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Capping the positivity cone: dimension-8 Higgs operators in the SMEFT

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arxiv 2309.15922 v2 pith:Y343IHFR submitted 2023-09-27 hep-ph hep-th

Qing Chen , Ken Mimasu , Tong Arthur Wu , Guo-Dong Zhang , Shuang-Yong Zhou This is my paper
classification hep-phhep-th
keywords boundspositivityunitaritydimension-8smeftcoefficientsconditionscone
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

SMEFT Wilson coefficients are subject to various positivity bounds in order to be consistent with the fundamental principles of S-matrix. Previous bounds on dimension-8 SMEFT operators have been obtained using the positivity part of UV partial wave unitarity and form a (projective) convex cone. We derive a set of linear UV unitarity conditions that go beyond positivity and are easy to implement in an optimization scheme with dispersion relations in a multi-field EFT. Using Higgs scattering as an example, we demonstrate how to obtain closed bounds in the space of the three relevant dimension-8 coefficients, making use of the UV unitarity conditions as well as so-called null constraints that arise from full crossing symmetry. Specifically, we show that they are bounded by inequalities schematically going like $C<O\left((4\pi)^2\right)$. We compare the newly obtained upper bounds with the traditional perturbative unitarity bounds from within the EFT, and discuss some phenomenological implications of the two-sided positivity bounds in the context of experimental probes of Vector Boson Scattering.

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Cited by 6 Pith papers

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  1. Full positivity bounds for anomalous quartic gauge couplings in SMEFT

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    Thermodynamic consistency in thermal scalar EFTs requires the Wilson coefficient of the leading dimension-8 operator to be strictly positive.

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