% IMPORTANT: The following is UTF-8 encoded. This means that in the presence % of non-ASCII characters, it will not work with BibTeX 0.99 or older. % Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or % “biber”. @ARTICLE{Aaij:474152, author = {Aaij, Roel and others}, collaboration = {{LHCb Collaboration}}, title = {{S}tudy of ${B}^0_s \to {J}\psi \pi^+\pi^-{K}^+{K}^-$ decays}, journal = {Journal of high energy physics}, volume = {04}, number = {2}, issn = {1029-8479}, address = {[Trieste]}, publisher = {SISSA}, reportid = {PUBDB-2022-00542, arXiv:2011.01867. LHCb-PAPER-2020-35. CERN-EP-2020-192}, pages = {024}, year = {2021}, note = {JHEP 02 (2021) 024. All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2020-035.html (LHCb public pages)'}, abstract = {The decays $ {\mathrm{B}}_{\mathrm{s}}^0 $ → J/ψπ$^{+}$π$^{−}$K$^{+}$K$^{−}$ are studied using a data set corresponding to an integrated luminosity of 9 fb$^{−1}$, collected with the LHCb detector in proton-proton collisions at centre-of-mass energies of 7, 8 and 13 TeV. The decays $ {\mathrm{B}}_{\mathrm{s}}^0 $ → $ \mathrm{J}/{\psi \mathrm{K}}^{\ast 0}{\overline{\mathrm{K}}}^{\ast 0} $ and $ {\mathrm{B}}_{\mathrm{s}}^0 $ → χ$_{c1}$(3872)K$^{+}$K$^{−}$, where the K$^{+}$K$^{−}$pair does not originate from a ϕ meson, are observed for the first time. Precise measurements of the ratios of branching fractions between intermediate χ$_{c1}$(3872)ϕ, $ \mathrm{J}/{\psi \mathrm{K}}^{\ast 0}{\overline{\mathrm{K}}}^{\ast 0} $, ψ(2S)ϕ and χ$_{c1}$(3872)K$^{+}$K$^{−}$ states are reported. A structure, denoted as X(4740), is observed in the J/ψϕ mass spectrum and, assuming a Breit-Wigner parameterisation, its mass and width are determined to be$ {\displaystyle \begin{array}{c}{m}_{\mathrm{X}(4740)}=4741\pm 6\pm 6\kern0.5em \mathrm{MeV}/{c}^2,\\ {}{\Gamma}_{\mathrm{X}(4740)}=53\pm 15\pm 11\kern0.5em \mathrm{MeV},\end{array}} $where the first uncertainty is statistical and the second is systematic. In addition, the most precise single measurement of the mass of the $ {\mathrm{B}}_{\mathrm{s}}^0 $ meson is performed and gives a value of$ {m}_{{\mathrm{B}}_{\mathrm{s}}^0}=5366.98\pm 0.07\pm 0.13\kern0.5em \mathrm{MeV}/{c}^2. $}, keywords = {p p: colliding beams (INSPIRE) / branching ratio: ratio: measured (INSPIRE) / B/s0: branching ratio (INSPIRE) / p p: scattering (INSPIRE) / B/s0: hadronic decay (INSPIRE) / B/s0: decay modes (INSPIRE) / J/psi(3100) (INSPIRE) / parametrization (INSPIRE) / mass spectrum: (J/psi(3100) Phi(1020)) (INSPIRE) / Breit-Wigner (INSPIRE) / mass: width (INSPIRE) / intermediate state (INSPIRE) / statistical (INSPIRE) / psi(3685) (INSPIRE) / X(3872) (INSPIRE) / B/s0: mass: measured (INSPIRE) / structure (INSPIRE) / LHC-B (INSPIRE) / CERN LHC Coll (INSPIRE) / experimental results (INSPIRE) / B/s0 --> J/psi(3100) pi+ pi- K+ K- (INSPIRE) / B/s0 --> J/psi(3100) 2K*(892)0 (INSPIRE) / B/s0 --> X(3872) K+ K- (INSPIRE) / 7000 GeV-cms (INSPIRE) / 8000 GeV-cms (INSPIRE) / 13000 GeV-cms (INSPIRE) / B physics (autogen) / Branching fraction (autogen) / Hadron-Hadron scattering (experiments) (autogen) / Quarkonium (autogen) / Spectroscopy (autogen)}, cin = {IT}, ddc = {530}, cid = {I:(DE-H253)IT-20120731}, pnm = {6G9 - IDAF (DESY) (POF4-6G9)}, pid = {G:(DE-HGF)POF4-6G9}, experiment = {EXP:(DE-H253)TIER-II-20150101}, typ = {PUB:(DE-HGF)16}, eprint = {2011.01867}, howpublished = {arXiv:2011.01867}, archivePrefix = {arXiv}, SLACcitation = {$\%\%CITATION$ = $arXiv:2011.01867;\%\%$}, UT = {WOS:000614815700001}, doi = {10.1007/JHEP02(2021)024}, url = {https://bib-pubdb1.desy.de/record/474152}, }