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The inclusive production of the charm-strange baryon Ω0c is measured for the first time via its semileptonic decay into Ω−e+νe at midrapidity (|y| < 0.8) in proton–proton (pp) collisions at the centre-of-mass energy √s = 13 TeV with the ALICE detector at the LHC. The transverse momentum (pT) differential cross section multiplied by the branching ratio is presented in the interval 2 < pT < 12 GeV/c. The branching-fraction ratio BR(Ω0c → Ω−e+νe)/BR(Ω0c → Ω−π+) is measured to be 1.12 ± 0.22 (stat.) ± 0.27 (syst.). Comparisons with other experimental measurements, as well as with theoretical calculations, are presented.
The measurement of the production of deuterons, tritons and 3He and their antiparticles in Pb-Pb collisions at √sNN = 5.02 TeV is presented in this article. The measurements are carried out at midrapidity (y|< 0.5) as a function of collision centrality using the ALICE detector. The pT-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different center-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.
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 production of K∗(892)± meson resonance is measured at midrapidity (|y|<0.5) in Pb-Pb collisions at sNN−−−√=5.02 TeV using the ALICE detector at the LHC. The resonance is reconstructed via its hadronic decay channel K∗(892)±→K0Sπ±. The transverse momentum distributions are obtained for various centrality intervals in the pT range of 0.4-16 GeV/c. The reported measurements of integrated yields, mean transverse momenta, and particle yield ratios are consistent with previous ALICE measurements for K∗(892)0. The pT-integrated yield ratio 2K∗(892)±/(K++K−) in central Pb-Pb collisions shows a significant suppression (9.3σ) relative to pp collisions. Thermal model calculations overpredict the particle yield ratio. Although both simulations consider the hadronic phase, only HRG-PCE accurately represents the measurements, whereas MUSIC+SMASH tends to overpredict them. These observations, along with the kinetic freeze-out temperatures extracted from the yields of light-flavored hadrons using the HRG-PCE model, indicate a finite hadronic phase lifetime, which increases towards central collisions. The pT-differential yield ratios 2K∗(892)±/(K++K−) and 2K∗(892)±/(π++π−) are suppressed by up to a factor of five at pT<2 GeV/c in central Pb-Pb collisions compared to pp collisions at s√= 5.02 TeV. Both particle ratios and are qualitatively consistent with expectations for rescattering effects in the hadronic phase. The nuclear modification factor shows a smooth evolution with centrality and is below unity at pT>8 GeV/c, consistent with measurements for other light-flavored hadrons. The smallest values are observed in most central collisions, indicating larger energy loss of partons traversing the dense medium.
The production of K∗(892)± meson resonance is measured at midrapidity (|y|<0.5) in Pb-Pb collisions at sNN−−−√=5.02 TeV using the ALICE detector at the LHC. The resonance is reconstructed via its hadronic decay channel K∗(892)±→K0Sπ±. The transverse momentum distributions are obtained for various centrality intervals in the pT range of 0.4-16 GeV/c. The reported measurements of integrated yields, mean transverse momenta, and particle yield ratios are consistent with previous ALICE measurements for K∗(892)0. The pT-integrated yield ratio 2K∗(892)±/(K++K−) in central Pb-Pb collisions shows a significant suppression (9.3σ) relative to pp collisions. Thermal model calculations overpredict the particle yield ratio. Although both simulations consider the hadronic phase, only HRG-PCE accurately represents the measurements, whereas MUSIC+SMASH tends to overpredict them. These observations, along with the kinetic freeze-out temperatures extracted from the yields of light-flavored hadrons using the HRG-PCE model, indicate a finite hadronic phase lifetime, which increases towards central collisions. The pT-differential yield ratios 2K∗(892)±/(K++K−) and 2K∗(892)±/(π++π−) are suppressed by up to a factor of five at pT<2 GeV/c in central Pb-Pb collisions compared to pp collisions at s√= 5.02 TeV. Both particle ratios and are qualitatively consistent with expectations for rescattering effects in the hadronic phase. The nuclear modification factor shows a smooth evolution with centrality and is below unity at pT>8 GeV/c, consistent with measurements for other light-flavored hadrons. The smallest values are observed in most central collisions, indicating larger energy loss of partons traversing the dense medium.
