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Reis, Thomas/0000-0003-3703-6624; Shchedrolosiev, Mykyta/0000-0003-3510-2093; Das, Pallabi/0000-0002-9770-1377; Giacomelli, Paolo/0000-0002-6368-7220; Sharma, Vivek/0000-0003-1736-8795; Melo Da Costa, Eliza/0000-0002-5016-6434; Palencia Cortezon, Jose Enrique/0000-0001-8264-0287; Heath, Helen/0000-0001-6576-9740; Goldouzian, Reza/0000-0002-0295-249X; Faltermann, Nils/0000-0001-6506-3107; Singh, Jasbir/0000-0001-9029-2462; Gadallah, Mahmoud Moussa Abdelkhalek/0000-0002-8305-6661; Donega, Mauro/0000-0001-9830-0412; Redondo, Ignacio/0000-0003-3737-4121; Dallavalle, Gaetano Marco/0000-0002-8614-0420; Gonzalez Fernandez, Juan Rodrigo/0000-0002-4825-8188; Chatterjee, Suman/0000-0003-2660-0349; Botta, Cristina/0000-0002-8072-795X; Mitra, Soureek/0000-0002-3060-2278; Jabeen, Shabnam/0000-0002-0155-7383; Escalante Del Valle, Alberto/0000-0002-9702-6359; Feld, Lutz/0000-0001-9813-8646; Meuser, Danilo/0000-0002-2722-7526Energy correlators that describe energy-weighted distances between two or three particles in a hadronic jet are measured using an event sample of root s = 13 TeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3 fb(-1). The measured distributions are consistent with the trends in the simulation that reveal two key features of the strong interaction: confinement and asymptotic freedom. By comparing the ratio of the measured three- and two-particle energy correlator distributions with theoretical calculations that resum collinear emissions at approximate next-to-next-to-leading-logarithmic accuracy matched to a next-to-leading-order calculation, the strong coupling is determined at the Z boson mass: alpha(S)(m(Z)) = 0.1229(-0.0050)(+0.0040), the most precise alpha(S)(m(Z)) value obtained using jet substructure observables.eninfo:eu-repo/semantics/openAccessArticleQ1Q11337WOS:001382521700002392135831