528 research outputs found

    Dynamics of Hot QCD Matter -- Current Status and Developments

    Get PDF
    The discovery and characterization of hot and dense QCD matter, known as Quark Gluon Plasma (QGP), remains the most international collaborative effort and synergy between theorists and experimentalists in modern nuclear physics to date. The experimentalists around the world not only collect an unprecedented amount of data in heavy-ion collisions, at Relativistic Heavy Ion Collider (RHIC), at Brookhaven National Laboratory (BNL) in New York, USA, and the Large Hadron Collider (LHC), at CERN in Geneva, Switzerland but also analyze these data to unravel the mystery of this new phase of matter that filled a few microseconds old universe, just after the Big Bang. In the meantime, advancements in theoretical works and computing capability extend our wisdom about the hot-dense QCD matter and its dynamics through mathematical equations. The exchange of ideas between experimentalists and theoreticians is crucial for the progress of our knowledge. The motivation of this first conference named "HOT QCD Matter 2022" is to bring the community together to have a discourse on this topic. In this article, there are 36 sections discussing various topics in the field of relativistic heavy-ion collisions and related phenomena that cover a snapshot of the current experimental observations and theoretical progress. This article begins with the theoretical overview of relativistic spin-hydrodynamics in the presence of the external magnetic field, followed by the Lattice QCD results on heavy quarks in QGP, and finally, it ends with an overview of experiment results.Comment: Compilation of the contributions (148 pages) as presented in the `Hot QCD Matter 2022 conference', held from May 12 to 14, 2022, jointly organized by IIT Goa & Goa University, Goa, Indi

    Abstracts of 1st International Conference on Machine Intelligence and System Sciences

    Get PDF
    This book contains the abstracts of the papers presented at the International Conference on Machine Intelligence and System Sciences (MISS-2021) Organized by the Techno College of Engineering, Agartala, Tripura, India & Tongmyong University, Busan, South Korea, held on 1–2 November 2021. This conference was intended to enable researchers to build connections between different digital technologies based on Machine Intelligence, Image Processing, and the Internet of Things (IoT). Conference Title: 1st International Conference on Machine Intelligence and System SciencesConference Acronym: MISS-2021Conference Date: 1–2 November 2021Conference Location: Techno College of Engineering Agartala, Tripura(w), IndiaConference Organizer: Techno College of Engineering, Agartala, Tripura, India & Tongmyong University, Busan, South Korea

    Measurement of the angle between jet axes in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV$

    No full text
    This letter presents the first measurement of the angle between different jet axes (denoted as ΔR{\Delta}R) in Pb-Pb collisions. The measurement is carried out in the 0-10% most-central events at sNN=5.02\sqrt{s_ {\rm NN}} = 5.02 TeV. Jets are assembled by clustering charged particles at midrapidity using the anti-kTk_{\rm T} algorithm with resolution parameters R=0.2R=0.2 and 0.40.4 and transverse momenta in the intervals 40<pTchjet<14040 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc and 80<pTchjet<14080 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc, respectively. Measurements at these low transverse momenta enhance the sensitivity to quark-gluon plasma (QGP) effects. A comparison to models implementing various mechanisms of jet energy loss in the QGP shows that the observed narrowing of the Pb-Pb distribution relative to pp can be explained if quark-initiated jets are more likely to emerge from the medium than gluon-initiated jets. These new measurements discard intra-jet pTp_{\rm T} broadening as described in a model calculation with the BDMPS formalism as the main mechanism of energy loss in the QGP. The data are sensitive to the angular scale at which the QGP can resolve two independent splittings, favoring mechanisms that incorporate incoherent energy loss.This letter presents the first measurement of the angle between different jet axes (denoted as ΔR{\Delta}R) in Pb-Pb collisions. The measurement is carried out in the 0-10% most-central events at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV. Jets are assembled by clustering charged particles at midrapidity using the anti-kTk_{\rm T} algorithm with resolution parameters R=0.2R=0.2 and 0.40.4 and transverse momenta in the intervals 40<pTchjet<14040 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc and 80<pTchjet<14080 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc, respectively. Measurements at these low transverse momenta enhance the sensitivity to quark-gluon plasma (QGP) effects. A comparison to models implementing various mechanisms of jet energy loss in the QGP shows that the observed narrowing of the Pb-Pb distribution relative to pp can be explained if quark-initiated jets are more likely to emerge from the medium than gluon-initiated jets. These new measurements discard intra-jet pTp_{\rm T} broadening as described in a model calculation with the BDMPS formalism as the main mechanism of energy loss in the QGP. The data are sensitive to the angular scale at which the QGP can resolve two independent splittings, favoring mechanisms that incorporate incoherent energy loss

    Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV

    Get PDF
    The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p-Pb and Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV down to transverse momentum (pTp_{\rm T}) of 0.5 GeV/cc and 2 GeV/cc, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution (v2v_2) in high-multiplicity p-Pb collisions is positive, with a significance reaching 6.8σ\sigma at low pTp_{\rm T}. Comparisons with the inclusive charged-particle v2v_2 and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle v2v_2 in high-multiplicity p-Pb collisions and indicates that the positive jet-particle v2v_2 is generated by parton interactions.The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p-Pb and Pb-Pb collisions at sNN \sqrt{{\textrm{s}}_{\textrm{NN}}} = 5.02 TeV down to transverse momentum (pT_{T}) of 0.5 GeV/c and 2 GeV/c, respectively, with ALICE. The results obtained in p-Pb collisions are based on a novel three-particle correlation technique. The azimuthal anisotropy coefficient v2_{2} in high-multiplicity p-Pb collisions is positive, with a significance reaching 6.8σ at low pT_{T}, and its magnitude is smaller than in semicentral Pb-Pb collisions. In contrast to the measurements in Pb-Pb collisions, the v2_{2} coefficient is also found independent of pT_{T} within uncertainties. Comparisons with the inclusive charged-particle v2_{2} and with AMPT calculations are discussed. The predictions suggest that parton interactions play an important role in generating a non-zero jet-particle v2_{2} in p-Pb collisions, even though they overestimate the reported measurement. These observations shed new insights on the understanding of the origin of the collective behaviour of jet particles in small systems such as p-Pb collisions, and provide significant stringent new constraints to models.[graphic not available: see fulltext]The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p-Pb and Pb-Pb collisions at sNN\sqrt{s_{\rm NN}} = 5.02 TeV down to transverse momentum (pTp_{\rm T}) of 0.5 GeV/cc and 2 GeV/cc, respectively, with ALICE. The results obtained in p-Pb collisions are based on a novel three-particle correlation technique. The azimuthal anisotropy coefficient v2v_2 in high-multiplicity p-Pb collisions is positive, with a significance reaching 6.8σ\sigma at low pTp_{\rm T}, and its magnitude is smaller than in semicentral Pb-Pb collisions. In contrast to the measurements in Pb-Pb collisions, the v2v_2 coefficient is also found independent of pTp_{\rm T} within uncertainties. Comparisons with the inclusive charged-particle v2v_2 and with AMPT calculations are discussed. The predictions suggest that parton interactions play an important role in generating a non-zero jet-particle v2v_2 in p-Pb collisions, even though they overestimate the reported measurement. These observations shed new insights on the understanding of the origin of the collective behaviour of jet particles in small systems such as p-Pb collisions, and provide significant stringent new constraints to models

    Measurement of the angle between jet axes in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV

    No full text
    International audienceThis letter presents the first measurement of the angle between different jet axes (denoted as ΔR{\Delta}R) in Pb-Pb collisions. The measurement is carried out in the 0-10% most-central events at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV. Jets are assembled by clustering charged particles at midrapidity using the anti-kTk_{\rm T} algorithm with resolution parameters R=0.2R=0.2 and 0.40.4 and transverse momenta in the intervals 40<pTchjet<14040 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc and 80<pTchjet<14080 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc, respectively. Measurements at these low transverse momenta enhance the sensitivity to quark-gluon plasma (QGP) effects. A comparison to models implementing various mechanisms of jet energy loss in the QGP shows that the observed narrowing of the Pb-Pb distribution relative to pp can be explained if quark-initiated jets are more likely to emerge from the medium than gluon-initiated jets. These new measurements discard intra-jet pTp_{\rm T} broadening as described in a model calculation with the BDMPS formalism as the main mechanism of energy loss in the QGP. The data are sensitive to the angular scale at which the QGP can resolve two independent splittings, favoring mechanisms that incorporate incoherent energy loss

    First polarisation measurement of coherently photoproduced J/ψ\psi in ultra-peripheral Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV

