1,253 research outputs found

    Measurements of Λ+c production in pp collisions at √s = 7TeV with ALICE

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    A Large Ion Collider Experiment (ALICE) has been designed to study the strongly interacting medium created in heavy-ion collisions at LHC energies, the Quark Gluon Plasma (QGP). Heavy quarks (charm and beauty), produced in the early stages of the collisions, are among the most powerful probes to study this state of matter. We report about the charmed baryon Λ+c measurement in pp collisions at √s = 7TeV with the ALICE experiment, through the reconstruction of the decay channels Λ+c → pK−π+ and Λ+c → p ÂŻK 0 (and charge conjugates)

    INFN What Next: Ultra-relativistic Heavy-Ion Collisions

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    This document was prepared by the community that is active in Italy, within INFN (Istituto Nazionale di Fisica Nucleare), in the field of ultra-relativistic heavy-ion collisions. The experimental study of the phase diagram of strongly-interacting matter and of the Quark-Gluon Plasma (QGP) deconfined state will proceed, in the next 10-15 years, along two directions: the high-energy regime at RHIC and at the LHC, and the low-energy regime at FAIR, NICA, SPS and RHIC. The Italian community is strongly involved in the present and future programme of the ALICE experiment, the upgrade of which will open, in the 2020s, a new phase of high-precision characterisation of the QGP properties at the LHC. As a complement of this main activity, there is a growing interest in a possible future experiment at the SPS, which would target the search for the onset of deconfinement using dimuon measurements. On a longer timescale, the community looks with interest at the ongoing studies and discussions on a possible fixed-target programme using the LHC ion beams and on the Future Circular Collider.Comment: 99 pages, 56 figure

    Multi-particle azimuthal correlations in p-Pb and Pb-Pb collisions at the CERN Large Hadron Collider

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    Measurements of multi-particle azimuthal correlations (cumulants) for charged particles in p-Pb and Pb-Pb collisions are presented. They help address the question of whether there is evidence for global, flow-like, azimuthal correlations in the p-Pb system. Comparisons are made to measurements from the larger Pb-Pb system, where such evidence is established. In particular, the second harmonic two-particle cumulants are found to decrease with multiplicity, characteristic of a dominance of few-particle correlations in p-Pb collisions. However, when a âˆŁÎ”Î·âˆŁ|\Delta \eta| gap is placed to suppress such correlations, the two-particle cumulants begin to rise at high-multiplicity, indicating the presence of global azimuthal correlations. The Pb-Pb values are higher than the p-Pb values at similar multiplicities. In both systems, the second harmonic four-particle cumulants exhibit a transition from positive to negative values when the multiplicity increases. The negative values allow for a measurement of v2{4}v_{2}\{4\} to be made, which is found to be higher in Pb-Pb collisions at similar multiplicities. The second harmonic six-particle cumulants are also found to be higher in Pb-Pb collisions. In Pb-Pb collisions, we generally find v2{4}≃v2{6}≠0v_{2}\{4\} \simeq v_{2}\{6\}\neq 0 which is indicative of a Bessel-Gaussian function for the v2v_{2} distribution. For very high-multiplicity Pb-Pb collisions, we observe that the four- and six-particle cumulants become consistent with 0. Finally, third harmonic two-particle cumulants in p-Pb and Pb-Pb are measured. These are found to be similar for overlapping multiplicities, when a âˆŁÎ”Î·âˆŁ>1.4|\Delta\eta| > 1.4 gap is placed.Comment: 25 pages, 11 captioned figures, 3 tables, authors from page 20, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/87

    АĐșŃ‚ŃƒĐ°Đ»ŃŒĐœŃ– ĐżĐžŃ‚Đ°ĐœĐœŃ рДалізації Ń–ĐżĐŸŃ‚Đ”Ń‡ĐœĐžŃ… Đ·ĐŸĐ±ĐŸĐČ'ŃĐ·Đ°ĐœŃŒ ĐČ ĐœĐŸŃ‚Đ°Ń€Ń–Đ°Đ»ŃŒĐœĐŸĐŒŃƒ ĐżŃ€ĐŸŃ†Đ”ŃŃ–

