1,573 research outputs found
Multi-particle azimuthal correlations in p-Pb and Pb-Pb collisions at the CERN Large Hadron Collider
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 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
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
which is indicative of a Bessel-Gaussian
function for the 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 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
Multiplicity dependence of jet-like two-particle correlations in p-Pb collisions at = 5.02 TeV
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 5.0 GeV/ 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
. 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
ĐĐșŃŃĐ°Đ»ŃĐœŃ ĐżĐžŃĐ°ĐœĐœŃ ŃДалŃĐ·Đ°ŃŃŃ ŃĐżĐŸŃĐ”ŃĐœĐžŃ Đ·ĐŸĐ±ĐŸĐČ'ŃĐ·Đ°ĐœŃ ĐČ ĐœĐŸŃĐ°ŃŃĐ°Đ»ŃĐœĐŸĐŒŃ ĐżŃĐŸŃĐ”ŃŃ
ĐĄŃĐ°ŃŃŃ ĐżŃĐžŃĐČŃŃĐ”ĐœĐ° ŃĐ”ĐŸŃĐ”ŃĐžŃĐœĐŸĐŒŃ ĐŽĐŸŃĐ»ŃĐŽĐ¶Đ”ĐœĐœŃ ĐČажлОĐČĐŸŃŃŃ ĐČĐžĐșĐŸŃĐžŃŃĐ°ĐœĐœŃ ŃŃĐœŃŃŃĐžŃ
ĐŒĐ”Ń
Đ°ĐœŃĐ·ĐŒŃĐČ ĐżŃĐ”ĐČĐ”ĐœŃĐžĐČĐœĐŸŃ ŃŃŃĐžŃŃŃ ŃĐ° ĐŽŃŃĐČĐŸŃŃŃ ĐżŃĐ°ĐČĐŸĐ·Đ°Ń
ĐžŃĐœĐŸŃ ŃŃĐœĐșŃŃŃ ĐœĐŸŃĐ°ŃŃĐ°ŃŃ.
ĐĐŸĐČĐ”ĐŽĐ”ĐœĐŸ, ŃĐŸ ĐœĐŸŃĐ°ŃŃŃŃ ŃĐș гаŃĐ°ĐœŃ ĐżŃĐ”ĐČĐ”ĐœŃĐžĐČĐœĐŸŃŃŃ ĐżŃĐ°ĐČĐŸĐČŃĐŽĐœĐŸŃĐžĐœ ŃДалŃĐ·ŃŃ ŃĐČĐŸŃ ĐżŃĐ°ĐČĐŸĐ·Đ°Ń
ĐžŃĐœŃ ŃŃĐœĐșŃŃŃ ĐœĐ” лОŃĐ” ĐœĐ° ŃŃĐ°ĐŽŃŃ ŃДалŃĐ·Đ°ŃŃŃ ŃĐżĐŸŃĐ”ŃĐœĐžŃ
Đ·ĐŸĐ±ĐŸĐČŃĐ·Đ°ĐœŃ, ŃĐ»ŃŃ
ĐŸĐŒ ĐČŃĐžĐœĐ”ĐœĐœŃ ĐČĐžĐșĐŸĐœĐ°ĐČŃĐŸĐłĐŸ ĐœĐ°ĐżĐžŃŃ ĐœĐ° Đ±ĐŸŃĐłĐŸĐČĐŸĐŒŃ ĐŽĐŸĐșŃĐŒĐ”ĐœŃŃ, Đ° Ń ĐœĐ° ŃŃĐ°ĐŽŃŃ ŃĐ·ĐłĐŸĐŽĐ¶Đ”ĐœĐœŃ ŃĐ° ĐČĐžĐșĐ»Đ°ĐŽĐ”ĐœĐœŃ ĐČŃŃŃ
ŃŃŃĐŸŃĐœĐžŃ
ŃĐŒĐŸĐČ ĐŽĐŸĐłĐŸĐČĐŸŃŃ.