    No full text
    The first measurement of the polarisation of coherently photoproduced J/ψ\psi mesons in ultra-peripheral Pb-Pb collisions, using data at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV , is presented. The J/ψ\psi meson is measured via its dimuon decay channel in the forward rapidity interval -4.0 J/ψ mesons in ultra-peripheral Pb–Pb collisions, using data at sNN=5.02 TeV, is presented. The J/ψ meson is measured via its dimuon decay channel in the forward rapidity interval −4.0<y<−2.5 using the ALICE detector at the CERN LHC. An event sample corresponding to an integrated luminosity of 750 μb−1 ± 5% (syst) is analysed. Hadronic activity is highly suppressed since the interaction is mediated by a photon. The polar and azimuthal angle distributions of the decay muons are measured, and the polarisation parameters λθ, λφ, λθφ are extracted. The analysis is carried out in the helicity frame. The results are found to be consistent with a transversely polarised J/ψ. These values are compared with previous measurements by the H1 and ZEUS experiments. The polarisation parameters of coherent J/ψ photoproduction in Pb–Pb collisions are found to be consistent with the s-channel helicity conservation hypothesis.The first measurement of the polarisation of coherently photoproduced J/\psimesonsinultraperipheralPbPbcollisions,usingdataat mesons in ultra-peripheral Pb-Pb collisions, using data at \sqrt{s_{\rm NN}}=5.02TeV,ispresented.TheJ/ = 5.02 TeV, is presented. The J/\psimesonismeasuredviaitsdimuondecaychannelintheforwardrapidityinterval meson is measured via its dimuon decay channel in the forward rapidity interval -4.0 < y < -2.5usingtheALICEdetectorattheCERNLHC.Aneventsamplecorrespondingtoanintegratedluminosityof750 using the ALICE detector at the CERN LHC. An event sample corresponding to an integrated luminosity of 750 \mu\text{b}^{-1}\pm5 5% (syst) is analysed. Hadronic activity is highly suppressed since the interaction is mediated by a photon. The polar and azimuthal angle distributions of the decay muons are measured, and the polarisation parameters \mathbf{\lambda_{\theta}},, \mathbf{\lambda_{\varphi}},, \mathbf{\lambda_{\theta\varphi}}areextracted.Theanalysisiscarriedoutinthehelicityframe.TheresultsarefoundtobeconsistentwithatransverselypolarisedJ/ are extracted. The analysis is carried out in the helicity frame. The results are found to be consistent with a transversely polarised J/\psi.ThesevaluesarecomparedwithpreviousmeasurementsbytheH1andZEUSexperiments.ThepolarisationparametersofcoherentJ/. These values are compared with previous measurements by the H1 and ZEUS experiments. The polarisation parameters of coherent J/\psiphotoproductioninPbPbcollisionsarefoundtobeconsistentwiththe photoproduction in Pb-Pb collisions are found to be consistent with the s$-channel helicity conservation hypothesis

    Measurement of the angle between jet axes in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV

    No full text
    International audienceThis letter presents the first measurement of the angle between different jet axes (denoted as ΔR{\Delta}R) in Pb-Pb collisions. The measurement is carried out in the 0-10% most-central events at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV. Jets are assembled by clustering charged particles at midrapidity using the anti-kTk_{\rm T} algorithm with resolution parameters R=0.2R=0.2 and 0.40.4 and transverse momenta in the intervals 40<pTchjet<14040 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc and 80<pTchjet<14080 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc, respectively. Measurements at these low transverse momenta enhance the sensitivity to quark-gluon plasma (QGP) effects. A comparison to models implementing various mechanisms of jet energy loss in the QGP shows that the observed narrowing of the Pb-Pb distribution relative to pp can be explained if quark-initiated jets are more likely to emerge from the medium than gluon-initiated jets. These new measurements discard intra-jet pTp_{\rm T} broadening as described in a model calculation with the BDMPS formalism as the main mechanism of energy loss in the QGP. The data are sensitive to the angular scale at which the QGP can resolve two independent splittings, favoring mechanisms that incorporate incoherent energy loss

    Measurement of the angle between jet axes in Pb-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV

    No full text
    This letter presents the first measurement of the angle between different jet axes (denoted as ΔR{\Delta}R) in Pb-Pb collisions. The measurement is carried out in the 0-10% most-central events at sNN=5.02\sqrt{s_{\rm NN}} = 5.02 TeV. Jets are assembled by clustering charged particles at midrapidity using the anti-kTk_{\rm T} algorithm with resolution parameters R=0.2R=0.2 and 0.40.4 and transverse momenta in the intervals 40 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc and 80 < p_{\rm T}^{\rm ch jet} < 140 GeV/cc, respectively. Measurements at these low transverse momenta enhance the sensitivity to quark-gluon plasma (QGP) effects. A comparison to models implementing various mechanisms of jet energy loss in the QGP shows that the observed narrowing of the Pb-Pb distribution relative to pp can be explained if quark-initiated jets are more likely to emerge from the medium than gluon-initiated jets. These new measurements discard intra-jet pTp_{\rm T} broadening as described in a model calculation with the BDMPS formalism as the main mechanism of energy loss in the QGP. The data are sensitive to the angular scale at which the QGP can resolve two independent splittings, favoring mechanisms that incorporate incoherent energy loss

    ALICE upgrades during the LHC Long Shutdown 2

    No full text
    A Large Ion Collider Experiment (ALICE) has been conceivedand constructed as a heavy-ion experiment at the LHC. During LHCRuns 1 and 2, it has produced a wide range of physics results usingall collision systems available at the LHC. In order to bestexploit new physics opportunities opening up with the upgraded LHCand new detector technologies, the experiment has undergone a majorupgrade during the LHC Long Shutdown 2 (2019–2022). This comprisesthe move to continuous readout, the complete overhaul of coredetectors, as well as a new online event processing farm with aredesigned online-offline software framework. These improvementswill allow to record Pb-Pb collisions at rates up to 50 kHz, whileensuring sensitivity for signals without a triggerable signature
    corecore