467 research outputs found

    Global Incidence and Risk Factors Associated With Postoperative Urinary Retention Following Elective Inguinal Hernia Repair

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    Importance Postoperative urinary retention (POUR) is a well-recognized complication of inguinal hernia repair (IHR). A variable incidence of POUR has previously been reported in this context, and contradictory evidence surrounds potential risk factors.Objective To ascertain the incidence of, explore risk factors for, and determine the health service outcomes of POUR following elective IHR.Design, Setting, and Participants The Retention of Urine After Inguinal Hernia Elective Repair (RETAINER I) study, an international, prospective cohort study, recruited participants between March 1 and October 31, 2021. This study was conducted across 209 centers in 32 countries in a consecutive sample of adult patients undergoing elective IHR.Exposure Open or minimally invasive IHR by any surgical technique, under local, neuraxial regional, or general anesthesia.Main Outcomes and Measures The primary outcome was the incidence of POUR following elective IHR. Secondary outcomes were perioperative risk factors, management, clinical consequences, and health service outcomes of POUR. A preoperative International Prostate Symptom Score was measured in male patients.Results In total, 4151 patients (3882 male and 269 female; median [IQR] age, 56 [43-68] years) were studied. Inguinal hernia repair was commenced via an open surgical approach in 82.2% of patients (n = 3414) and minimally invasive surgery in 17.8% (n = 737). The primary form of anesthesia was general in 40.9% of patients (n = 1696), neuraxial regional in 45.8% (n = 1902), and local in 10.7% (n = 446). Postoperative urinary retention occurred in 5.8% of male patients (n = 224), 2.97% of female patients (n = 8), and 9.5% (119 of 1252) of male patients aged 65 years or older. Risk factors for POUR after adjusted analyses included increasing age, anticholinergic medication, history of urinary retention, constipation, out-of-hours surgery, involvement of urinary bladder within the hernia, temporary intraoperative urethral catheterization, and increasing operative duration. Postoperative urinary retention was the primary reason for 27.8% of unplanned day-case surgery admissions (n = 74) and 51.8% of 30-day readmissions (n = 72).Conclusions The findings of this cohort study suggest that 1 in 17 male patients, 1 in 11 male patients aged 65 years or older, and 1 in 34 female patients may develop POUR following IHR. These findings could inform preoperative patient counseling. In addition, awareness of modifiable risk factors may help to identify patients at increased risk of POUR who may benefit from perioperative risk mitigation strategies

    Pseudorapidity densities of charged particles with transverse momentum thresholds in pp collisions at √ s = 5.02 and 13 TeV

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    The pseudorapidity density of charged particles with minimum transverse momentum (pT) thresholds of 0.15, 0.5, 1, and 2 GeV/c is measured in pp collisions at the center of mass energies of √s=5.02 and 13 TeV with the ALICE detector. The study is carried out for inelastic collisions with at least one primary charged particle having a pseudorapidity (η) within 0.8pT larger than the corresponding threshold. In addition, measurements without pT-thresholds are performed for inelastic and nonsingle-diffractive events as well as for inelastic events with at least one charged particle having |η|2GeV/c), highlighting the importance of such measurements for tuning event generators. The new measurements agree within uncertainties with results from the ATLAS and CMS experiments obtained at √s=13TeV.

    Higher-order correlations between different moments of two flow amplitudes in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}}=5.02 TeV

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    International audienceThe correlations between different moments of two flow amplitudes, extracted with the recently developed asymmetric cumulants, are measured in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV recorded by the ALICE detector at the LHC. The magnitudes of the measured observables show a dependence on the different moments as well as on the collision centrality, indicating the presence of non-linear response in all even moments up to the eighth. Furthermore, the higher-order asymmetric cumulants show different signatures than the symmetric and lower-order asymmetric cumulants. Comparisons with state-of-the-art event generators using two different parameterizations obtained from Bayesian optimization show differences between data and simulations in many of the studied observables, indicating a need for further tuning of the models behind those event generators. These results provide new and independent constraints on the initial conditions and transport properties of the system created in heavy-ion collisions

