Dilepton production in the SMEFT at $\mathcal O(1/\Lambda^4)$

TL;DR

This paper investigates the impact of including dimension-6 squared and dimension-8 operators in SMEFT analyses of LHC dilepton data, revealing significant effects on bounds and the importance of certain operators for accurate fits.

Contribution

It provides a comprehensive analysis of dimension-6 and dimension-8 operators at next-to-leading-order, highlighting their effects on LHC dilepton data fits and proposing a subset of operators to include.

Findings

Dimension-6 squared terms significantly affect fits.

Dimension-8 operators can be probed at several-TeV scales.

Including dimension-8 operators alters bounds on dimension-6 operators.

Abstract

We study the inclusion of $\mathcal O(1/\Lambda^4)$ effects in the Standard Model Effective Field Theory in fits to the current Drell-Yan data at the LHC. Our analysis includes the full set of dimension-6 and dimension-8 operators contributing to the dilepton process, and is performed to next-to-leading-order in the QCD coupling constant at both $\mathcal O(1/\Lambda^2)$ and $\mathcal O(1/\Lambda^4)$. We find that the inclusion of dimension-6 squared terms and certain dimension-8 operators has significant effects on fits to the current data. Neglecting them leads to bounds on dimension-6 operators off by large factors. We find that dimension-8 four-fermion operators can already be probed to the several-TeV level by LHC results, and that their inclusion significantly changes the limits found for dimension-6 operators. We discuss which dimension-8 operators should be included in fits to the LHC data. Only a manageable subset of two-derivative dimension-8 four-fermion operators need to be included at this stage given current LHC uncertainties.