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

A bstract 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...

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Published inThe journal of high energy physics Vol. 2024; no. 3; pp. 180 - 47
Main Authors Chen, Qing, Mimasu, Ken, Wu, Tong Arthur, Zhang, Guo-Dong, Zhou, Shuang-Yong
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 29.03.2024
Springer Nature B.V
SpringerOpen
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Summary:A bstract 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 ((4 π ) 2 ). 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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ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP03(2024)180