Hayrapetyan, A.Tumasyan, A.Adam, W.Andrejkovic, J. W.Bergauer, T.Chatterjee, S.Damanakis, K.2026-04-252026-04-2520252470-00102470-0029https://doi.org/10.1103/PhysRevD.111.092014https://hdl.handle.net/11486/8424A measurement of the Higgs boson mass and width via its decay to two Z bosons is presented. Proton-proton collision data collected by the CMS experiment, corresponding to an integrated luminosity of 138 fb(-1) at a center-of-mass energy of 13 TeV, is used. The invariant mass distribution of four leptons in the on-shell Higgs boson decay is used to measure its mass and constrain its width. This yields the most precise single measurement of the Higgs boson mass to date, 125.04 +/- 0.12 GeV, and an upper limit on the width Gamma(H) < 330 MeV at 95% confidence level. A combination of the on- and off-shell Higgs boson production decaying to four leptons is used to determine the Higgs boson width, assuming that no new virtual particles affect the production, a premise that is tested by adding new heavy particles in the gluon fusion loop model. This result is combined with a previous CMS analysis of the off-shell Higgs boson production with decay to two leptons and two neutrinos, giving a measured Higgs boson width of 3.0(-1.5)(+2.0) MeV, in agreement with the standard model prediction of 4.1 MeV. The strength of the off-shell Higgs boson production is also reported. The scenario of no off-shell Higgs boson production is excluded at a confidence level corresponding to 3.8 standard deviations.eninfo:eu-repo/semantics/openAccess#BAŞV!Measurement of the Higgs boson mass and width using the four-lepton final state in proton-proton collisions at √s=13 TeVArticle111910.1103/PhysRevD.111.0920142-s2.0-105027237446Q1WOS:001511668600001Q10000-0001-8448-883X0000-0003-2752-11830000-0002-2633-67120000-0003-3632-02870000-0002-9404-59330000-0002-0711-63190000-0003-0320-4407