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    Стаття просĐČŃŃ‡Đ”ĐœĐ° Ń‚Đ”ĐŸŃ€Đ”Ń‚ĐžŃ‡ĐœĐŸĐŒŃƒ ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐœŃŽ ĐČажлОĐČĐŸŃŃ‚Ń– ĐČĐžĐșĐŸŃ€ĐžŃŃ‚Đ°ĐœĐœŃ Ń–ŃĐœŃƒŃŽŃ‡ĐžŃ… ĐŒĐ”Ń…Đ°ĐœŃ–Đ·ĐŒŃ–ĐČ ĐżŃ€Đ”ĐČĐ”ĐœŃ‚ĐžĐČĐœĐŸŃ— юстоції та ЮієĐČĐŸŃŃ‚Ń– праĐČĐŸĐ·Đ°Ń…ĐžŃĐœĐŸŃ— Ń„ŃƒĐœĐșції ĐœĐŸŃ‚Đ°Ń€Ń–Đ°Ń‚Ńƒ. Đ”ĐŸĐČĐ”ĐŽĐ”ĐœĐŸ, Ń‰ĐŸ ĐœĐŸŃ‚Đ°Ń€Ń–ŃƒŃ яĐș ĐłĐ°Ń€Đ°ĐœŃ‚ прДĐČĐ”ĐœŃ‚ĐžĐČĐœĐŸŃŃ‚Ń– праĐČĐŸĐČŃ–ĐŽĐœĐŸŃĐžĐœ Ń€Đ”Đ°Đ»Ń–Đ·ŃƒŃ” сĐČĐŸŃ— праĐČĐŸĐ·Đ°Ń…ĐžŃĐœŃ– Ń„ŃƒĐœĐșції ĐœĐ” лОшД ĐœĐ° стаЮії рДалізації Ń–ĐżĐŸŃ‚Đ”Ń‡ĐœĐžŃ… Đ·ĐŸĐ±ĐŸĐČŃĐ·Đ°ĐœŃŒ, ŃˆĐ»ŃŃ…ĐŸĐŒ ĐČŃ‡ĐžĐœĐ”ĐœĐœŃ ĐČĐžĐșĐŸĐœĐ°ĐČŃ‡ĐŸĐłĐŸ ĐœĐ°ĐżĐžŃŃƒ ĐœĐ° Đ±ĐŸŃ€ĐłĐŸĐČĐŸĐŒŃƒ ĐŽĐŸĐșŃƒĐŒĐ”ĐœŃ‚Ń–, Đ° і ĐœĐ° стаЮії ŃƒĐ·ĐłĐŸĐŽĐ¶Đ”ĐœĐœŃ та ĐČĐžĐșĐ»Đ°ĐŽĐ”ĐœĐœŃ ĐČсіх Ń–ŃŃ‚ĐŸŃ‚ĐœĐžŃ… ŃƒĐŒĐŸĐČ ĐŽĐŸĐłĐŸĐČĐŸŃ€Ńƒ. ĐšĐ»ŃŽŃ‡ĐŸĐČі ŃĐ»ĐŸĐČĐ°: ĐœĐŸŃ‚Đ°Ń€Ń–Đ°Ń‚; праĐČĐŸĐ·Đ°Ń…ĐžŃĐœĐ° Ń„ŃƒĐœĐșція ĐœĐŸŃ‚Đ°Ń€Ń–Đ°Ń‚Ńƒ; ĐČĐžĐșĐŸĐœĐ°ĐœĐœŃ Đ·ĐŸĐ±ĐŸĐČŃĐ·Đ°ĐœŃŒ; прДĐČĐ”ĐœŃ‚ĐžĐČĐœĐ° юстоція.Статья ĐżĐŸŃĐČŃŃ‰Đ”ĐœĐ° Ń‚Đ”ĐŸŃ€Đ”Ń‚ĐžŃ‡Đ”ŃĐșĐŸĐŒŃƒ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃŽ ĐœĐ”ĐŸĐ±Ń…ĐŸĐŽĐžĐŒĐŸŃŃ‚Đž ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžŃ ŃŃƒŃ‰Đ”ŃŃ‚ĐČующох ĐŒĐ”Ń…Đ°ĐœĐžĐ·ĐŒĐŸĐČ ĐżŃ€Đ”ĐČĐ”ĐœŃ‚ĐžĐČĐœĐŸĐč юстоцоо Đž ĐŽĐ”ĐčстĐČĐ”ĐœĐœĐŸŃŃ‚Đž праĐČĐŸĐ·Đ°Ń‰ĐžŃ‚ĐœĐŸĐč