The total charm-quark production cross section per unit of rapidity dσ(cc)/dy, and the fragmentation fractions of charm quarks to different charm-hadron species f(c → hc), are measured for the first time in p–Pb collisions at √sNN = 5.02 TeV at midrapidity (−0.96 < y < 0.04 in the centre-ofmass frame) using data collected by ALICE at the CERN LHC. The results are obtained based on all the available measurements of prompt production of ground-state charm-hadron species: D0, D+,D+s, and J/ψ mesons, and Λ+cand Ξ0cbaryons. The resulting cross section is dσ(cc)/dy = 219.6±6.3 (stat.)+10.5−11.8(syst.)+7.6−2.9(extr.)±5.4 (BR)±4.6 (lumi.)±19.5 (rapidity shape) +15.0 (Ω0c) mb, which is consistent with a binary scaling of pQCD calculations from pp ollisions. The measured fragmentation fractions are compatible with those measured in pp collisions at √s = 5.02 and 13 TeV, showing an increase in the relative production rates of charm baryons with respect to charm mesons in pp and p–Pb collisions compared with e+e − and e−p collisions. The pT-integrated nuclear modification factor of charm quarks, RpPb(cc) = 0.91±0.04 (stat.) +0.08 −0.09 (syst.) +0.04 −0.03 (extr.)±0.03 (lumi.), is found to be consistent with unity and with theoretical predictions including nuclear modifications of the parton distribution functions.
This work aims to differentiate strangeness produced from hard processes (jet-like) and softer processes (underlying event) by measuring the angular correlation between a high-momentum trigger hadron (h) acting as a jet-proxy and a produced strange hadron (φ(1020) meson). Measuring h–φ correlations at midrapidity in p–Pb collisions at √sNN = 5.02 TeV as a function of event multiplicity provides insight into the microscopic origin of strangeness enhancement in small collision systems. The jet-like and the underlying-event-like strangeness production are investigated as a function of event multiplicity. They are also compared between a lower and higher momentum region. The evolution of the per-trigger yields within the near-side (aligned with the trigger hadron) and away-side (in the opposite direction of the trigger hadron) jet is studied separately, allowing for the characterization of two distinct jet-like production regimes. Furthermore, the h–φ correlations within the underlying event give access to a production regime dominated by soft production processes, which can be compared directly to the in-jet production. Comparisons between h–φ and dihadron correlations show that the observed strangeness enhancement is largely driven by the underlying event, where the φ/h ratio is significantly larger than within the jet regions. As multiplicity increases, the fraction of the total φ(1020) yield coming from jets decreases compared to the underlying event production, leading to high-multiplicity events being dominated by the increased strangeness production from the underlying event
Measurements of the production of electrons from heavy-flavour hadron decays in pp collisions at s√=13 TeV at midrapidity with the ALICE detector are presented down to a transverse momentum (pT) of 0.2 GeV/c and up to pT=35 GeV/c, which is the largest momentum range probed for inclusive electron measurements in ALICE. In p−Pb collisions, the production cross section and the nuclear modification factor of electrons from heavy-flavour hadron decays are measured in the pT range 0.5<pT<26 GeV/c at sNN−−−√=8.16 TeV. The nuclear modification factor is found to be consistent with unity within the statistical and systematic uncertainties. In both collision systems, first measurements of the yields of electrons from heavy-flavour hadron decays in different multiplicity intervals normalised to the multiplicity-integrated yield (self-normalised yield) at midrapidity are reported as a function of the self-normalised charged-particle multiplicity estimated at midrapidity. The self-normalised yields in pp and p−Pb collisions grow faster than linear with the self-normalised multiplicity. A strong pT dependence is observed in pp collisions, where the yield of high-pT electrons increases faster as a function of multiplicity than the one of low-pT electrons. The measurement in p−Pb collisions shows no pT dependence within uncertainties. The self-normalised yields in pp and p−Pb collisions are compared with measurements of other heavy-flavour, light-flavour, and strange particles, and with Monte Carlo simulations.
Du fait de la traite négrière qui a vu des millions d’Africains être déportés aux Amériques, les langues européennes (anglais, espagnol, français, néerlandais, portugais) des colons qui y étaient déjà installés et qui avaient un fort besoin en main-d’oeuvre africaine, ont eu à intégrer à des degrés divers de nombreux mots africains. Les chercheurs qui travaillent sur ces africanismes sont d’accord pour dire que ces mots ont deux grandes origines africaines : bantoue et non-bantoue.
The Genet is a little carnivore whose status is not very well-known in Vendée (France). The methods for a county survey about these carnivores are set out in order to get information about its presence. The results will make it possible to map out an atlas showing where it is located and where it lives.
