Event-Shape Engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV

Acharya, S.; Acosta, F.; Adamová, D.; Adler, A.; Adolfsson, J.; Aggarwal, M.; Aglieri Rinella, G.; Agnello, M.; Agrawal, N.; Ahammed, Z.; Ahn, S.; Aiola, S.; Akindinov, A.; Al-Turany, M.; Alam, S.; Albuquerque, D.; Aleksandrov, D.; Alessandro, B.; Alfanda, H.; Alfaro Molina, R.; Ali, Y.; Alici, A.; Alkin, A.; Alme, J.; Alt, T.; Altenkamper, L.; Altsybeev, I.; Anaam, M.; Andrei, C.; Andreou, D.; Andrews, H.; Andronic, A.; Angeletti, M.; Anguelov, V.; Anson, C.; Antičić, T.; Antinori, F.; Antonioli, P.; Anwar, R.; Apadula, N.; Aphecetche, L.; Appelshäuser, H.; Arcelli, S.; Arnaldi, R.; Arratia, M.; Arsene, I.; Arslandok, M.; Augustinus, A.; Averbeck, R.; Azmi, M.; Badalà, A.; Baek, Y.; Bagnasco, S.; Bailhache, R.; Bala, R.; Baldisseri, A.; Ball, M.; Baral, R.; Barbera, R.; Barile, F.; Barioglio, L.; Barnaföldi, G.; Barnby, L.; Barret, V.; Bartalini, P.; Barth, K.; Bartsch, E.; Bastid, N.; Basu, S.; Batigne, G.; Batyunya, B.; Batzing, P.; Bazo Alba, J.; Bearden, I.; Beck, H.; Bedda, C.; Behera, N.; 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Ding, Y.; Divià, R.; Djuvsland, Ø.; Dobrin, A.; Domenicis Gimenez, D.; Dönigus, B.; Dordic, O.; Dubey, A.; Dubla, A.; Ducroux, L.; Dudi, S.; Duggal, A.; Dukhishyam, M.; Dupieux, P.; Ehlers, R.; Elia, D.; Engel, H.; Epple, E.; Erazmus, B.; Erhardt, F.; Erokhin, A.; Ersdal, M.; Espagnon, B.; Eulisse, G.; Eum, J.; Evans, D.; Evdokimov, S.; Fabbietti, L.; Faggin, M.; Faivre, J.; Fantoni, A.; Fasel, M.; Feldkamp, L.; Feliciello, A.; Feofilov, G.; Fernández Téllez, A.; Ferretti, A.; Festanti, A.; Feuillard, V.; Figiel, J.; Figueredo, M.; Filchagin, S.; Finogeev, D.; Fionda, F.; Fiorenza, G.; Flor, F.; Floris, M.; Foertsch, S.; Foka, P.; Fokin, S.; Fragiacomo, E.; Francescon, A.; Francisco, A.; Frankenfeld, U.; Fronze, G.; Fuchs, U.; Furget, C.; Furs, A.; Fusco Girard, M.; Gaardhøje, J.; Gagliardi, M.; Gago, A.; Gajdosova, K.; Gallio, M.; Galvan, C.; Ganoti, P.; Garabatos, C.; Garcia-Solis, E.; Garg, K.; Gargiulo, C.; Garner, K.; Gasik, P.; Gauger, E.; Gay Ducati, M.; Germain, M.; Ghosh, J.; Ghosh, P.; Ghosh, S.; Gianotti, P.; Giubellino, P.; Giubilato, P.; Glässel, P.; Goméz Coral, D.; Gomez Ramirez, A.; Gonzalez, V.; González-Zamora, P.; Gorbunov, S.; Görlich, L.; Gotovac, S.; Grabski, V.; Graczykowski, L.; Graham, K.; Greiner, L.; Grelli, A.; Grigoras, C.; Grigoriev, V.; Grigoryan, A.; Grigoryan, S.; Gronefeld, J.; Grosa, F.; Grosse-Oetringhaus, J.; Grosso, R.; Guernane, R.; Guerzoni, B.; Guittiere, M.; Gulbrandsen, K.; Gunji, T.; Gupta, A.; Gupta, R.; Guzman, I.; Haake, R.; Habib, M.; Hadjidakis, C.; Hamagaki, H.; Hamar, G.; Hamid, M.; Hamon, J.; Hannigan, R.; Haque, M.; Harlenderova, A.; Harris, J.; Harton, A.; Hassan, H.; Hatzifotiadou, D.; Hauer, P.; Hayashi, S.; Heckel, S.; Hellbär, E.; Helstrup, H.; Herghelegiu, A.; Hernandez, E.; Herrera