ĐĐ»ŃŃĐŸĐČŃ ŃĐ»ĐŸĐČĐ°: ĐœĐŸŃĐ°ŃŃĐ°Ń; ĐżŃĐ°ĐČĐŸĐ·Đ°Ń
ĐžŃĐœĐ° ŃŃĐœĐșŃŃŃ ĐœĐŸŃĐ°ŃŃĐ°ŃŃ; ĐČĐžĐșĐŸĐœĐ°ĐœĐœŃ Đ·ĐŸĐ±ĐŸĐČŃĐ·Đ°ĐœŃ; ĐżŃĐ”ĐČĐ”ĐœŃĐžĐČĐœĐ° ŃŃŃĐžŃŃŃ.ĐĄŃĐ°ŃŃŃ ĐżĐŸŃĐČŃŃĐ”ĐœĐ° ŃĐ”ĐŸŃĐ”ŃĐžŃĐ”ŃĐșĐŸĐŒŃ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃ ĐœĐ”ĐŸĐ±Ń
ĐŸĐŽĐžĐŒĐŸŃŃĐž ĐžŃĐżĐŸĐ»ŃĐ·ĐŸĐČĐ°ĐœĐžŃ
ŃŃŃĐ”ŃŃĐČŃŃŃĐžŃ
ĐŒĐ”Ń
Đ°ĐœĐžĐ·ĐŒĐŸĐČ ĐżŃĐ”ĐČĐ”ĐœŃĐžĐČĐœĐŸĐč ŃŃŃĐžŃОО Đž ĐŽĐ”ĐčŃŃĐČĐ”ĐœĐœĐŸŃŃĐž ĐżŃĐ°ĐČĐŸĐ·Đ°ŃĐžŃĐœĐŸĐč
ŃŃĐœĐșŃОО ĐœĐŸŃĐ°ŃОаŃĐ°. ĐĐŸĐșĐ°Đ·ŃĐČĐ°Đ”ŃŃŃ, ŃŃĐŸ ĐœĐŸŃĐ°ŃĐžŃŃ ĐșĐ°Đș гаŃĐ°ĐœŃ ĐżŃĐ”ĐČĐ”ĐœŃĐžĐČĐœĐŸŃŃĐž ĐżŃĐ°ĐČĐŸĐŸŃĐœĐŸŃĐ”ĐœĐžĐč ŃДалОзŃĐ”Ń ŃĐČĐŸĐž ĐżŃĐ°ĐČĐŸĐ·Đ°ŃĐžŃĐœŃĐ” ŃŃĐœĐșŃОО ĐœĐ” ŃĐŸĐ»ŃĐșĐŸ ĐœĐ° ŃŃаЎОО ŃДалОзаŃОО
ĐžĐżĐŸŃĐ”ŃĐœŃŃ
ĐŸĐ±ŃĐ·Đ°ŃДлŃŃŃĐČ, ĐČ ŃĐČŃĐ·Đž Ń ŃĐŸĐČĐ”ŃŃĐ”ĐœĐžĐ”ĐŒ ĐžŃĐżĐŸĐ»ĐœĐžŃДлŃĐœĐŸĐč ĐœĐ°ĐŽĐżĐžŃĐž ĐœĐ° ĐŽĐŸĐ»ĐłĐŸĐČĐŸĐŒ
ĐŽĐŸĐșŃĐŒĐ”ĐœŃĐ”, Đ° Đž ĐœĐ° ŃŃаЎОО ŃĐŸĐłĐ»Đ°ŃĐŸĐČĐ°ĐœĐžŃ Đž ĐžĐ·Đ»ĐŸĐ¶Đ”ĐœĐžŃ ĐČŃĐ”Ń
ŃŃŃĐ”ŃŃĐČĐ”ĐœĐœŃŃ
ŃŃĐ»ĐŸĐČĐžĐč ĐŽĐŸĐłĐŸĐČĐŸŃĐ°.
