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Weak boson fusion at 100 TeV

2017/02/16 by Dorival Gonçalves, Dorival Goncalves, Tilman Plehn +2 · 1 citation
Physics and Astronomy · #Boson #Fusion #Higgs boson #High-Energy Particle Collisions Research #Jet (fluid) #Large Hadron Collider #Muon collider #Nuclear physics #Particle Detector Development and Performance #Particle accelerator #Particle physics #Particle physics theoretical and experimental studies #Physics #Yukawa potential #hep-ph

paper · pdf · doi:10.1103/physrevd.95.095011

published as Phys. Rev. D 95, 095011 (2017) · 18 pages, 16 figures

arxiv created 2017/02/16 · openalex publication_date 2017/05/16 · arxiv updated 2017/05/24 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

From the LHC runs we know that, with increasing collider energy, weak-boson-fusion Higgs production dominates as an environment for precision measurements. We show how a future hadron collider performs for three challenging benchmark signatures. Because all of these measurements rely on the tagging jet signature, we first give a comprehensive analysis of weak-boson-fusion kinematics and a proposed two-step jet veto at a 100 TeV hadron collider. We then find this machine to be sensitive to invisible Higgs branching ratios of 0.5%, a second-generation muon Yukawa coupling of 2%, and an enhanced total Higgs width of around 5%, the latter with essentially no model dependence. This kind of performance crucially relies on a sufficient detector coverage and a dedicated weak-boson-fusion trigger channel.

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