2023
DOI: 10.1007/jhep06(2023)064
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Where is M-theory in the space of scattering amplitudes?

Abstract: We use the S-matrix bootstrap to carve out the space of unitary, analytic, crossing symmetric and supersymmetric graviton scattering amplitudes in nine, ten and eleven dimensions. We extend and improve the numerical methods of our previous work in ten dimensions. A key new tool employed here is unitarity in the celestial sphere. In all dimensions, we find that the minimal allowed value of the Wilson coefficient α, controlling the leading correction to maximal supergravity, is very close but not equal to the mi… Show more

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Cited by 14 publications
(2 citation statements)
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“…In turn, the consistency of anomaly inflow on these defects can restrict the theory even with lower amounts of supersymmetry, as exemplified in [23]. Perhaps one can achieve more mileage complementing such kinematical considerations with dynamical ones, for instance relying on S-matrix bootstrap techniques along the lines of [103,104]. Another promising avenue is the study of equivariant topological modular forms [105][106][107], a generalised cohomology theory believed to encode deformation classes of 2d SQFTs (and thus of heterotic worldsheets) [108] according to the Stolz-Teichner conjecture [43].…”
Section: Jhep04(2024)067 9 Conclusionmentioning
confidence: 99%
“…In turn, the consistency of anomaly inflow on these defects can restrict the theory even with lower amounts of supersymmetry, as exemplified in [23]. Perhaps one can achieve more mileage complementing such kinematical considerations with dynamical ones, for instance relying on S-matrix bootstrap techniques along the lines of [103,104]. Another promising avenue is the study of equivariant topological modular forms [105][106][107], a generalised cohomology theory believed to encode deformation classes of 2d SQFTs (and thus of heterotic worldsheets) [108] according to the Stolz-Teichner conjecture [43].…”
Section: Jhep04(2024)067 9 Conclusionmentioning
confidence: 99%
“…By now positivity bounds have been derived in a variety of contexts, including without and with gravity, see, e.g., [72][73][74][75][76][77][78] and with [79][80][81][82][83][84][85][86][87] respectively, and [88] for reviews. The impact of broken Lorentz invariance has been considered in [89][90][91] and in a quantum gravitational context, positivity bounds have been considered in string theory [92][93][94]. In order to make use of results on photon self-interactions in asymptotically safe gravity [95][96][97], we focus on positivity bounds for the photon [1,[98][99][100].…”
mentioning
confidence: 99%