# Search results for: F. Ambrogi

Journal of High Energy Physics > 2019 > 2019 > 2 > 1-42

^{−1}from proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV collected...

Journal of High Energy Physics > 2019 > 2019 > 2 > 1-110

^{−1}. The differential...

Journal of High Energy Physics > 2019 > 2019 > 2 > 1-48

*.*9 fb

^{−1}. No deviations from the predictions of the standard model are observed. The results are interpreted...

The European Physical Journal C > 2019 > 79 > 2 > 1-49

The European Physical Journal C > 2019 > 79 > 2 > 1-27

The European Physical Journal C > 2019 > 79 > 2 > 1-29

Journal of High Energy Physics > 2019 > 2019 > 1 > 1-51

*.*9 fb

^{−1}. The cross sections are measured in a fiducial phase space...

Journal of High Energy Physics > 2019 > 2019 > 1 > 1-39

^{−1}of proton-proton collisions at s = 13 $$ \sqrt{s} = 13 $$ TeV, produced by the LHC and collected with the CMS detector in 2016. Theoretical models...

Journal of High Energy Physics > 2019 > 2019 > 1 > 1-55

The European Physical Journal C > 2019 > 79 > 1 > 1-28

Journal of High Energy Physics > 2019 > 2019 > 1 > 1-42

Journal of High Energy Physics > 2019 > 2019 > 1 > 1-45

^{−1}. The final state consists of two b quark-antiquark pairs. The search is conducted in the region of phase space where one...

Journal of High Energy Physics > 2018 > 2018 > 12 > 1-42

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-60

*γγ*decay channel are reported. The analysis is based on data collected by the CMS experiment in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV during the 2016 LHC running period, corresponding to an integrated luminosity of 35.9 fb

^{−1}. Allowing the Higgs mass to float, the measurement yields a signal strength relative to...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-47

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-37

^{−1}, respectively. The search...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-64

*τ*lepton pair. Both hadronic and leptonic decay modes are considered for the

*τ*leptons. Scenarios involving the direct pair production of

*τ*sleptons, or their indirect production via the decays of charginos and neutralinos,...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-42

*γ*→

*ℓℓγ*,

*ℓ*= e or

*μ*), or to two photons, one of which has an internal conversion into a muon pair (H →

*γ*

^{*}

*γ*→

*μμγ*) were considered. The analysis is performed using a data set recorded by the CMS experiment at the LHC from proton-proton collisions...

The European Physical Journal C > 2018 > 78 > 11 > 1-41

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-38

^{−1}of pp collision data at s = 8 $$ \sqrt{s}=8 $$ TeV. The production mechanism investigated in this search is t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ pair production in which one top quark...