hep-phMay 18, 2026

Probing SMEFT Operators through t\bar{t}t\bar{t} Production with Hyper-Graph Neural Networks at the LHC

Authors: Amir SubbaSanmay Ganguly

Abstract

We present a phenomenological study of ttˉttˉt\bar{t}t\bar{t} production in proton-proton collisions at s=13\sqrt{s} = 13~TeV, using a Hyper-Graph Neural Network (H-GNN) to discriminate multilepton signal events from the dominant SM backgrounds, namely ttˉWt\bar{t}W, ttˉZt\bar{t}Z, ttˉHt\bar{t}H, ttˉVVt\bar{t}VV, single-top associated production, and diboson and triboson processes. In the H-GNN architecture each event is represented as a hypergraph whose nodes correspond to reconstructed jets and leptons and whose hyperedges encode higher-order correlations among arbitrary subsets of these objects, allowing the network to learn the many-body kinematic structures that characterize the ttˉttˉt\bar{t}t\bar{t} final state. Combining same-sign di-lepton, tri-lepton, and four-lepton channels following a CMS-like event selection, the H-GNN attains an area under the ROC curve of 0.9510.951 for the ttˉttˉt\bar{t}t\bar{t} signal and yields a statistical significance of Z=9.11Z = 9.11 at an integrated luminosity of L=140 fb1\mathcal{L} = 140~\mathrm{fb}^{-1}, to be compared with Z=8.62Z = 8.62 for a SPANet baseline, Z=7.37Z = 7.37 for a Particle Transformer baseline, and Z=5.13Z = 5.13 obtained by the ATLAS analysis, evaluated under identical event selection. We exploit the improved signal extraction to derive one- and two-parameter 95%95\% confidence level limits on the Wilson coefficients of the dimension-six operators OΦu\mathcal{O}_{Φu}, Ott(1)\mathcal{O}^{(1)}_{tt}, Oqq(1)\mathcal{O}^{(1)}_{qq}, Oqt(1)\mathcal{O}^{(1)}_{qt}, and Oqt(8)\mathcal{O}^{(8)}_{qt}, and we project the expected sensitivity at the HL-LHC integrated luminosities of 1000 fb11000~\mathrm{fb}^{-1} and 3000 fb13000~\mathrm{fb}^{-1} with 50%50\% uncertainty on the background estimation.

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