ĐĐ»ŃŃĐ”ĐČŃĐ” ŃĐ»ĐŸĐČĐ°: ĐœĐŸŃĐ°ŃОаŃ; ĐżŃĐ°ĐČĐŸĐ·Đ°ŃĐžŃĐœĐ°Ń ŃŃĐœĐșŃĐžŃ ĐœĐŸŃĐ°ŃОаŃŃ; ĐžŃĐżĐŸĐ»ĐœĐ”ĐœĐžĐ” ĐŸĐ±ŃĐ·Đ°ŃДлŃŃŃĐČ; ĐżŃĐ”ĐČĐ”ĐœŃĐžĐČĐœĐ°Ń ŃŃŃĐžŃĐžŃ.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
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
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
CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTĂFICO E TECNOLĂGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAĂĂO DE AMPARO Ă PESQUISA DO ESTADO DE SĂO 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 CIENTĂFICO E TECNOLĂGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAĂĂO DE AMPARO Ă PESQUISA DO ESTADO DE SĂO PAULOCNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTĂFICO E TECNOLĂGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAĂĂO DE AMPARO Ă PESQUISA DO ESTADO DE SĂO PAULOSem informaçãoSem informaçãoSem informaçãoAgĂȘncias de fomento estrangeiras apoiaram essa pesquisa, mais informaçÔes acesse artig
Observation of flow angle and flow magnitude fluctuations in Pb-Pb collisions at sNN=5.02TeV at the CERN Large Hadron Collider
This Letter reports on the first measurements of transverse momentum dependent flow angle n and flow magnitude vn fluctuations determined using new four-particle correlators. The measurements are performed for various centralities in PbâPb collisions at a center-of-mass energy per nucleon pair of âs NN = 5.02 TeV with ALICE at the CERN Large Hadron Collider. Both flow angle and flow magnitude fluctuations are observed in the presented centrality ranges and are strongest in the most central collisions and for a transverse momentum pT > 2 GeV/c. Comparison with theoretical models, including iEBE-VISHNU, MUSIC, and AMPT, show that the measurements exhibit unique sensitivities to the initial state of heavy-ion collisions
Accessing the strong interaction between Î baryons and charged kaons with the femtoscopy technique at the LHC
The interaction between Î baryons and kaons/antikaons is a crucial ingredient for the strangeness S=0 and S=-2 sector of the mesonâbaryon interaction at low energies. In particular, the Lambda-Kbar might help in understanding the origin of states such as the Csi(1620), whose nature and properties are still under debate. Experimental data on Lambda-K and Lambda-Kbar systems are scarce, leading to large uncertainties and tension between the available theoretical predictions constrained by such data. In this Letter we present the measurements of ÎâKKâ and ÎâKK+ correlations obtained in the high-multiplicity triggered data sample in pp collisions at sqrt(s) = 13 TeV recorded by ALICE at the LHC. The correlation function for both pairs is modeled using the LednickĂœâLyuboshits analytical formula and the corresponding scattering parameters are extracted. The ÎâKK+ correlations show the presence of several structures at relative momenta k* above 200 MeV/c, compatible with the Ω baryon, the , and resonances decaying into ÎâKâ pairs. The low k* region in the ÎâKK+ also exhibits the presence of the state, expected to strongly couple to the measured pair. The presented data allow to access the ÎK+ and ÎKâ strong interaction with an unprecedented precision and deliver the first experimental observation of the decaying into ÎKâ
Measurement of the production of high-p(T) electrons from heavy-flavour hadron decays in Pb-Pb collisions at root s(NN)=2.76 TeV
CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTĂFICO E TECNOLĂGICO - CNPQFINANCIADORA DE ESTUDOS E PROJETOS - FINEPFUNDAĂĂO DE AMPARO Ă PESQUISA DO ESTADO DE SĂO PAULO - FAPESPElectrons from heavy-flavour hadron decays (charm and beauty) were measured with the ALICE detector in Pb-Pb collisions at a centre-of-mass of energy root s(NN) = 2.76 TeV. The transverse momentum (pT) differential production yields at mid-rapidity were used to calculate the nuclear modification factor R-AA in the interval 3 < p(T) < 18 GeV/c. The R-AA shows a strong suppression compared to binary scaling of pp collisions at the same energy (up to a factor of 4) in the 10% most central Pb-Pb collisions. There is a centrality trend of suppression, and a weaker suppression (down to a factor of 2) in semi-peripheral (50-80%) collisions is observed. The suppression of electrons in this broad p(T) interval indicates that both charm and beauty quarks lose energy when they traverse the hot medium formed in Pb-Pb collisions at LHC.771467481CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTĂFICO E TECNOLĂGICO - CNPQFINANCIADORA DE ESTUDOS E PROJETOS - FINEPFUNDAĂĂO DE AMPARO Ă PESQUISA DO ESTADO DE SĂO PAULO - FAPESPCONSELHO NACIONAL DE