Into the EFThedron and UV constraints from IR consistency

• Published in: The journal of high energy physics Vol. 2022; no. 3; pp. 63 - 50
• Main Authors: Chiang, Li-Yuan, Huang, Yu-tin, Li, Wei, Rodina, Laurentiu, Weng, He-Chen
• Format: Journal Article
• Language: English
• Published: Berlin/Heidelberg Springer Berlin Heidelberg 01.03.2022; Springer Nature B.V; SpringerOpen
• Subjects: Classical and Quantum Gravitation; Convexity; Couplings; Effective Field Theories; Elementary Particles; Geometry; Hankel matrices; High energy physics; Permutations; Physics; Physics and Astronomy; Polytopes; Quantum Field Theories; Quantum Field Theory; Quantum Physics; Regular Article - Theoretical Physics; Relativity Theory; Scattering Amplitudes; String Theory; Symmetry; Effective Field Theories; Scattering Amplitudes
• ISSN: 1029-8479; 1029-8479
• DOI: 10.1007/JHEP03(2022)063

A bstract Recently it was proposed that the theory space of effective field theories with consistent UV completions can be described as a positive geometry, termed the EFThedron. In this paper we demonstrate that at the core, the geometry is given by the convex hull of the product of two moment curves. This makes contact with the well studied bi-variate moment problem, which in various instances has known solutions, generalizing the Hankel matrices of couplings into moment matrices. We extend these solutions to hold for more general bi-variate problem, and are thus able to obtain analytic expressions for bounds, which closely match (and in some cases exactly match) numerical results from semi-definite programing methods. Furthermore, we demonstrate that crossing symmetry in the IR imposes non-trivial constraints on the UV spectrum. In particular, permutation invariance for identical scalar scattering requires that any UV completion beyond the scalar sector must contain arbitrarily high spins, including at least all even spins ℓ ≤ 28, with the ratio of spinning spectral functions bounded from above, exhibiting large spin suppression. The spinning spectrum must also include at least one state satisfying a bound m J 2 < M h 2 J 2 − 12 J 4 − 32 J 2 + 204 8 150 − 43 J 2 + 2 J 4 , where J 2 = ℓ ( ℓ +1), and M h is the mass of the heaviest spin 2 state in the spectrum.