AION/Magis

Abstract:

A combination of measurements sensitive to anomalous quartic electroweak gauge boson couplings is presented using proton–proton collision data collected by the ATLAS detector at s = 13 TeV at the LHC. Contributing analyses include measurements of vector-boson scattering in numerous final states as well as a tri-boson measurement. The combined measurement is used to constrain anomalous electroweak boson quartic self-couplings that result from dimension-8 operators in the Éboli model using an effective field theory. Results are presented as 68% and 95% confidence level intervals parameterised by one or two Wilson coefficients, both with and without unitarity constraints applied. Theoretical bounds from unitarity and positivity are overlaid where relevant. Confidence intervals obtained from simultaneous profiled fits to all Wilson coefficients are also presented.

Abstract:

A search for resonant structures in the $J/\psi +\psi (2\mathrm{S})$ mass spectrum is performed using proton-proton collision data at $\sqrt{s}=13\mathrm{TeV}$ , corresponding to an integrated luminosity of $140{\mathrm{fb}}^{-1}$ , recorded by the ATLAS experiment at the LHC. The decay channels of $J/\psi +\psi (2\mathrm{S})\to 4\mu$ and $J/\psi +\psi (2\mathrm{S})\to 4\mu +2\pi$ are analyzed. An excess near 6.9 GeV is observed in both channels with a combined significance of $8.9\sigma$ . No significant signal is observed near 7.2 GeV, and an upper limit on its yield relative to $X(6900)$ is provided. A simultaneous fit with the di- $J/\psi$ channel is carried out under assumptions regarding the resonance interferences, yielding a ratio of the partial decay widths between the $J/\psi +\psi (2\mathrm{S})$ and di- $J/\psi$ channels of $1.08\pm 0.20_{-0.17}^{+0.40}$ for the resonance near 6.9 GeV.

Abstract:

Abstract A search for a pair of low-mass pseudoscalars a that promptly decay into τ -leptons is presented using 140 fb − 1 of proton–proton collision data at 13 TeV centre-of-mass energy recorded with the ATLAS detector at the Large Hadron Collider. The result is used to place constraints on exotic decays of the Higgs boson into four τ -leptons, H → a a → τ + τ − τ + τ − . This search focuses on events with either one or two τ -leptons decaying into hadrons and neutrinos, and the remaining three or two τ -leptons decaying into either electron or muon and neutrinos. No significant excess is observed above the expected Standard Model background and upper limits at the 95% confidence level on B ( H → a a → τ + τ − τ + τ − ) are set ranging from 0.06 to 0.23, depending on the mass m a ranging from 15 to 60 GeV.

Abstract:

The production of single top quarks and top antiquarks via the t-channel exchange of a virtual W boson is measured in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider. The full Run 2 data sample recorded with the ATLAS detector in the years 2015–2018 is used, corresponding to an integrated luminosity of 140 fb−1. The absolute and normalised production cross-sections are measured differentially as a function of the transverse momentum and absolute rapidity of the top quark and top antiquark. In addition, the ratio of top quark to top antiquark production cross-sections is measured. The measured distributions are compared with next-to-leading-order quantum chromodynamics predictions obtained with different combinations of matrix-element generators, parton-shower programs and proton parton distribution functions, as well as to next-to-next-to-leading-order calculations. Overall, good agreement is observed between the measurements and the theoretical predictions. For most measured distributions, the sensitivity to differences between the predictions is limited by the systematic uncertainties in the measurement. The measured differential distributions are also interpreted in an effective field theory approach to constrain the Wilson-Coefficient CQq3, 1 associated with a four-quark operator. The interpretation accounts for the effect of the selection efficiency, which is altered significantly by non-zero contributions from CQq3, 1.