory in the bulk interacting with a defect of codimension one situated at $x_3=0$ [ref] .
Two-point functions in AdS/dCFT and the boundary conformal bootstrap equations · Action and propagators · 0.89
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