Corral, G.; Herrmann, F.; Hetland, K.; Hilden, T.; Hillemanns, H.; Hills, C.; Hippolyte, B.; Hohlweger, B.; Horak, D.; Hornung, S.; Hosokawa, R.; Hota, J.; Hristov, P.; Huang, C.; Hughes, C.; Huhn, P.; Humanic, T.; Hushnud, H.; Hussain, N.; Hussain, T.; Hutter, D.; Hwang, D.; Iddon, J.; Ilkaev, R.; Inaba, M.; Ippolitov, M.; Islam, M.; Ivanov, M.; Ivanov, V.; Izucheev, V.; Jacak, B.; Jacazio, N.; Jacobs, P.; Jadhav, M.; Jadlovska, S.; Jadlovsky, J.; Jaelani, S.; Jahnke, C.; Jakubowska, M.; Janik, M.; Jena, C.; Jercic, M.; Jevons, O.; Jimenez Bustamante, R.; Jin, M.; Jones, P.; Jusko, A.; Kalinak, P.; Kalweit, A.; Kang, J.; Kaplin, V.; Kar, S.; Karasu Uysal, A.; Karavichev, O.; Karavicheva, T.; Karczmarczyk, P.; Karpechev, E.; Kebschull, U.; Keidel, R.; Keijdener, D.; Keil, M.; Ketzer, B.; Khabanova, Z.; Khan, A.; Khan, S.; Khan, S.; Khanzadeev, A.; Kharlov, Y.; Khatun, A.; Khuntia, A.; Kielbowicz, M.; Kileng, B.; Kim, B.; Kim, B.; Kim, D.; Kim, D.; Kim, E.; Kim, H.; Kim, J.; Kim, J.; Kim, J.; Kim, M.; Kim, S.; Kim, T.; Kim, T.; Kindra, K.; Kirsch, S.; Kisel, I.; Kiselev, S.; Kisiel, A.; Klay, J.; Klein, C.; Klein, J.; Klein-Bösing, C.; Klewin, S.; Kluge, A.; Knichel, M.; Knospe, A.; Kobdaj, C.; Kofarago, M.; Köhler, M.; Kollegger, T.; 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doi:10.1007/JHEP02(2019)150
Event-Shape Engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at $\sqrt{s_{N N}} = 5.02$ $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV

S. Acharya (Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India) ; F. Acosta (Department of Physics, University of California, Berkeley, California, United States) ; D. Adamová (Nuclear Physics Institute of the Czech Academy of Sciences, Řež u Prahy, Czech Republic) ; A. Adler (Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany) ; J. Adolfsson (Lund University Department of Physics, Division of Particle Physics, Lund, Sweden) ; et al. - Show all 1022 authors
The production yield of prompt D mesons and their elliptic flow coefficient v 2 were measured with the Event-Shape Engineering (ESE) technique applied to mid-central (10–30% and 30–50% centrality classes) Pb-Pb collisions at the centre-of-mass energy per nucleon pair $\sqrt{s_{N N}} = 5.02$ $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV, with the ALICE detector at the LHC. The ESE technique allows the classification of events, belonging to the same centrality, according to the azimuthal anisotropy of soft particle production in the collision. The reported measurements give the opportunity to investigate the dynamics of charm quarks in the Quark-Gluon Plasma and provide information on their participation in the collective expansion of the medium. D mesons were reconstructed via their hadronic decays at mid-rapidity, |η| < 0.8, in the transverse momentum interval 1 < p T < 24 GeV/c. The v 2 coefficient is found to be sensitive to the event-shape selection confirming a correlation between the D-meson azimuthal anisotropy and the collective expansion of the bulk matter, while the per-event D-meson yields do not show any significant modification within the current uncertainties.
