1,416 research outputs found

    The ALICE CPV Detector

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    The Charged-Particle Veto (CPV) detector of ALICE at the LHC is presented. Physics motivation for the detector, its construction and operation in physics runs are shortly discussed. Readout electronics and data taking conditions are described. Special attention is focused on CPV automation via the detector control system. Different states of the detector and protection algorithms implemented into the control system are described

    Multiplicity dependence of jet-like two-particle correlations in p-Pb collisions at sNN\sqrt{s_{NN}} = 5.02 TeV

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    Two-particle angular correlations between unidentified charged trigger and associated particles are measured by the ALICE detector in p-Pb collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV. The transverse-momentum range 0.7 <pT,assoc<pT,trig< < p_{\rm{T}, assoc} < p_{\rm{T}, trig} < 5.0 GeV/cc is examined, to include correlations induced by jets originating from low momen\-tum-transfer scatterings (minijets). The correlations expressed as associated yield per trigger particle are obtained in the pseudorapidity range ∣η∣<0.9|\eta|<0.9. The near-side long-range pseudorapidity correlations observed in high-multiplicity p-Pb collisions are subtracted from both near-side short-range and away-side correlations in order to remove the non-jet-like components. The yields in the jet-like peaks are found to be invariant with event multiplicity with the exception of events with low multiplicity. This invariance is consistent with the particles being produced via the incoherent fragmentation of multiple parton--parton scatterings, while the yield related to the previously observed ridge structures is not jet-related. The number of uncorrelated sources of particle production is found to increase linearly with multiplicity, suggesting no saturation of the number of multi-parton interactions even in the highest multiplicity p-Pb collisions. Further, the number scales in the intermediate multiplicity region with the number of binary nucleon-nucleon collisions estimated with a Glauber Monte-Carlo simulation.Comment: 23 pages, 6 captioned figures, 1 table, authors from page 17, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/161

    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

    Long- and short-range correlations and their event-scale dependence in high-multiplicity pp collisions at 1as = 13 TeV

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    Two-particle angular correlations are measured in high-multiplicity proton-proton collisions at s = 13 TeV by the ALICE Collaboration. The yields of particle pairs at short-( 06\u3b7 3c 0) and long-range (1.6 < | 06\u3b7| < 1.8) in pseudorapidity are extracted on the near-side ( 06\u3c6 3c 0). They are reported as a function of transverse momentum (pT) in the range 1 < pT< 4 GeV/c. Furthermore, the event-scale dependence is studied for the first time by requiring the presence of high-pT leading particles or jets for varying pT thresholds. The results demonstrate that the long-range \u201cridge\u201d yield, possibly related to the collective behavior of the system, is present in events with high-pT processes as well. The magnitudes of the short- and long-range yields are found to grow with the event scale. The results are compared to EPOS LHC and PYTHIA 8 calculations, with and without string-shoving interactions. It is found that while both models describe the qualitative trends in the data, calculations from EPOS LHC show a better quantitative agreement for the pT dependency, while overestimating the event-scale dependency. [Figure not available: see fulltext.

    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

    Insight into particle production mechanisms via angular correlations of identified particles in pp collisions at root s=7 TeV

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    Sem informaçãoTwo-particle angular correlations were measured in pp collisions at root s = 7 TeV for pions, kaons, protons, and lambdas, for all particle/anti-particle combinations in the pair. Data for mesons exhibit an expected peak dominated by effects associated with mini-jets and are well reproduced by general purpose Monte Carlo generators. However, for baryon-baryon and anti-baryon-anti-baryon pairs, where both particles have the same baryon number, a near-side anti-correlation structure is observed instead of a peak. This effect is interpreted in the context of baryon production mechanisms in the fragmentation process. It currently presents a challenge to Monte Carlo models and its origin remains an open question.778117Sem informaçãoSem informaçãoSem informaçãoFunded by SCOAP3

    Search for a common baryon source in high-multiplicity pp collisions at the LHC

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    We report on the measurement of the size of the particle-emitting source from two-baryon correlations with ALICE in high-multiplicity pp collisions at s=13 TeV. The source radius is studied with low relative momentum p–p, p‟–p‟, p–Λ, and p‟–Λ‟ pairs as a function of the pair transverse mass mT considering for the first time in a quantitative way the effect of strong resonance decays. After correcting for this effect, the radii extracted for pairs of different particle species agree. This indicates that protons, antiprotons, Λ s, and Λ‟ s originate from the same source. Within the measured mT range (1.1–2.2) GeV/c2the invariant radius of this common source varies between 1.3 and 0.85 fm. These results provide a precise reference for studies of the strong hadron–hadron interactions and for the investigation of collective properties in small colliding systems. © 2020 CERN for the benefit of the ALICE CollaborationPeer reviewe

    First measurement of the |t|-dependence of coherent J/ψ photonuclear production

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