Journal
JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 4, Pages -Publisher
SPRINGER
DOI: 10.1007/JHEP04(2021)154
Keywords
Beyond Standard Model; Higgs Physics
Categories
Funding
- Swiss National Science Foundation [PP00P2176884]
- MIUR [2017FMJFMW]
- Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy [EXC 2121, 390833306]
- International Helmholtz-Weizmann Research School for Multimessenger Astronomy through the Initiative and Networking Fund of the Helmholtz Association
- ERC Starting Grant NewAve [638528]
- National Science Foundation [PHY-160761]
- European Research Council (ERC) [638528] Funding Source: European Research Council (ERC)
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The FCC-hh hadron collider will provide access to clean final states, with the Zh production channel showing sensitivity to various SMEFT operators. While O-phi q((3)) shows the best sensitivity, binning in Zh rapidity can improve sensitivity to O-phi q((1)). Estimated bounds at FCC-hh are significantly better than those at HL-LHC and future lepton colliders.
The future 100 TeV FCC-hh hadron collider will give access to rare but clean final states which are out of reach of the HL-LHC. One such process is the Zh production channel in the (nu(nu) over bar /l(+)l(-) )gamma gamma final states. We study the sensitivity of this channel to the O-phi q((1)), O-phi q((3)), O-phi u and O-phi d SMEFT operators, which parametrize deviations of the W and Z couplings to quarks, or, equivalently, anomalous trilinear gauge couplings (aTGC). While our analysis shows that good sensitivity is only achievable for O-phi q((3)), we demonstrate that binning in the Zh rapidity has the potential to improve the reach on O-phi q((1)). Our estimated bounds are one order of magnitude better than projections at HL-LHC and is better than global fits at future lepton colliders. The sensitivity to O-phi q((3)) is competitive with other channels that could probe the same operator at FCC-hh. Therefore, combining the different diboson channels sizeably improves the bound on O-phi q((3)), reaching a precision of |delta g(1z)| less than or similar to 2 x 10(-4) on the deviations in the ZWW interactions.
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