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The Effective Action of N=8 Supergravity
High Energy Physics - Theory · Submitted 14 Nov 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim By generalizing the dimensional arguments in superspace to non-local invariants, we show that the 1-loop effective action does not contain any contributions from bubble and triangle diagrams.
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The abstract, sentence by sentence
We present a simple form of the on-shell gauge-invariant 1-loop effective action of N=8 supergravity which is manifestly N=8 supersymmetric at the linear level. By generalizing the dimensional arguments in superspace to non-local invariants, we show that the 1-loop effective action does not contain any contributions from bubble and triangle diagrams. The absence of bubbles implies the absence of conformal and axial anomalies. We also show that the 1-loop effective action of N=8 supergravity features a "dual" conformal symmetry in the momentum space.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a simple form of the on-shell gauge-invariant 1-loop effective action of N=8 supergravity which is manifestly N=8 supersymmetric at the linear level. | contribution 0.96 | 0.95 | 0.28 | asserted 1.00 |
| s1 | By generalizing the dimensional arguments in superspace to non-local invariants, we show that the 1-loop effective action does not contain any contributions from bubble and triangle diagrams. | result 0.79 | 0.94 | 0.37 | asserted 1.00 |
| s2 | The absence of bubbles implies the absence of conformal and axial anomalies. | interpretation 0.96 | 0.72 | 0.17 | asserted 1.00 |
| s3 | We also show that the 1-loop effective action of N=8 supergravity features a "dual" conformal symmetry in the momentum space. | result 0.97 | 0.94 | 0.15 | asserted 1.00 |
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The paper
Original abstract
We present a simple form of the on-shell gauge-invariant 1-loop effective action of N=8 supergravity which is manifestly N=8 supersymmetric at the linear level. By generalizing the dimensional arguments in superspace to non-local invariants, we show that the 1-loop effective action does not contain any contributions from bubble and triangle diagrams. The absence of bubbles implies the absence of conformal and axial anomalies. We also show that the 1-loop effective action of N=8 supergravity features a "dual" conformal symmetry in the momentum space.
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References
How the literature uses it
10 arXiv papers cite this in 15 sentences
Papers citing it · 11 sentences without a confident label
Uses its data or values 1 paper
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For the 1-loop UV finite amplitude [ref] we take according to [ref] , [ref] P^1-loop (1^+, 2^+, 3^+, 4^+)= P^3_UV F^box where $P^3_UV$ is dimensionless P^3_UV (1^+, 2^+, 3^+, 4^+)= ( s_12 s_14 ⟨1 2⟩⟨23⟩⟨34⟩⟨41⟩)^2.
N=8 Supergravity 4-point Amplitudes · The 4-point generating function in =8 SG · 0.89
Cites it as support 1 paper
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Our observation that the UV divergent terms in the S-matrix in different gauges are incompatible with each other leads to a prediction that the perturbative =8 supergravity amplitudes are all-loop finite, if there are no anomalies.[The recent proof of the no-triangle conjecture in [ref] , [ref] may be an indication of the absence of anomalies as suggested in [ref] .
On a possibility of a UV finite N=8 supergravity · All-loop argument for the $n$-particle UV finiteness · 1.00
Cites it as background 2 papers
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Any one-loop amplitude may be expressed both as a sum over Feynman diagrams, and also in terms of scalar box integrals[For a superspace effective action perspective on one-loop amplitudes, see [ref] .]:
On the structure of scattering amplitudes in N=4 super Yang-Mills and N=8 supergravity · One-Loop Amplitudes in $N=4$ SYM and $N=8$ Supergravity · 0.94
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There are several indications that maximal supergravity may be an extraordinarily remarkable theory [ref] , and possibly even ultraviolet finite [ref] , but our feeling is that even at tree level we are still far from fully unlocking the structure of graviton amplitudes.
The Tree Formula for MHV Graviton Amplitudes · Introduction · 0.80
What it cites · 28 sentences without a confident label
Uses the method or tool of 2 papers
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Here we will present our results for non-local manifestly supersymmetric =4 SYM and =8 supergravity effective actions using dual conformal coordinates [ref] .
On planar gluon amplitudes/Wilson loops duality · On the dual conformal symmetry of the effective action · 0.90
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This action acquires a simple form after a dualization as performed in [ref] .
Simplifying superstring action on AdS_5 x S^5 · On the dual conformal symmetry of the effective action · 0.86
Compares with 2 papers
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To the best of our understanding, this fact corresponds to the no-triangle hypothesis for the 1-loop graphs in =8 supergravity as formulated in [ref] , despite the difference in the two approaches.
One-Loop n-Point Gauge Theory Amplitudes, Unitarity and Collinear Limits · Discussion · 0.95
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If the relation between our approach and that in [ref] can be fully clarified, it may lead to a proof of the no-triangle property of the 1-loop graphs in =8 supergravity in the form required in [ref] .
Three-Loop Superfiniteness of N=8 Supergravity · Discussion · 0.89
Cites as background 11 papers
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The results of the 3-loop computations have been reported in [ref] .
Three-Loop Superfiniteness of N=8 Supergravity · Introduction · 0.80
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A careful treatment of the supergraphs in the background field method in supersymmetric theories was made in [ref] , [ref] and in the harmonic superspace in [ref] , [ref] .
(N,p,q) Harmonic Superspace · Introduction · 0.92
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According to [ref] , [ref] , they may start at the 8-loop level, or even earlier, at the 3-loop level, according to [ref] , or from the 5-loop level [ref] .
Supersymmetry counterterms revisited · Introduction · 0.80
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