002750649 001__ 2750649
002750649 003__ SzGeCERN
002750649 005__ 20221117153234.0
002750649 0247_ $$2DOI$$9IOP$$a10.1088/1742-6596/1690/1/012148
002750649 0248_ $$aoai:inspirehep.net:1838722$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT$$pcerncds:CERN$$qINSPIRE:HEP$$qForCDS
002750649 035__ $$9http://old.inspirehep.net/oai2d$$aoai:inspirehep.net:1838722$$d2021-01-29T11:02:24Z$$h2021-01-30T05:00:08Z$$mmarcxml
002750649 035__ $$9Inspire$$a1838722
002750649 041__ $$aeng
002750649 100__ $$aIvanov, Kirill$$uMoscow, MIPT
002750649 245__ $$9IOP$$aStudies of excited states of beauty hadrons at CMS
002750649 260__ $$c2020
002750649 300__ $$a7 p
002750649 520__ $$9IOP$$aStudies of excited states of beauty mesons and baryons, performed at the CMS Experiment, are presented. The first observation of $B\tfrac{+}{c}$ (2S) and $B\tfrac{*+}{c}$ (2S) states in the $B\tfrac{+}{c}{\pi }^{+}{\pi }^{-}$ invariant mass spectrum is reported as well as the study of excited Λb(5912)0, Λb(5920)0, Λb(6146)0 and Λb(6152)0 baryons decaying to ${\Lambda }\tfrac{0}{b}{\pi }^{+}{\pi }^{-}$.The analyses use Run-2 data collected in pp collisions at $\sqrt{s}$ = 13 TeV.
002750649 540__ $$aCC-BY-3.0$$bIOP$$uhttp://creativecommons.org/licenses/by/3.0
002750649 595__ $$aFor annual report
002750649 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002750649 693__ $$aCERN LHC$$eCMS
002750649 690C_ $$aCERN
002750649 690C_ $$aARTICLE
002750649 710__ $$gCMS Collaboration
002750649 773__ $$01838300$$c012148$$n1$$pJ. Phys.: Conf. Ser.$$v1690$$wC20-10-05$$y2020
002750649 8564_ $$82275864$$s822785$$uhttps://cds.cern.ch/record/2750649/files/Ivanov_2020_J._Phys.__Conf._Ser._1690_012148.pdf$$yFulltext
002750649 960__ $$a13
002750649 962__ $$b2718781$$k012148$$nmoscow20201005
002750649 980__ $$aARTICLE
002750649 980__ $$aConferencePaper