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    {
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    {
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    {
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        {
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    {
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        {
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    {
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        {
          "country": "Germany", 
          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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    {
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        {
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          "value": "Dipartimento di Fisica e Astronomia dell\u2019Universit\u00e0 and Sezione INFN, Bologna, Italy", 
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    {
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        {
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          "value": "SUBATECH, IMT Atlantique, Universit\u00e9 de Nantes, CNRS-IN2P3, Nantes, France", 
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        {
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          "value": "Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark", 
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    {
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        {
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    {
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        {
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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    {
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        {
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          "value": "Institut de Physique Nucl\u00e9aire d\u2019Orsay (IPNO), Institut National de Physique Nucl\u00e9aire et de Physique des Particules (IN2P3/CNRS), Universit\u00e9 de Paris-Sud, Universit\u00e9 Paris-Saclay, Orsay, France", 
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        {
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          "value": "Nagasaki Institute of Applied Science, Nagasaki, Japan", 
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    {
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        {
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          "value": "Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary", 
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      "given_names": "G.", 
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    {
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        {
          "country": "China", 
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    {
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        {
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          "value": "Universit\u00e9 de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, F-67000, France", 
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    {
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        {
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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    {
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        {
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        {
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    {
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    {
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        {
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          "value": "University of Liverpool, Liverpool, United Kingdom", 
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    {
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        {
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          "value": "Universit\u00e9 de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, F-67000, France", 
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    {
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        {
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          "value": "Physik Department, Technische Universit\u00e4t M\u00fcnchen, Munich, Germany", 
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    {
      "affiliations": [
        {
          "country": "Czech Republic", 
          "value": "Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic", 
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    {
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        {
          "country": "Germany", 
          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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    {
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        {
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      "affiliations": [
        {
          "country": "India", 
          "value": "Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India", 
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    {
      "affiliations": [
        {
          "country": "CERN", 
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    {
      "affiliations": [
        {
          "country": "France", 
          "value": "Institut de Physique Nucl\u00e9aire d\u2019Orsay (IPNO), Institut National de Physique Nucl\u00e9aire et de Physique des Particules (IN2P3/CNRS), Universit\u00e9 de Paris-Sud, Universit\u00e9 Paris-Saclay, Orsay, France", 
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      "given_names": "C.", 
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      "affiliations": [
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    {
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    {
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        {
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          "value": "The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland", 
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    {
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    {
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      "full_name": "Kim, B."
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      "full_name": "Kim, B."
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    {
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          "country": "South Korea", 
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      "full_name": "Kim, D."
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    {
      "affiliations": [
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      "surname": "Kim", 
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      "full_name": "Kim, D."
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    {
      "affiliations": [
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      "surname": "Kim", 
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    {
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      "full_name": "Kim, H."
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    {
      "affiliations": [
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      "full_name": "Kim, J."
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    {
      "affiliations": [
        {
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          "value": "Physikalisches Institut, Ruprecht-Karls-Universit\u00e4t Heidelberg, Heidelberg, Germany", 
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      ], 
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      "full_name": "Kim, J."
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    {
      "affiliations": [
        {
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    {
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        {
          "country": "Germany", 
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      "full_name": "Kim, M."
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    {
      "affiliations": [
        {
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    {
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          "value": "SUBATECH, IMT Atlantique, Universit\u00e9 de Nantes, CNRS-IN2P3, Nantes, France", 
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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  "titles": [
    {
      "source": "Springer", 
      "title": "Event-Shape Engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \\sqrt{s_{\\mathrm{NN}}}=5.02 $$  TeV"
    }
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  "dois": [
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      "value": "10.1007/JHEP02(2019)150"
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    {
      "page_end": "36", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2019", 
      "artid": "JHEP022019150", 
      "year": 2019, 
      "page_start": "1", 
      "journal_issue": "2"
    }
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  "acquisition_source": {
    "date": "2019-07-24T17:40:50.471996", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "e65802daae2711e98f2d02163e01809a"
  }, 
  "page_nr": [
    36
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  "license": [
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      "url": "https://creativecommons.org/licenses/by/3.0", 
      "license": "CC-BY-3.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2019"
    }
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  "control_number": "45840", 
  "collaborations": [
    {
      "value": "The ALICE collaboration"
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      "categories": [
        "nucl-ex", 
        "hep-ex"
      ], 
      "value": "1809.09371"
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  "abstracts": [
    {
      "source": "Springer", 
      "value": "The production yield of prompt D mesons and their elliptic flow coefficient v 2 were measured with the Event-Shape Engineering (ESE) technique applied to mid-central (10\u201330% and 30\u201350% centrality classes) Pb-Pb collisions at the centre-of-mass energy per nucleon pair   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \\sqrt{s_{\\mathrm{NN}}}=5.02 $$  TeV, with the ALICE detector at the LHC. The ESE technique allows the classification of events, belonging to the same centrality, according to the azimuthal anisotropy of soft particle production in the collision. The reported measurements give the opportunity to investigate the dynamics of charm quarks in the Quark-Gluon Plasma and provide information on their participation in the collective expansion of the medium. D mesons were reconstructed via their hadronic decays at mid-rapidity, |\u03b7| &lt; 0.8, in the transverse momentum interval 1 &lt; p T &lt; 24 GeV/c. The v 2 coefficient is found to be sensitive to the event-shape selection confirming a correlation between the D-meson azimuthal anisotropy and the collective expansion of the bulk matter, while the per-event D-meson yields do not show any significant modification within the current uncertainties."
    }
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  "imprints": [
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      "date": "2019-05-07", 
      "publisher": "Springer"
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}
Published on:: 07 May 2019
Publisher:: Springer
Published in:: Journal of High Energy Physics , Volume 2019 (2019)
Issue 2
Pages 1-36
DOI:: https://doi.org/10.1007/JHEP02(2019)150
arXiv:: 1809.09371
Copyrights:: The Author(s)
Licence:: CC-BY-3.0
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