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<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msup><mml:mi>K</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mn>892</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mn>0</mml:mn></mml:msup></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>ϕ</mml:mi><mml:mo>(</mml:mo><mml:mn>1020</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math> meson production at high transverse momentum in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math> and Pb-Pb collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mi mathvariant="italic">NN</mml:mi></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>2.76</mml:mn></mml:mrow></mml:math> TeV

J. AdamFaculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech RepublicD. AdamováNuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech RepublicM. M. AggarwalPhysics Department, Panjab University, Chandigarh, IndiaG. Aglieri RinellaEuropean Organization for Nuclear Research (CERN), Geneva, SwitzerlandM. AgnelloDipartimento DISAT del Politecnico and Sezione INFN, Turin, ItalyN. AgrawalIndian Institute of Technology Bombay (IIT), Mumbai, IndiaZ. AhammedVariable Energy Cyclotron Centre, Kolkata, IndiaS. AhmadDepartment of Physics, Aligarh Muslim University, Aligarh, IndiaS. U. AhnKorea Institute of Science and Technology Information, Daejeon, South KoreaS. AiolaYale University, New Haven, Connecticut, USAA. AkindinovInstitute for Theoretical and Experimental Physics, Moscow, RussiaS. N. AlamVariable Energy Cyclotron Centre, Kolkata, IndiaD. S. D. AlbuquerqueUniversidade Estadual de Campinas (UNICAMP), Campinas, BrazilD. AleksandrovNational Research Centre Kurchatov Institute, Moscow, RussiaB. AlessandroSezione INFN, Turin, ItalyD. AlexandreSchool of Physics and Astronomy, University of Birmingham, Birmingham, United KingdomR. Alfaro MolinaInstituto de Física, Universidad Nacional Autónoma de México, Mexico City, MexicoA. AliciCentro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, ItalyA. AlkinBogolyubov Institute for Theoretical Physics, Kiev, UkraineJ. AlmeDepartment of Physics and Technology, University of Bergen, Bergen, NorwayT. AltFrankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, GermanyS. AltinpinarDepartment of Physics and Technology, University of Bergen, Bergen, NorwayI. AltsybeevC. Alves Garcia PradoUniversidade de São Paulo (USP), São Paulo, BrazilM. AnCentral China Normal University, Wuhan, ChinaC. AndreiH. A. AndrewsSchool of Physics and Astronomy, University of Birmingham, Birmingham, United KingdomA. AndronicResearch Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, GermanyV. AnguelovPhysikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, GermanyC. AnsonPhysics Department, Creighton University, Omaha, Nebraska, USAT. AntičićRudjer Bošković Institute, Zagreb, CroatiaF. AntinoriSezione INFN, Padova, ItalyP. AntonioliSezione INFN, Bologna, ItalyR. AnwarUniversity of Houston, Houston, Texas, USAL. AphecetcheSUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, FranceH. AppelshäuserInstitut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, GermanyS. ArcelliDipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, ItalyR. ArnaldiSezione INFN, Turin, ItalyO. W. ArnoldExcellence Cluster Universe, Technische Universität München, Munich, GermanyI. C. ArseneDepartment of Physics, University of Oslo, Oslo, NorwayM. ArslandokInstitut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, GermanyB. AudurierSUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, FranceA. AugustinusEuropean Organization for Nuclear Research (CERN), Geneva, SwitzerlandR. AverbeckResearch Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, GermanyM. D. AzmiDepartment of Physics, Aligarh Muslim University, Aligarh, IndiaA. BadalàSezione INFN, Catania, ItalyY. W. BaekKonkuk University, Seoul, South KoreaS. BagnascoSezione INFN, Turin, ItalyR. BailhacheInstitut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, GermanyR. BalaPhysics Department, University of Jammu, Jammu, IndiaA. BaldisseriIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France, Saclay, FranceM. BallHelmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, GermanyR. C. BaralInstitute of Physics, Bhubaneswar, IndiaAnastasia Maria BarbanoDipartimento di Fisica dell'Università and Sezione INFN, Turin, ItalyR. BarberaDipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, ItalyF. BarileDipartimento Interateneo di Fisica “M. Merlin” and Sezione INFN, Bari, ItalyL. BarioglioDipartimento di Fisica dell'Università and Sezione INFN, Turin, ItalyG. G. BarnaföldiWigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, HungaryL. S. BarnbyEuropean Organization for Nuclear Research (CERN), Geneva, SwitzerlandV. BarretLaboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, FranceP. BartaliniCentral China Normal University, Wuhan, ChinaKlaus BarthEuropean Organization for Nuclear Research (CERN), Geneva, SwitzerlandJ. BartkeThe Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, PolandE. BartschInstitut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, GermanyM. BasileDipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, ItalyN. BastidLaboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, FranceS. BasuVariable Energy Cyclotron Centre, Kolkata, IndiaB. BathenInstitut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, GermanyG. BatigneSUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, FranceA. Batista CamejoLaboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, FranceB. BatyunyaJoint Institute for Nuclear Research (JINR), Dubna, RussiaPaul Christoph BatzingDepartment of Physics, University of Oslo, Oslo, NorwayI. G. BeardenNiels Bohr Institute, University of Copenhagen, Copenhagen, DenmarkH. BeckPhysikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, GermanyC. BeddaDipartimento DISAT del Politecnico and Sezione INFN, Turin, ItalyN. K. BeheraInha University, Incheon, South KoreaI. BelikovUniversité de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, FranceF. BelliniDipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, ItalyH. Martı́nezBenemérita Universidad Autónoma de Puebla, Puebla, MexicoR. BellwiedUniversity of Houston, Houston, Texas, USAL. G. E. BeltranUniversidad Autónoma de Sinaloa, Culiacán, MexicoV. BelyaevMoscow Engineering Physics Institute, Moscow, RussiaG. BencediWigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, HungaryS. BeolèDipartimento di Fisica dell'Università and Sezione INFN, Turin, ItalyA. BercuciY. BerdnikovPetersburg Nuclear Physics Institute, Gatchina, RussiaD. BerenyiWigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, HungaryR. A. BertensInstitute for Subatomic Physics of Utrecht University, Utrecht, NetherlandsD. BerzanoEuropean Organization for Nuclear Research (CERN), Geneva, SwitzerlandL. BetevEuropean Organization for Nuclear Research (CERN), Geneva, SwitzerlandA. BhasinPhysics Department, University of Jammu, Jammu, IndiaI. R. BhatPhysics Department, University of Jammu, Jammu, IndiaA. K. BhatiPhysics Department, Panjab University, Chandigarh, IndiaB. BhattacharjeeGauhati University, Department of Physics, Guwahati, IndiaJ. BhomThe Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, PolandL. BianchiUniversity of Houston, Houston, Texas, USAN. BianchiLaboratori Nazionali di Frascati, INFN, Frascati, ItalyC. BianchinWayne State University, Detroit, Michigan, USAJ. BielčíkFaculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech RepublicJ. BielčíkováNuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
2017lv
ABI