Observation d’une genette, Genetta genetta (Linné, 1758), sur les rives du lac du Jaunay en Vendée
(2001)
The diurnal observation of a Genet, such as the one made in the bocage of Vendée (France) related here, is exceptional because this small carnivore is said to be so shy and so exclusively nocturnal.
Dans les langues bantoues du Gabon, tons lexicaux flottants et tons intonatifs permettent d’expliquer trois phénomènes tonals que nous avons voulu passer en revue dans cet article. Dorénavant, il est donné de croire, avec l’élargissement du domaine d’observation des tons intonatifs aux groupes B10, B20 et B30, qu’un certain nombre de problèmes tonals considérés hier encore comme insolubles ou relevant de types ou de cas tonals, trouvent des solutions ou des analyses satisfaisantes. Déjà, la découverte des tons intonatifs en myènènkomi (B11e) et en tsogo (B31) permet aujourd’hui de proposer une description pour le moins correcte de la tonalité de ces deux langues.
Ce texte s’est voulu une brève présentation des tons phonologiques qu’on rencontre dans les langues bantoues parlées au Gabon. L’élément nouveau ici par rapport à ce que l’on sait de l'analyse de la tonalité des langues bantoues en général, c’est la prise en compte de l'intonation dans l'explication de certaines modifications tonales du niveau lexical dont les tons lexicaux (fixes ou flottants) ne peuvent pas rendre compte.
La présente étude est parvenue à identifier une vingtaine de bantouismes dans le LG et moins d'une dizaine de candidats à bantouismes (six au total), grâce aux cognats et aux candidats à cognats vili que nous avons pu établir. Ce faisant, elle a falsifié le point de vue dominant dans la littérature d'une origine restreinte à trois langues (le kikongo, le kimbundu et l'umbundu) de tous les bantouismes et candidats à bantouismes latino-américains connus à ce jour. La suite du travail est déjà en vue qui consiste à étendre aux autres langues bantoues du Gabon des zones A et B la recherche des mots apparentés aux termes du LG, ce qui assurément ne pourra que rallonger la liste des bantouismes présents dans le LG.
La présente étude revisite la liste des langues bantoues du Gabon contenues dans la classification des langues bantoues de Guthrie (1967 - 1971), en y ajoutant une nouvelle langue, des nouveaux dialectes, et pour la première fois des sous dialectes. Prenant en compte les acquis des classifications antérieures des langues bantoues du Gabon, elle revient sur les propositions de codification de Maho (2003,2006 et 2007) visant à ajouter des nouvelles langues et de nouveaux dialectes dans la liste de Guthrie sans remettre en question le système de codification établi par ce dernier. Des nouvelles propositions sont formulées ici qui réanalysent ou réaménagent les modèles de codification avancés par cet auteur, tout en se portant en faux contre une sacralisation inavouée de la classification de Guthrie qui viserait à mettre ses propositions d’indexation des langues bantoues à l’abris de toute modification ou réaménagement. Enfin, la présente classification revient sur un certain nombre de dénominations et de problèmes orthographiques des noms de langues relevées dans les anciennes classifications, pour proposer des corrections qui tiennent comptent soit du bon sens, soit du point de vue des locuteurs ou des conventions de notation des langues bantoues arrêtées par les linguistes de l’Ecole de Tervuren.
On est parti ici du constat qu’il était impossible à Blanchon de poser les réflexes réels des schèmes tonals des thèmes nominaux du proto-bantou en wumvu de Malinga, à partir du moment où il s’interdisait, sur le plan méthodologique, d’observer le principe d’identité des niveaux de correspondance entre le proto-bantou et le wumvu de Malinga, c’est-à-dire niveau structurel proto-bantou égale niveau structurel wumvu. Nous nous sommes donc attelé dans la section 1 de cette étude à fixer la structure mélodique et tonale des substantifs du wumvu de Malinga, avant de donner les correspondances tonales entre les deux langues à la section 4. Il nous a paru également vicieux de la part de l’auteur d’avancer une explication, fûtelle historique, sur les faits de tonalité observés dans cette langue, dès lors qu’on ne possédait aucune étude quelconque sur la tonalité de cette dernière. Nous avons donc consacré la section 2 de ce travail à l étude des différents processus tonals relevés dans les substantifs du wumvu de Malinga. Dans la section 3, nous avons été amené à mettre en évidence l’incidence de l’accent dans le traitement de la tonalité de cette langue bantoue du Gabon, montrant par là les limites de l’hypothèse explicative de Blanchon. Enfin, en terme de perspective, on ne peut qu’appeler à la réalisation d’une description complète du wumvu de Malinga, afin que son étude historique ne soit que meilleure.