    First measurement of the t|t|-dependence of incoherent J/ψ\psi photonuclear production

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    International audienceThe first measurement of the cross section for incoherent photonuclear production of J/ψ\psi vector meson as a function of the Mandelstam t|t| variable is presented. The measurement was carried out with the ALICE detector at midrapidity, y<0.8|y|<0.8, using ultra-peripheral collisions of Pb nuclei at a centre-of-mass energy per nucleon pair sNN=5.02\sqrt{s_{\mathrm{NN}}} = 5.02 TeV. This rapidity interval corresponds to a Bjorken-xx range (0.3(0.3-1.4)×1031.4)\times 10^{-3}. Cross sections are reported in five t|t| intervals in the range 0.04<t<10.04<|t|<1~GeV2^2 and compared to the predictions of different models. Models that ignore quantum fluctuations of the gluon density in the colliding hadron predict a t|t|-dependence of the cross section much steeper than in data. The inclusion of such fluctuations in the same models provides a better description of the data

    Data-driven precision determination of the material budget in ALICE

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    The knowledge of the material budget with a high precision is fundamental for measurements of direct photon production using the photon conversion method due to its direct impact on the total systematic uncertainty. Moreover, it influences many aspects of the charged-particle reconstruction performance. In this article, two procedures to determine data-driven corrections to the material-budget description in ALICE simulation software are developed. One is based on the precise knowledge of the gas composition in the Time Projection Chamber. The other is based on the robustness of the ratio between the produced number of photons and charged particles, to a large extent due to the approximate isospin symmetry in the number of produced neutral and charged pions. Both methods are applied to ALICE data allowing for a reduction of the overall material budget systematic uncertainty from 4.5% down to 2.5%. Using these methods, a locally correct material budget is also achieved. The two proposed methods are generic and can be applied to any experiment in a similar fashion.The knowledge of the material budget with a high precision is fundamental for measurements of direct photon production using the photon conversion method due to its direct impact on the total systematic uncertainty. Moreover, it influences many aspects of the charged-particle reconstruction performance. In this article, two procedures to determine data-driven corrections to the material-budget description in ALICE simulation software are developed. One is based on the precise knowledge of the gas composition in the Time Projection Chamber. The other is based on the robustness of the ratio between the produced number of photons and charged particles, to a large extent due to the approximate isospin symmetry in the number of produced neutral and charged pions. Both methods are applied to ALICE data allowing for a reduction of the overall material budget systematic uncertainty from 4.5% down to 2.5%. Using these methods, a locally correct material budget is also achieved. The two proposed methods are generic and can be applied to any experiment in a similar fashion

    Measurement of Non-prompt D0\rm D^0-meson Elliptic Flow in Pb-Pb Collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV

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    International audienceThe elliptic flow (v2v_2) of D0\rm D^0 mesons from beauty-hadron decays (non-prompt D0\rm D^0) was measured in midcentral (30-50%) Pb-Pb collisions at a centre-of-mass energy per nucleon pair sNN\sqrt{s_{\rm NN}} = 5.02 TeV with the ALICE detector at the LHC. The D0\rm D^0 mesons were reconstructed at midrapidity (y<0.8|y|<0.8) from their hadronic decay D0Kπ+\mathrm{D^0 \to K^-\pi^+}, in the transverse momentum interval 2<pT<122 < p_{\rm T} < 12 GeV/cc. The result indicates a positive v2v_2 for non-prompt D0\rm D^0 mesons with a significance of 2.7σ\sigma. The non-prompt D0\rm D^0-meson v2v_2 is lower than that of prompt non-strange D mesons with 3.2σ\sigma significance in 2<pT<82 < p_{\rm T} < 8 GeV/cc, and compatible with the v2v_2 of beauty-decay electrons. Theoretical calculations of beauty-quark transport in a hydrodynamically expanding medium describe the measurement within uncertainties

    Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies

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    International audienceThe first measurements of skewness and kurtosis of mean transverse momentum (pT\langle p_\mathrm{T}\rangle) fluctuations are reported in Pb-Pb collisions at sNN\sqrt{s_\mathrm{NN}} = 5.02 TeV, Xe-Xe collisions at sNN\sqrt{s_\mathrm{NN}}== 5.44 TeV and pp collisions at s=5.02\sqrt{s} = 5.02 TeV using the ALICE detector. The measurements are carried out as a function of system size dNch/dηη<0.51/3\langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle_{|\eta|<0.5}^{1/3}, using charged particles with transverse momentum (pTp_\mathrm{T}) and pseudorapidity (η\eta), in the range 0.2<pT<3.00.2 < p_\mathrm{T} < 3.0 GeV/cc and η<0.8|\eta| < 0.8, respectively. In Pb-Pb and Xe-Xe collisions, positive skewness is observed in the fluctuations of pT\langle p_\mathrm{T}\rangle for all centralities, which is significantly larger than what would be expected in the scenario of independent particle emission. This positive skewness is considered a crucial consequence of the hydrodynamic evolution of the hot and dense nuclear matter created in heavy-ion collisions. Furthermore, similar observations of positive skewness for minimum bias pp collisions are also reported here. Kurtosis of pT\langle p_\mathrm{T}\rangle fluctuations is found to be in good agreement with the kurtosis of Gaussian distribution, for most central Pb-Pb collisions. Hydrodynamic model calculations with MUSIC using Monte Carlo Glauber initial conditions are able to explain the measurements of both skewness and kurtosis qualitatively from semicentral to central collisions in Pb--Pb system. Color reconnection mechanism in PYTHIA8 model seems to play a pivotal role in capturing the qualitative behavior of the same measurements in pp collisions

    Photoproduction of K+^{+}K^{-} pairs in ultra-peripheral collisions

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    International audienceK+^{+}K^{-} pairs may be produced in photonuclear collisions, either from the decays of photoproduced ϕ(1020)\phi (1020) mesons, or directly as non-resonant K+^{+}K^{-} pairs. Measurements of K+^{+}K^{-} photoproduction probe the couplings between the ϕ(1020)\phi (1020) and charged kaons with photons and nuclear targets. We present the first measurement of coherent photoproduction of K+^{+}K^{-} pairs on lead ions in ultra-peripheral collisions using the ALICE detector, including the first investigation of direct K+^{+}K^{-} production. There is significant K+^{+}K^{-} production at low transverse momentum, consistent with coherent photoproduction on lead targets. In the mass range 1.1<MKK<1.41.1 < M_{\rm{KK}} < 1.4 GeV/c2c^2 above the ϕ(1020)\phi (1020) resonance, for rapidity yKK<0.8|y_{\rm{KK}}|<0.8 and pT,KK<0.1p_{\rm T,KK} < 0.1 GeV/cc, the measured coherent photoproduction cross section is dσ/dy\mathrm{d}\sigma/\mathrm{d}y = 3.37 ± 0.61\pm\ 0.61 (stat.) ± 0.15\pm\ 0.15 (syst.) mb. The centre-of-mass energy per nucleon of the photon-nucleus (Pb) system WγPb,nW_{\gamma \mathrm{Pb, n}} ranges from 33 to 188 GeV, far higher than previous measurements on heavy-nucleus targets. The cross section is larger than expected for ϕ(1020)\phi (1020) photoproduction alone. The mass spectrum is fit to a cocktail consisting of ϕ(1020)\phi (1020) decays, direct K+^{+}K^{-} photoproduction, and interference between the two. The confidence regions for the amplitude and relative phase angle for direct K+^{+}K^{-} photoproduction are presented

