54 research outputs found

    Assessment of pollen rewards by foraging bees

    Get PDF
    This is the author accepted manuscript. The final version is available from Wiley via the DOI in this record.The removal of pollen by flower-visiting insects is costly to plants, not only in terms of production, but also via lost reproductive potential. Modern angiosperms have evolved various reward strategies to limit these costs, yet many plant species still offer pollen as a sole or major reward for pollinating insects. 2. The benefits plants gain by offering pollen as a reward for pollinating are defined by the behaviour of their pollinators, some of which feed on the pollen at the flower, while others collect pollen to provision offspring. 3. We explore how pollen impacts on the behaviour and foraging decisions of pollen-collecting bees, drawing comparisons with what is known for nectar rewards. This question is of particular interest since foraging bees typically do not ingest pollen during collection, meaning the sensory pathways involved in evaluating this resource are not immediately obvious. 4. Previous research focussed on whether foraging bees can determine the quality of pollen sources offered by different plant species, and attempted to infer the mechanisms underpinning such evaluations, mainly through observations of collection preferences in the field 5. More recent experimental research has started to focus on if pollen itself can mediate the detection of, and learning about, pollen sources and associated floral cues. 6. We review advancements in the understanding of how bees forage for pollen and respond to variation in pollen quality, and discuss future directions for studying how this ancestral floral food reward shapes the behaviour of pollinating insects

    First observation of a doubly charged tetraquark and its neutral partner

    Get PDF
    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

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

    Get PDF
    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

    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

    Get PDF
    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

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

    Get PDF
    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

    Get PDF
    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

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

    Get PDF
    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

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

    Get PDF
    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

    Test of lepton universality in beauty-quark decays

    Get PDF
    The standard model of particle physics currently provides our best description of fundamental particles and their interactions. The theory predicts that the different charged leptons, the electron, muon and tau, have identical electroweak interaction strengths. Previous measurements have shown that a wide range of particle decays are consistent with this principle of lepton universality. This article presents evidence for the breaking of lepton universality in beauty-quark decays, with a significance of 3.1 standard deviations, based on proton–proton collision data collected with the LHCb detector at CERN’s Large Hadron Collider. The measurements are of processes in which a beauty meson transforms into a strange meson with the emission of either an electron and a positron, or a muon and an antimuon. If confirmed by future measurements, this violation of lepton universality would imply physics beyond the standard model, such as a new fundamental interaction between quarks and leptons

    Reception and learning of electric fields in bees

    No full text
    • 

    corecore