Infrared finite observables in \({\mathcal N}=8\) supergravity
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Publication:641901
DOI10.1134/S0081543811010056zbMath1228.83111arXiv1008.2302MaRDI QIDQ641901
A. V. Zhiboedov, Grigory Vartanov, Dmitri I. Kazakov, Leonid V. Bork
Publication date: 25 October 2011
Published in: Proceedings of the Steklov Institute of Mathematics (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1008.2302
Related Items (3)
One-loop superconformal and Yangian symmetries of scattering amplitudes in \( \mathcal{N} = 4 \) super Yang-Mills ⋮ On form factors in \(\mathcal{N} = 4\) SYM ⋮ On NMHV form factors in \( \mathcal{N}=4 \) SYM theory from generalized unitarity
Cites Work
- An analytic result for the two-loop hexagon Wilson loop in \( \mathcal{N} = 4 \) SYM
- The footprint of \(E_{7(7)}\) in amplitudes of \(\mathcal N= 8\) supergravity
- Is \(\mathcal N=8\) supergravity ultraviolet finite?
- Explicit action of \(E_{7(7)}\) on \(\mathcal N=8\) supergravity fields plasma from boost invariant expansion
- Multi-leg one-loop gravity amplitudes from gauge theory
- One-loop \(n\)-point gauge theory amplitudes, unitarity and collinear limits.
- What is the simplest quantum field theory?
- String theory dualities and supergravity divergences
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- Infinities within graviton scattering amplitudes
- Mass Singularities of Feynman Amplitudes
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