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Observation of the $\chi_\mathrm{b1}$(3P) and $\chi_\mathrm{b2}$(3P) and measurement of their masses
dc.contributor.author | CMS collaboration (2300 authors) | |
dc.contributor.author | Nayak, Aruna | |
dc.contributor.author | Araujo, Mariana | |
dc.contributor.author | Bargassa, Pedrame | |
dc.contributor.author | Beirão Da Cruz E Silva, Cristóvão | |
dc.contributor.author | Di Francesco, Agostino | |
dc.contributor.author | Faccioli, Pietro | |
dc.contributor.author | Galinhas, Bruno | |
dc.contributor.author | Gallinaro, Michele | |
dc.contributor.author | Hollar, Jonathan | |
dc.contributor.author | Leonardo, Nuno | |
dc.contributor.author | Seixas, Joao | |
dc.contributor.author | Strong, Giles | |
dc.contributor.author | Toldaiev, Oleksii | |
dc.contributor.author | Vadruccio, Daniele | |
dc.contributor.author | Varela, Joao | |
dc.contributor.author | Vischia, Pietro | |
dc.contributor.author | David Tinoco Mendes, Andre | |
dc.contributor.author | Silva, Pedro | |
dc.contributor.author | Musella, Pasquale | |
dc.date.accessioned | 2019-02-05T16:26:28Z | |
dc.date.available | 2019-02-05T16:26:28Z | |
dc.date.issued | 2018-08-29 | |
dc.date.updated | 2019-02-05T16:26:28Z | |
dc.description.abstract | The $\chi_\mathrm{b1}$(3P) and $\chi_\mathrm{b2}$(3P) states are observed through their $\Upsilon$(3S) $\gamma$ decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 80.0 fb$^{-1}$. The $\Upsilon$(3S) mesons are identified through their dimuon decay channel, while the low-energy photons are detected after converting to e$^+$e$^-$ pairs in the silicon tracker, leading to a $\chi_\mathrm{b}$(3P) mass resolution of 2.2 MeV. This is the first time that the $J =$ 1 and 2 states are well resolved and their masses individually measured: 10$\,$513.42 $\pm$ 0.41 (stat) $\pm$ 0.18 (syst) MeV and 10$\,$524.02 $\pm$ 0.57 (stat) $\pm$ 0.18 (syst) MeV; they are determined with respect to the world-average value of the $\Upsilon$(3S) mass, which has an uncertainty of 0.5 MeV. The mass splitting is measured to be 10.60 $\pm$ 0.64 (stat) $\pm$ 0.17 (syst) MeV. | |
dc.description.version | Peer Reviewed | |
dc.identifier | Phys.Rev.Lett. 121 (2018) 092002; DOI 10.1103/PhysRevLett.121.092002 | |
dc.identifier.uri | http://dx.doi.org/10.1103/PhysRevLett.121.092002 | |
dc.identifier.uri | http://hdl.handle.net/10400.26/27648 | |
dc.language.iso | eng | |
dc.title | Observation of the $\chi_\mathrm{b1}$(3P) and $\chi_\mathrm{b2}$(3P) and measurement of their masses | |
dc.type | journal article | |
dspace.entity.type | Publication | |
rcaap.rights | openAccess | pt |
rcaap.type | article |
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