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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorTumasyan, A.en_US
dc.contributor.authorALPANA, K.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorKANSAL, B.en_US
dc.contributor.authorLAHA, A.en_US
dc.contributor.authorPANDEY, S.en_US
dc.contributor.authorRASTOGI, A.en_US
dc.contributor.authorSHARMA, SEEMA et al.en_US
dc.date.accessioned2022-09-23T11:18:21Z
dc.date.available2022-09-23T11:18:21Z
dc.date.issued2022-05en_US
dc.identifier.citationEuropean Physical Journal C, 82(5), 499.en_US
dc.identifier.issn1434-6044en_US
dc.identifier.issn1434-6052en_US
dc.identifier.urihttps://doi.org/10.1140/epjc/s10052-022-10315-yen_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/7374
dc.description.abstractUsing a data sample of s√=13TeVs=13TeV proton-proton collisions collected by the CMS experiment at the LHC in 2017 and 2018 with an integrated luminosity of 103~fb−1103~fb−1, the B0s→ψ(2S)K0SBs0→ψ(2S)KS0 and B0→ψ(2S)K0Sπ+π−B0→ψ(2S)KS0π+π− decays are observed with significances exceeding 5 standard deviations. The resulting branching fraction ratios, measured for the first time, correspond to B(B0s→ψ(2S)K0S)/B(B0→ψ(2S)K0S)=(3.33±0.69(stat)±0.11(syst)±0.34(fs/fd))×10−2B(Bs0→ψ(2S)KS0)/B(B0→ψ(2S)KS0)=(3.33±0.69(stat)±0.11(syst) ±0.34(fs/fd))×10−2 and B(B0→ψ(2S)K0Sπ+π−)/B(B0→ψ(2S)K0S)=0.480±0.013(stat ±0.032(syst)B(B0→ψ(2S)KS0π+π−)/B(B0→ψ(2S)KS0)=0.480±0.013(stat)±0.032(syst), where the last uncertainty in the first ratio is related to the uncertainty in the ratio of production cross sections of B0sBs0 and B0B0 mesons, fs/fdfs/fd.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subjectPhysicsen_US
dc.subject2022-SEP-WEEK3en_US
dc.subjectTOC-SEP-2022en_US
dc.subject2022en_US
dc.titleObservation of B00 →→ ψψ(2S)K0Sπ+π−S0π+π− and B0ss0 →→ ψψ(2S)K0SS0 decaysen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleEuropean Physical Journal Cen_US
dc.publication.originofpublisherForeignen_US
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