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Weak boson probes of Higgs unitarity restoration at 10 TeV parton colliders

Christoph Englert, Wrishik Naskar, Andrew D. Pilkington, Michael Spannowsky

TL;DR

The work tackles whether Higgs coupling deviations away from the SM can signal unitarity-restoring resonances at multi-TeV scales and how to directly probe them with a $100~\text{TeV}$ FCC-hh or a $10~\text{TeV}$ muon collider. It models unitarity-restoring scenarios with a minimal spectrum (scalar $H'$ or vector $W'/Z'$) parameterized by $\mu_H = \kappa_H^2$ and resonance masses $m_{H'}, m_{V'}$, then simulates weak-boson-fusion processes and performs bump-hunt analyses using $m_{VV}$ and $m_T$ discriminants. Key findings show that both collider concepts can discover narrow resonances up to about $m_{H'}\sim 6~\text{TeV}$, with sensitivity for vector resonances depending on $\mu_H$ and fermion couplings (which can suppress certain decay channels like $Z'\to t\bar t$). The results support a modern no-lose theorem linking precision Higgs measurements with high-energy resonance searches, complemented by an FCC-ee program to corroborate deviations.

Abstract

Higgs coupling deviations, at levels accessible to the high-luminosity LHC, can imply a phenomenological no-lose theorem for the next generation of collider facilities. Correlating Higgs coupling deviations from the SM expectation in the gauge boson sector with high-scale unitarity requirements, we estimate and compare the sensitivity that can be expected at a future hadron collider (operating at 100 TeV centre-of-mass energy) and a 10 TeV muon collider. Both muon and hadron colliders offer discovery potential for mass scales up to ${\cal{O}}(6~\text{TeV})$ where unitarity violation induced by (sub)percent Higgs coupling modifications is mended. We comment on how an intermediate precision FCC-ee programme can corroborate such deviations.

Weak boson probes of Higgs unitarity restoration at 10 TeV parton colliders

TL;DR

The work tackles whether Higgs coupling deviations away from the SM can signal unitarity-restoring resonances at multi-TeV scales and how to directly probe them with a FCC-hh or a muon collider. It models unitarity-restoring scenarios with a minimal spectrum (scalar or vector ) parameterized by and resonance masses , then simulates weak-boson-fusion processes and performs bump-hunt analyses using and discriminants. Key findings show that both collider concepts can discover narrow resonances up to about , with sensitivity for vector resonances depending on and fermion couplings (which can suppress certain decay channels like ). The results support a modern no-lose theorem linking precision Higgs measurements with high-energy resonance searches, complemented by an FCC-ee program to corroborate deviations.

Abstract

Higgs coupling deviations, at levels accessible to the high-luminosity LHC, can imply a phenomenological no-lose theorem for the next generation of collider facilities. Correlating Higgs coupling deviations from the SM expectation in the gauge boson sector with high-scale unitarity requirements, we estimate and compare the sensitivity that can be expected at a future hadron collider (operating at 100 TeV centre-of-mass energy) and a 10 TeV muon collider. Both muon and hadron colliders offer discovery potential for mass scales up to where unitarity violation induced by (sub)percent Higgs coupling modifications is mended. We comment on how an intermediate precision FCC-ee programme can corroborate such deviations.
Paper Structure (8 sections, 6 equations, 4 figures)

This paper contains 8 sections, 6 equations, 4 figures.

Figures (4)

  • Figure 1: Feynman diagram contributions to the $s$ channel of $WW\to WW$ scattering (suppressing $t$ topologies). Similar diagrams exist for $WZ$ scattering with $W$ resonances appearing as $s$ and $t$ channel contributions.
  • Figure 2: Sensitivity of resonance searches in the $WW$ and $ZZ$ weak boson fusion production modes when considering scalar unitarity restoration for $\mu_H<1$. We show two scenarios for comparison related to the width of the (assumed narrow) resonance (a) $\Gamma_{H'}/m_{H'}=10\%$ and (b) $\Gamma_{H'}/m_{H'}=2.5\%$; overlaid on the significance plot is the signal strength that such parameter choices will probe. The magenta lines include the expected improvements from accessing semi-leptonic channels (FCC-hh efficiencies are provided at the end of Sec. \ref{['sec:ana']}, we comment on more conservative current LHC efficiencies in the text).
  • Figure 3: Sensitivity of a WBF search of unitarity-restoring vector resonances. Shown are (a) the $Z'$ search and (b) the $W'$ search for two choices of Higgs signal strengths $\mu_H=0.95,0.99$. A significant coupling modification leads to a large signal at an FCC-hh, which decreases more quickly as it approaches the SM, since the kinematic endpoint of the FCC-hh is probed with lower statistical yield compared to the muon collider. The magenta lines include the expected improvements from accessing semi-leptonic channels.
  • Figure 4: Sensitivity for wide fermion-aware resonances. The magenta line includes semi-leptonic channels using the FCC-hh extrapolation of efficiencies given in the text.