ALP-ine quests at the LHC: hunting axion-like particles via peaks and dips in $$ t\overline{t} $$ production

interference: effect interpretation of experiments: CERN LHC Coll spin: correlation dip 610 FOS: Physical sciences Top Quark QC770-798 interpretation of experiments: CMS 530 mass spectrum High Energy Physics - Phenomenology (hep-ph) Nuclear and particle physics. Atomic energy. Radioactivity TeV Axions and ALPs info:eu-repo/classification/ddc/530 pseudoscalar Specific BSM Phenomenology two-photon angular correlation Physics ddc:530 gluon sensitivity High Energy Physics - Phenomenology axion-like particles top: pair production Multi-Higgs Models new particle
DOI: 10.1007/jhep12(2024)197 Publication Date: 2025-01-06T23:21:24Z
ABSTRACT
A bstract We present an analysis of the sensitivity current and future LHC searches for new spin-0 particles in top–anti-top-quark $$ \left(t\overline{t}\right) <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfenced> <mml:mrow> <mml:mi>t</mml:mi> <mml:mover> <mml:mo>¯</mml:mo> </mml:mover> </mml:mrow> </mml:mfenced> </mml:math> final states, focusing on generic axion-like (ALPs) that are coupled to top quarks gluons. As a first step, we derive limits effective ALP Lagrangian terms Wilson coefficients c t {c}_{\overset{\sim }{G}} <mml:msub> <mml:mi>c</mml:mi> <mml:mi>G</mml:mi> <mml:mo>~</mml:mo> </mml:msub> based results CMS search using 35 . 9 fb − 1 data, collected at \sqrt{s} <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> = 13 TeV. then investigate how production with couplings gluons can be distinguished from pseudoscalar which couples exclusively via top-quark loop. To this end, make use invariant t\overline{t} mass distribution angular correlations sensitive spin correlation. Using 400 GeV as example, find already data during Run 2 3 provides interesting underlying nature possible particle. also analyze prospects anticipated high-luminosity phase LHC. Finally, compare obtained existing experimental bounds narrow di-photon resonances, measurements four quarks, global analyses ALP–SMEFT interference effects.
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