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dc.contributor.authorAaij, R.
dc.contributor.authorBeteta, C. A
dc.contributor.authorAckernley, T.
dc.contributor.authorAdeva, B.
dc.contributor.authorAdinolfi, M.
dc.contributor.authorAfsharnia, H.
dc.contributor.authorAidala, C. A
dc.contributor.authorAiola, S.
dc.contributor.authorAjaltouni, Z.
dc.contributor.authorAkar, S.
dc.contributor.authorAlbicocco, P.
dc.contributor.authorAlbrecht, J.
dc.contributor.authorAlessio, F.
dc.contributor.authorAlexander, M.
dc.contributor.authorAlbero, A. A
dc.contributor.authorAlkhazov, G.
dc.contributor.authorCartelle, P. A
dc.contributor.authorJr, A. A A
dc.contributor.authorAmato, S.
dc.contributor.authorAmhis, Y.
dc.date.accessioned2021-09-20T17:29:00Z
dc.date.available2021-09-20T17:29:00Z
dc.date.issued2019-08-22
dc.identifier.urihttps://hdl.handle.net/1721.1/131617
dc.description.abstractAbstract The decay-time-dependent $$CP$$ CP asymmetry in $${{B} ^0_{s}} \rightarrow J/\psi {{K} ^+} {{K} ^-} $$ B s 0 → J / ψ K + K - decays is measured using proton–proton collision data, corresponding to an integrated luminosity of $$1.9\,\mathrm{fb}^{-1} $$ 1.9 fb - 1 , collected with the LHCb detector at a centre-of-mass energy of $$13\,\mathrm {TeV}$$ 13 TeV in 2015 and 2016. Using a sample of approximately 117 000 signal decays with an invariant $${{K} ^+} {{K} ^-} $$ K + K - mass in the vicinity of the $$\phi (1020)$$ ϕ ( 1020 ) resonance, the $$CP$$ CP -violating phase $$\phi _s$$ ϕ s is measured, along with the difference in decay widths of the light and heavy mass eigenstates of the $${{B} ^0_{s}} $$ B s 0 - $${{\overline{B}{}} {}^0_{s}} $$ B ¯ s 0 system, $$\Delta \Gamma _s$$ Δ Γ s . The difference of the average $${{B} ^0_{s}} $$ B s 0 and $${{B} ^0} $$ B 0 meson decay widths, $$\Gamma _s-\Gamma _d$$ Γ s - Γ d , is determined using in addition a sample of $${{B} ^0} \rightarrow J/\psi {{K} ^+} {{\pi } ^-} $$ B 0 → J / ψ K + π - decays. The values obtained are $$\phi _s = -0.083\pm 0.041\pm 0.006\mathrm { \,rad} $$ ϕ s = - 0.083 ± 0.041 ± 0.006 rad , $$\Delta \Gamma _s = 0.077 \pm 0.008 \pm 0.003 {\mathrm { \,ps^{-1}}} $$ Δ Γ s = 0.077 ± 0.008 ± 0.003 ps - 1 and $$\Gamma _s-\Gamma _d = -0.0041 \pm 0.0024 \pm 0.0015{\mathrm { \,ps^{-1}}} $$ Γ s - Γ d = - 0.0041 ± 0.0024 ± 0.0015 ps - 1 , where the first uncertainty is statistical and the second systematic. These are the most precise single measurements of these quantities to date and are consistent with expectations based on the Standard Model and with a previous LHCb analysis of this decay using data recorded at centre-of-mass energies 7 and 8 TeV. Finally, the results are combined with recent results from $${{B} ^0_{s}} \rightarrow J/\psi {{\pi } ^+} {{\pi } ^-} $$ B s 0 → J / ψ π + π - decays obtained using the same dataset as this analysis, and with previous independent LHCb results.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1140/epjc/s10052-019-7159-8en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleUpdated measurement of time-dependent $$CP$$ CP -violating observables in $${{B} ^0_{s}} \rightarrow J/\psi K^+ K^-$$ B s 0 → J / ψ K + K - decaysen_US
dc.typeArticleen_US
dc.identifier.citationThe European Physical Journal C. 2019 Aug 22;79(8):706en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.identifier.mitlicensePUBLISHER_CC
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2020-06-26T12:42:32Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2020-06-26T12:42:32Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Needed


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