Ń„ŃƒĐœĐșцоо ĐœĐŸŃ‚Đ°Ń€ĐžĐ°Ń‚Đ°. Đ”ĐŸĐșĐ°Đ·Ń‹ĐČĐ°Đ”Ń‚ŃŃ, Ń‡Ń‚ĐŸ ĐœĐŸŃ‚Đ°Ń€ĐžŃƒŃ ĐșĐ°Đș ĐłĐ°Ń€Đ°ĐœŃ‚ прДĐČĐ”ĐœŃ‚ĐžĐČĐœĐŸŃŃ‚Đž праĐČĐŸĐŸŃ‚ĐœĐŸŃˆĐ”ĐœĐžĐč Ń€Đ”Đ°Đ»ĐžĐ·ŃƒĐ”Ń‚ сĐČĐŸĐž праĐČĐŸĐ·Đ°Ń‰ĐžŃ‚ĐœŃ‹Đ” Ń„ŃƒĐœĐșцоо ĐœĐ” Ń‚ĐŸĐ»ŃŒĐșĐŸ ĐœĐ° стаЮоо рДалОзацОО ĐžĐżĐŸŃ‚Đ”Ń‡ĐœŃ‹Ń… ĐŸĐ±ŃĐ·Đ°Ń‚Đ”Đ»ŃŒŃŃ‚ĐČ, ĐČ ŃĐČŃĐ·Đž с ŃĐŸĐČĐ”Ń€ŃˆĐ”ĐœĐžĐ”ĐŒ ĐžŃĐżĐŸĐ»ĐœĐžŃ‚Đ”Đ»ŃŒĐœĐŸĐč ĐœĐ°ĐŽĐżĐžŃĐž ĐœĐ° ĐŽĐŸĐ»ĐłĐŸĐČĐŸĐŒ ĐŽĐŸĐșŃƒĐŒĐ”ĐœŃ‚Đ”, Đ° Đž ĐœĐ° стаЮоо ŃĐŸĐłĐ»Đ°ŃĐŸĐČĐ°ĐœĐžŃ Đž ĐžĐ·Đ»ĐŸĐ¶Đ”ĐœĐžŃ ĐČсДх ŃŃƒŃ‰Đ”ŃŃ‚ĐČĐ”ĐœĐœŃ‹Ń… ŃƒŃĐ»ĐŸĐČĐžĐč ĐŽĐŸĐłĐŸĐČĐŸŃ€Đ°. КлючДĐČŃ‹Đ” ŃĐ»ĐŸĐČĐ°: ĐœĐŸŃ‚Đ°Ń€ĐžĐ°Ń‚; праĐČĐŸĐ·Đ°Ń‰ĐžŃ‚ĐœĐ°Ń Ń„ŃƒĐœĐșцоя ĐœĐŸŃ‚Đ°Ń€ĐžĐ°Ń‚Ńƒ; ĐžŃĐżĐŸĐ»ĐœĐ”ĐœĐžĐ” ĐŸĐ±ŃĐ·Đ°Ń‚Đ”Đ»ŃŒŃŃ‚ĐČ; прДĐČĐ”ĐœŃ‚ĐžĐČĐœĐ°Ń юстоцоя.This article is dedicated into theoretical research of importance in using special mechanism of prevention justitia and acting law defender functions of notoriety. It is argued that notaries as a guaranty of prevention law relation realizes his law defender functions not only on the stage of realization ipothek obligations, making performance inscription on the duty document, but on the stage of consenting and stating all existence conditions of contract. Key words: notoriety, law defender function of notaries, making obligations, prevention justitia

    Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisions

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    At sufficiently high temperature and energy density, nuclear matter undergoes a transition to a phase in which quarks and gluons are not confined: the quark-gluon plasma (QGP)(1). Such an exotic state of strongly interacting quantum chromodynamics matter is produced in the laboratory in heavy nuclei high-energy collisions, where an enhanced production of strange hadrons is observed(2-6). Strangeness enhancement, originally proposed as a signature of QGP formation in nuclear collisions(7), is more pronounced for multi-strange baryons. Several effects typical of heavy-ion phenomenology have been observed in high-multiplicity proton-proton (pp) collisions(8,9), but the enhanced production of multi-strange particles has not been reported so far. Here we present the first observation of strangeness enhancement in high-multiplicity proton-proton collisions. We find that the integrated yields of strange and multi-strange particles, relative to pions, increases significantly with the event charged-particle multiplicity. The measurements are in remarkable agreement with the p-Pb collision results(10,11), indicating that the phenomenon is related to the final system created in the collision. In high-multiplicity events strangeness production reaches values similar to those observed in Pb-Pb collisions, where a QGP is formed.Peer reviewe

    Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at √sNN=5.02 and 2.76 TeV

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    Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb-Pb collisions at sqrt(s_NN) = 5.02 and 2.76TeV are reported in the pseudorapidity range |eta|< 0.8 and transverse momentum 0.2 < pT < 50 GeV/c. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) ub^-1 in the centrality range 0-80%, is analysed. Flow coefficients up to the sixth flow harmonic (v6) are reported and a detailed comparison among results at the two energies is carried out. The pT dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number n are investigated. An approximate power-law scaling of the form vn(pT) ~ pT^(n/3) is observed for all flow harmonics at low pT (0.2 < pT < 3 GeV/c). At the same time, the ratios vn/vm^(n/m) are observed to be essentially independent of pT for most centralities up to about pT = 10 GeV/c. Analysing the differences among higher-order cumulants of elliptic flow (v2), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event v2 distribution P(v2) is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise P(v2), extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio

    Measurement of azimuthal correlations of D mesons with charged particles in pp collisions at √s=7 TeV and p-Pb collisions at √sNN=5.02 TeV

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    The azimuthal correlations of D mesons with charged particles were measured with the ALICE apparatus in pp collisions at root s = 7 TeV and p-Pb collisions at root sNN = 5.02 TeV at the Large Hadron Collider. D-0, D+, and D*+ mesons and their charge conjugates with transverse momentum 3 0.3 GeV/c. The yield of charged particles in the correlation peak induced by the jet containing the D meson and the peak width are compatible within uncertainties in the two collision systems. The data are described within uncertainties by Monte-Carlo simulations based on PYTHIA, POWHEG, and EPOS 3 event generators.Peer reviewe

    Constraints on jet quenching in p-Pb collisions at root s(NN)=5.02 TeV measured by the event-activity dependence of semi-inclusive hadron-jet distributions

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    CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOThe ALICE Collaboration reports the measurement of semi-inclusive distributions of charged-particle jets recoiling from a high-transverse momentum trigger hadron in p-Pb collisions at root s(NN) = 5.02TeV. Jets are reconstructed from charged-particle tracks using the anti-k(T) algorithm with resolution parameter R = 0.2 and 0.4. A data-driven statistical approach is used to correct the uncorrelated background jet yield. Recoil jet distributions are reported for jet transverse momentum 15 < p(T,jet)(ch) < 50 GeV/c and are compared in various intervals of p-Pb event activity, based on charged-particle multiplicity and zero-degree neutral energy in the forward (Pb-going) direction. The semi-inclusive observable is self-normalized and such comparisons do not require the interpretation of p-Pb event activity in terms of collision geometry, in contrast to inclusive jet observables. These measurements provide new constraints on the magnitude of jet quenching in small systems at the LHC. In p-Pb collisions with high event activity, the average medium-induced out-of-cone energy transport for jets with R = 0.4 and 15 < p(T,jet)(ch) < 50 GeV/c is measured to be less than 0.4 GeV/c at 90% confidence, which is over an order of magnitude smaller than a similar measurement for central Pb-Pb collisions at root s(NN) = 2.76 TeV. Comparison is made to theoretical calculations of jet quenching in small systems, and to inclusive jet measurements in p-Pb collisions selected by event activity at the LHC and in d-Au collisions at RHIC.78395113CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOCNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOSem informaçãoSem informaçãoSem informaçãoAgĂȘncias de fomento estrangeiras apoiaram essa pesquisa, mais informaçÔes acesse artig

    Inclusive J/ψ production at forward and backward rapidity in p-Pb collisions at √sNN=8.16 TeV

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    Inclusive J/psi production is studied in p-Pb interactions at a centre-of-mass energy per nucleon-nucleon collision sqrt(s_NN) = 8.16TeV, using the ALICE detector at the CERN LHC. The J/psi meson is reconstructed, via its decay to a muon pair, in the centre-of-mass rapidity intervals 2.03 < ycms < 3.53 and -4.46 < ycms < -2.96, where positive and negative ycms refer to the p-going and Pb-going direction, respectively. The transverse momentum coverage is pT < 20 GeV/c. In this paper, ycms- and pT-differential cross sections for inclusive J/psi production are presented, and the corresponding nuclear modification factors RpPb are shown. Forward results show a suppression of the J/psi yield with respect to pp collisions, concentrated in the region pT < 5 GeV/c. At backward rapidity no significant suppression is observed. The results are compared to previous measurements by ALICE in p-Pb collisions at sqrt(s_NN) = 5.02TeV and to theoretical calculations. Finally, the ratios RFB between forward- and backward-ycms RpPb values are shown and discussed

    Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at √sNN = 2.76 TeV

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    Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb–Pb collisions at √SNN=2.76 TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.publishedVersio
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