37 research outputs found

    Search for the doubly heavy baryon Ξbc+\it{\Xi}_{bc}^{+} decaying to J/ψΞc+J/\it{\psi} \it{\Xi}_{c}^{+}

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    A first search for the Ξbc+→J/ψΞc+\it{\Xi}_{bc}^{+}\to J/\it{\psi}\it{\Xi}_{c}^{+} decay is performed by the LHCb experiment with a data sample of proton-proton collisions, corresponding to an integrated luminosity of 9 fb−19\,\mathrm{fb}^{-1} recorded at centre-of-mass energies of 7, 8, and 13 TeV13\mathrm{\,Te\kern -0.1em V}. Two peaking structures are seen with a local (global) significance of 4.3 (2.8)4.3\,(2.8) and 4.1 (2.4)4.1\,(2.4) standard deviations at masses of 6571 MeV ⁣/c26571\,\mathrm{Me\kern -0.1em V\!/}c^2 and 6694 MeV ⁣/c26694\,\mathrm{Me\kern -0.1em V\!/}c^2, respectively. Upper limits are set on the Ξbc+\it{\Xi}_{bc}^{+} baryon production cross-section times the branching fraction relative to that of the Bc+→J/ψDs+B_{c}^{+}\to J/\it{\psi} D_{s}^{+} decay at centre-of-mass energies of 8 and 13 TeV13\mathrm{\,Te\kern -0.1em V}, in the Ξbc+\it{\Xi}_{bc}^{+} and in the Bc+B_{c}^{+} rapidity and transverse-momentum ranges from 2.0 to 4.5 and 0 to 20 GeV ⁣/c20\,\mathrm{Ge\kern -0.1em V\!/}c, respectively. Upper limits are presented as a function of the Ξbc+\it{\Xi}_{bc}^{+} mass and lifetime.Comment: All figures and tables, along with machine-readable versions and any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-005.html (LHCb public pages

    First observation of a doubly charged tetraquark and its neutral partner

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    A combined amplitude analysis is performed for the decays B0→D‟0Ds+π−B^0 \rightarrow \overline{D}^0 D^+_s\pi^- and B+→D−Ds+π+B^+\rightarrow D^- D^+_s\pi^+, which are related by isospin symmetry. The analysis is based on data collected by the LHCb detector in proton-proton collisions at center-of-mass energies of 7, 8 and 13 TeV\,\rm{TeV}. The full data sample corresponds to an integrated luminosity of 9 fb−1\,\rm{fb^{-1}}. Two new resonant states with masses of 2.908±0.011±0.020 GeV2.908\pm0.011\pm0.020\,\rm{GeV} and widths of 0.136±0.023±0.011 GeV0.136\pm0.023\pm0.011\,\rm{GeV} are observed, which decay to Ds+π+D^+_s\pi^+ and Ds+π−D^+_s\pi^- respectively. The former state indicates the first observation of a doubly charged open-charm tetraquark state with minimal quark content [csˉudˉ][c\bar{s}u\bar{d}], and the latter state is a neutral tetraquark composed of [csˉuˉd][c\bar{s}\bar{u}d] quarks. Both states are found to have spin-parity 0+0^+, and their resonant parameters are consistent with each other, which suggests that they belong to an isospin triplet.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-026.html (LHCb public pages

    Amplitude analysis of B0→D‟0Ds+π−B^0 \rightarrow \overline{D}^0 D_s^+ \pi^- and B+→D−Ds+π+B^+ \rightarrow D^- D_s^+ \pi^+ decays

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    Resonant contributions in B0→D‟0Ds+π−B^0 \rightarrow \overline{D}^0 D^+_s\pi^- and B+→D−Ds+π+B^+\rightarrow D^- D^+_s\pi^+ decays are determined with an amplitude analysis, which is performed both separately and simultaneously, where in the latter case isospin symmetry between the decays is assumed. The analysis is based on data collected by the LHCb detector in proton-proton collisions at center-of-mass energies of 7, 8 and 13 TeV\rm{TeV}. The full data sample corresponds to an integrated luminosity of 9 fb−1\rm fb^{-1}. A doubly charged spin-0 open-charm tetraquark candidate together with a neutral partner, both with masses near 2.9 GeV2.9\,\rm{GeV}, are observed in the DsπD_s\pi decay channel.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-027.html (LHCb public pages

    Search for time-dependent CP violation in D-0 -> K+K- and D-0 -> pi(+)pi(-) decays

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    A search for time-dependent violation of the charge-parity symmetry in D0→K+K−D^0 \to K^+ K^- and D0→π+π−D^0 \to \pi^+ \pi^- decays is performed at the LHCb experiment using proton-proton collision data recorded from 2015 to 2018 at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 6 fb−1^{-1}. The D0D^0 meson is required to originate from a D∗(2010)+→D0π+D^*(2010)^+ \to D^0 \pi^+ decay, such that its flavour at production is identified by the charge of the accompanying pion. The slope of the time-dependent asymmetry of the decay rates of D0D^0 and Dˉ0\bar{D}^0 mesons into the final states under consideration is measured to be ΔYK+K−=(−2.3±1.5±0.3)×10−4\Delta Y_{K^+ K^-} = (-2.3 \pm 1.5 \pm 0.3) \times 10^{-4}, ΔYπ+π−=(−4.0±2.8±0.4)×10−4\Delta Y_{\pi^+ \pi^-} = (-4.0 \pm 2.8 \pm 0.4)\times 10^{-4}, where the first uncertainties are statistical and the second are systematic. These results are compatible with the conservation of the charge-parity symmetry at the level of 2 standard deviations and improve the precision by nearly a factor of two.Comment: Updated to match published version; all figures and tables, along with supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2020-045.htm