    Photoproduction of K+^{+}K^{-} pairs in ultra-peripheral collisions

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    International audienceK+^{+}K^{-} pairs may be produced in photonuclear collisions, either from the decays of photoproduced ϕ(1020)\phi (1020) mesons, or directly as non-resonant K+^{+}K^{-} pairs. Measurements of K+^{+}K^{-} photoproduction probe the couplings between the ϕ(1020)\phi (1020) and charged kaons with photons and nuclear targets. We present the first measurement of coherent photoproduction of K+^{+}K^{-} pairs on lead ions in ultra-peripheral collisions using the ALICE detector, including the first investigation of direct K+^{+}K^{-} production. There is significant K+^{+}K^{-} production at low transverse momentum, consistent with coherent photoproduction on lead targets. In the mass range 1.1<MKK<1.41.1 < M_{\rm{KK}} < 1.4 GeV/c2c^2 above the ϕ(1020)\phi (1020) resonance, for rapidity yKK<0.8|y_{\rm{KK}}|<0.8 and pT,KK<0.1p_{\rm T,KK} < 0.1 GeV/cc, the measured coherent photoproduction cross section is dσ/dy\mathrm{d}\sigma/\mathrm{d}y = 3.37 ± 0.61\pm\ 0.61 (stat.) ± 0.15\pm\ 0.15 (syst.) mb. The centre-of-mass energy per nucleon of the photon-nucleus (Pb) system WγPb,nW_{\gamma \mathrm{Pb, n}} ranges from 33 to 188 GeV, far higher than previous measurements on heavy-nucleus targets. The cross section is larger than expected for ϕ(1020)\phi (1020) photoproduction alone. The mass spectrum is fit to a cocktail consisting of ϕ(1020)\phi (1020) decays, direct K+^{+}K^{-} photoproduction, and interference between the two. The confidence regions for the amplitude and relative phase angle for direct K+^{+}K^{-} photoproduction are presented

    Charged-particle production as a function of the relative transverse activity classifier in pp, p-Pb, and Pb-Pb collisions at the LHC

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    International audienceMeasurements of charged-particle production in pp, p-Pb, and Pb-Pb collisions in the toward, away, and transverse regions with the ALICE detector are discussed. These regions are defined event-by-event relative to the azimuthal direction of the charged trigger particle, which is the reconstructed particle with the largest transverse momentum (pTtrigp_{\mathrm{T}}^{\rm trig}) in the range 8<pTtrig<158<p_{\mathrm{T}}^{\rm trig}<15 GeV/c/c. The toward and away regions contain the primary and recoil jets, respectively; both regions are accompanied by the underlying event (UE). In contrast, the transverse region perpendicular to the direction of the trigger particle is dominated by the so-called UE dynamics, and includes also contributions from initial- and final-state radiation. The relative transverse activity classifier, RT=NchT/NchTR_{\mathrm{T}}=N_{\mathrm{ch}}^{\mathrm{T}}/\langle N_{\mathrm{ch}}^{\mathrm{T}}\rangle, is used to group events according to their UE activity, where NchTN_{\mathrm{ch}}^{\mathrm{T}} is the charged-particle multiplicity per event in the transverse region and NchT\langle N_{\mathrm{ch}}^{\mathrm{T}}\rangle is the mean value over the whole analysed sample. The energy dependence of the RTR_{\mathrm{T}} distributions in pp collisions at s=2.76\sqrt{s}=2.76, 5.02, 7, and 13 TeV is reported, exploring the Koba-Nielsen-Olesen (KNO) scaling properties of the multiplicity distributions. The first measurements of charged-particle pTp_{\rm T} spectra as a function of RTR_{\mathrm{T}} in the three azimuthal regions in pp, p-Pb, and Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}}=5.02 TeV are also reported. Data are compared with predictions obtained from the event generators PYTHIA 8 and EPOS LHC. This set of measurements is expected to contribute to the understanding of the origin of collective-like effects in small collision systems (pp and p-Pb)
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