DESENVOLVIMENTO CIENTĂFICO E TECNOLĂGICO - CNPQFINANCIADORA DE ESTUDOS E PROJETOS - FINEPFUNDAĂĂO DE AMPARO Ă PESQUISA DO ESTADO DE SĂO PAULO - FAPESPSem informaçãoSem informaçãoSem informaçãoThe ALICE Collaboration would like to thank all its engineers and technicians for their invaluable contributions to the construction of the experiment and the CERN accelerator teams for the outstanding performance of the LHC complex. The ALICE Collaboration gratefully acknowledges the resources and support provided by all Grid centres and the Worldwide LHC Computing Grid (WLCG) collaboration. The ALICE Collaboration acknowledges the following funding agencies for their support in building and running the ALICE detector: A.I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation (ANSL), State Committee of Science and World Federation of Scientists (WFS), Armenia; Austrian Academy of Sciences and Nationalstiftung fĂŒr Forschung, Technologie und Entwicklung, Austria; Conselho Nacional de Desenvolvimento CientĂfico e TecnolĂłgico (CNPq), Financiadora de Estudos e Projetos (Finep) and Fundação de Amparo Ă Pesquisa do Estado de SĂŁo Paulo (FAPESP), Brazil; Ministry of Education of China (MOE of China), Ministry of Science & Technology of China (MOST of China) and National Natural Science Foundation of China (NSFC), China; Ministry of Science, Education and Sports and Croatian Science Foundation, Croatia; Centro de Investigaciones EnergĂ©ticas, Medioambientales y TecnolĂłgicas (CIEMAT), Cuba; Ministry of Education, Youth and Sports of the Czech Republic, Czech Republic; Danish National Research Foundation (DNRF), The Carlsberg Foundation and The Danish Council for Independent ResearchâNatural Sciences, Denmark; Helsinki Institute of Physics (HIP), Finland; Commissariat Ă l'Energie Atomique (CEA) and Institut National de Physique NuclĂ©aire et de Physique des Particules (IN2P3) and Centre National de la Recherche Scientifique (CNRS), France; Bundesministerium fĂŒr Bildung, Wissenschaft, Forschung und Technologie (BMBF) and GSI Helmholtzzentrum fĂŒr Schwerionenforschung GmbH, Germany; Ministry of Education, Research and Religious Affairs, Greece; National Research, Development and Innovation Office, Hungary; Department of Atomic Energy, Government of India (DAE), India; Indonesian Institute of Science, Indonesia; Centro Fermi â Museo Storico della Fisica e Centro Studi e Ricerche Enrico Fermi and Istituto Nazionale di Fisica Nucleare (INFN), Italy; Institute for Innovative Science and Technology, Nagasaki Institute of Applied Science (IIST), Japan Society for the Promotion of Science (JSPS) KAKENHI and Japanese Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan; Consejo Nacional de Ciencia y TecnologĂa (CONACYT), through Fondo de CooperaciĂłn Internacional en Ciencia y TecnologĂa (FONCICYT) and DirecciĂłn General de Asuntos del Personal Academico (DGAPA), Mexico; Nationaal instituut voor subatomaire fysica (Nikhef), Netherlands; The Research Council of Norway, Norway; Commission on Science and Technology for Sustainable Development in the South (COMSATS), Pakistan; Pontificia Universidad CatĂłlica del PerĂș, Peru; Ministry of Science and Higher Education and National Science Centre, Poland; Ministry of Education and Scientific Research, Institute of Atomic Physics and Romanian National Agency for Science, Technology and Innovation, Romania; Joint Institute for Nuclear Research (JINR), Ministry of Education and Science of the Russian Federation and National Research Centre Kurchatov Institute, Russia; Ministry of Education, Science, Research and Sport of the Slovak Republic, Slovakia; National Research Foundation of South Africa, South Africa; Korea Institute of Science and Technology Information and National Research Foundation of Korea (NRF), South Korea; Centro de Investigaciones EnergĂ©ticas, Medioambientales y TecnolĂłgicas (CIEMAT) and Ministerio de Ciencia e Innovacion, Spain; Knut & Alice Wallenberg Foundation (KAW) and Swedish Research Council (VR), Sweden; European Organization for Nuclear Research, Switzerland; National Science and Technology Development Agency (NSDTA), Office of the Higher Education Commission under NRU project of Thailand and Suranaree University of Technology (SUT), Thailand; Turkish Atomic Energy Agency (TAEK), Turkey; National Academy of Sciences of Ukraine, Ukraine; Science and Technology Facilities Council (STFC), United Kingdom; National Science Foundation of the United States of America (NSF) and United States Department of Energy, Office of Nuclear Physics (DOE NP), United States
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