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The AdS3 boundary energy momentum tensor, exact in the string length over the curvature radius
High Energy Physics - Theory · Submitted 22 Jun 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The bottom-line is a canonical shift in the normalization of the boundary energy-momentum tensor corresponding to a shift in the curvature radius over the string length squared by the dual Coxeter number of the SL(2,R) subalgebra of the space-time Virasoro algebra.
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The abstract, sentence by sentence
We first clarify the relation between boundary perturbations of AdS3 in general relativity, and exactly marginal worldsheet vertex operators in AdS3 string theory with Neveu-Schwarz Neveu-Schwarz flux. The latter correspond to solutions of the higher derivative low-energy tree level effective action to all orders in the string length over the curvature radius. We then calculate the exact expression of the boundary energy momentum tensor including all these higher derivative corrections in a purely bosonic string theory. The bottom-line is a canonical shift in the normalization of the boundary energy-momentum tensor corresponding to a shift in the curvature radius over the string length squared by the dual Coxeter number of the SL(2,R) subalgebra of the space-time Virasoro algebra. That allows us to derive the value of the Brown-Henneaux central charge including all tree level higher derivative corrections in bosonic string theory, in a scheme dictated by the worldsheet conformal field theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We first clarify the relation between boundary perturbations of AdS3 in general relativity, and exactly marginal worldsheet vertex operators in AdS3 string theory with Neveu-Schwarz Neveu-Schwarz flux. | contribution 0.92 | 0.71 | 0.04 | asserted 0.96 |
| s1 | The latter correspond to solutions of the higher derivative low-energy tree level effective action to all orders in the string length over the curvature radius. | background 0.52 | 0.21 | 0.06 | asserted 1.00 |
| s2 | We then calculate the exact expression of the boundary energy momentum tensor including all these higher derivative corrections in a purely bosonic string theory. | contribution 0.93 | 0.95 | 0.10 | asserted 1.00 |
| s3 | The bottom-line is a canonical shift in the normalization of the boundary energy-momentum tensor corresponding to a shift in the curvature radius over the string length squared by the dual Coxeter number of the SL(2,R) subalgebra of the space-time Virasoro algebra. | result 0.95 | 0.87 | 0.83 | asserted 1.00 |
| s4 | That allows us to derive the value of the Brown-Henneaux central charge including all tree level higher derivative corrections in bosonic string theory, in a scheme dictated by the worldsheet conformal field theory. | result 0.91 | 0.92 | 0.32 | asserted 1.00 |
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The paper
Original abstract
We first clarify the relation between boundary perturbations of AdS3 in general relativity, and exactly marginal worldsheet vertex operators in AdS3 string theory with Neveu-Schwarz Neveu-Schwarz flux. The latter correspond to solutions of the higher derivative low-energy tree level effective action to all orders in the string length over the curvature radius. We then calculate the exact expression of the boundary energy momentum tensor including all these higher derivative corrections in a purely bosonic string theory. The bottom-line is a canonical shift in the normalization of the boundary energy-momentum tensor corresponding to a shift in the curvature radius over the string length squared by the dual Coxeter number of the SL(2,R) subalgebra of the space-time Virasoro algebra. That allows us to derive the value of the Brown-Henneaux central charge including all tree level higher derivative corrections in bosonic string theory, in a scheme dictated by the worldsheet conformal field theory.
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References
How the literature uses it
4 arXiv papers cite this in 8 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 2 papers
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In string theory, the central charge in the space-time boundary conformal field theory was computed in $AdS_3$ with Neveu-Schwarz-Neveu-Schwarz flux in [ref] [ref] [ref] [ref] [ref] and for the case of $AdS_3$ with Ramond-Ramond flux in [ref] .
The AdS3 central charge in string theory · Introduction · 0.92
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More recently, in the series of papers [ref] , the $AdS_3$ background with RR flux has been considered from the point of view of the worldsheet current algebra and its massless sector and other interesting observables have been computed.
Superstrings in AdS · $b$ antighost · 0.95
What it cites · 23 sentences without a confident label
Uses the method or tool of 5 papers
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Using a similar equation for deriving with respect to $x̅$, we obtain the result: [equation] From now on, we again follow [ref] closely and compute the operator product $∂_x̅ T(x)T(y)$.
More Comments on String Theory on AdS_3 · The $TT$ operator product · 0.93
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One can do this by the techniques developed in [ref] and applied in [ref] [One uses the Ward identities computed in appendix A of [ref] and applies them to the operator $Φ_1 J J̅$ inserted in a two-point function of two unit operators.].
Strings in AdS_3 and the SL(2,R) WZW Model. Part 3: Correlation Functions · Final remark · 1.00
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One can do this by the techniques developed in [ref] and applied in [ref] [One uses the Ward identities computed in appendix A of [ref] and applies them to the operator $Φ_1 J J̅$ inserted in a two-point function of two unit operators.].
Operator product expansion and factorization in the $H_3^+$-WZNW model · Final remark · 1.00
Compares with 1 paper
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The normalization of the energy-momentum tensor is $1/(k-2)$ for a level $k$ current algebra[ Our equation differs from equation (4.15) in [ref] at higher orders in the $1/k$ expansion.
More Comments on String Theory on AdS_3 · The $TT$ operator product · 0.86
Cites as background 5 papers
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In the holographic $AdS/CFT$ correspondence [ref] [ref] [ref] the conserved boundary energy-momentum tensor couples to the massless graviton in the bulk.
The Large N Limit of Superconformal Field Theories and Supergravity · The boundary energy-momentum tensor · 0.99
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In the holographic $AdS/CFT$ correspondence [ref] [ref] [ref] the conserved boundary energy-momentum tensor couples to the massless graviton in the bulk.
Gauge Theory Correlators from Non-Critical String Theory · The boundary energy-momentum tensor · 0.99
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In the holographic $AdS/CFT$ correspondence [ref] [ref] [ref] the conserved boundary energy-momentum tensor couples to the massless graviton in the bulk.
Anti De Sitter Space And Holography · The boundary energy-momentum tensor · 0.99
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