    Evidence of a J/psi Lambda structure and observation of excited Xi(-) states in the Xi(-)(b) -> J/psi Lambda K- decay

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    First evidence of a structure in the J/ψΛJ/\psi \varLambda invariant mass distribution is obtained from an amplitude analysis of Ξb−→J/ψΛK−\varXi_b^- \to J/\psi \varLambda K^- decays. The observed structure is consistent with being due to a charmonium pentaquark with strangeness. Its mass and width are determined to be 4458.8\pm2.9\,^{+4.7}_{-1.1}MeV and 17.3\pm6.5\,^{+8.0}_{-5.7}MeV, where the quoted uncertainties are statistical and systematic, respectively. The structure is also consistent with being due to two resonances. In addition, the narrow excited Ξ−\varXi^- states, Ξ(1690)−\varXi(1690)^- and Ξ(1820)−\varXi(1820)^-, are seen for the first time in a Ξb−\varXi_b^- decay, and their masses and widths are measured with improved precision. The analysis is performed using pppp collision data corresponding to a total integrated luminosity of 9fb−1^{-1}, collected with the LHCb experiment at centre-of-mass energies of 77, 88 and 1313TeV.Comment: All figures and tables, along with machine-readable versions and any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2020-039.html (LHCb public pages

    Searches for rare B-s(0) and B-0 decays into four muons

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    Searches for rare Bs0B_s^0 and B0B^0 decays into four muons are performed using proton-proton collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 9 fb−1\text{fb}^{-1}. Direct decays and decays via light scalar and J/ψJ/\psi resonances are considered. No evidence for the six decays searched for is found and upper limits at the 95% confidence level on their branching fractions ranging between 1.8×10−101.8\times10^{-10} and 2.6×10−92.6\times10^{-9} are set

    Search for the doubly charmed baryon Ξ cc + in the Ξ c + π − π + final state

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    Abstract: A search for the doubly charmed baryon Ξcc+ is performed in the Ξc+π−π+ invariant-mass spectrum, where the Ξc+ baryon is reconstructed in the pK−π+ final state. The study uses proton-proton collision data collected with the LHCb detector at a centre- of-mass energy of 13 TeV, corresponding to a total integrated luminosity of 5.4 fb−1. No significant signal is observed in the invariant-mass range of 3.4–3.8 GeV/c2. Upper limits are set on the ratio of branching fractions multiplied by the production cross-section with respect to the Ξcc++→ (Ξc+→ pK−π+)π+ decay for different Ξcc+ mass and lifetime hypotheses in the rapidity range from 2.0 to 4.5 and the transverse momentum range from 2.5 to 25 GeV/c. The results from this search are combined with a previously published search for the Ξcc+→Λc+K−π+ decay mode, yielding a maximum local significance of 4.0 standard deviations around the mass of 3620 MeV/c2, including systematic uncertainties. Taking into account the look-elsewhere effect in the 3.5–3.7 GeV/c2 mass window, the combined global significance is 2.9 standard deviations including systematic uncertainties

    Measurement of forward W and Z boson production in pppp collisions at s=8 \sqrt{s}=8 TeV

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    Measurements are presented of electroweak boson production using data from pppp collisions at a centre-of-mass energy of s=8 TeV\sqrt{s} = 8\mathrm{\,Te\kern -0.1em V}. The analysis is based on an integrated luminosity of 2.0 fb−12.0\mathrm{\,fb}^{-1} recorded with the LHCb detector. The bosons are identified in the W→ΌΜW\rightarrow\mu\nu and Z→Ό+Ό−Z\rightarrow\mu^{+}\mu^{-} decay channels. The cross-sections are measured for muons in the pseudorapidity range 2.020 GeV ⁣/c2.0 20{\mathrm{\,Ge\kern -0.1em V\!/}c} and, in the case of the ZZ boson, a dimuon mass within 60<MÎŒ+Ό−<120 GeV ⁣/c260 < M_{\mu^{+}\mu^{-}} < 120{\mathrm{\,Ge\kern -0.1em V\!/}c^{2}}. The results are \begin{align*} \sigma_{W^{+}\rightarrow\mu^{+}\nu} &= 1093.6 \pm 2.1 \pm 7.2 \pm 10.9 \pm 12.7{\rm \,pb} \, , \sigma_{W^{-}\rightarrow\mu^{-}\bar{\nu}} &= \phantom{0}818.4 \pm 1.9 \pm 5.0 \pm \phantom{0}7.0 \pm \phantom{0}9.5{\rm \,pb} \, , \sigma_{Z\rightarrow\mu^{+}\mu^{-}} &= \phantom{00}95.0 \pm 0.3 \pm 0.7 \pm \phantom{0}1.1 \pm \phantom{0}1.1{\rm \,pb} \, , \end{align*} where the first uncertainties are statistical, the second are systematic, the third are due to the knowledge of the LHC beam energy and the fourth are due to the luminosity determination. The evolution of the WW and ZZ boson cross-sections with centre-of-mass energy is studied using previously reported measurements with 1.0 fb−11.0\mathrm{\,fb}^{-1} of data at 7 TeV7\mathrm{\,Te\kern -0.1em V}. Differential distributions are also presented. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2015-049.htm
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