Аннотация

The production of ${K}^{*}{(892)}^{0}$ and $\ensuremath{\phi}(1020)$ mesons in proton-proton ($pp$) and lead-lead (Pb-Pb) collisions at $\sqrt{{s}_{\mathit{NN}}}=2.76\phantom{\rule{4pt}{0ex}}\mathrm{TeV}$ has been analyzed using a high luminosity data sample accumulated in 2011 with the ALICE detector at the Large Hadron Collider (LHC). Transverse momentum (${p}_{\mathrm{T}}$) spectra have been measured for ${K}^{*}{(892)}^{0}$ and $\ensuremath{\phi}(1020)$ mesons via their hadronic decay channels for ${p}_{\mathrm{T}}$ up to $20\phantom{\rule{4pt}{0ex}}\mathrm{GeV}/c$. The measurements in $pp$ collisions have been compared to model calculations and used to determine the nuclear modification factor and particle ratios. The ${K}^{*}{(892)}^{0}/K$ ratio exhibits significant reduction from $pp$ to central Pb-Pb collisions, consistent with the suppression of the ${K}^{*}{(892)}^{0}$ yield at low ${p}_{\mathrm{T}}$ due to rescattering of its decay products in the hadronic phase. In central Pb-Pb collisions the ${p}_{\mathrm{T}}$ dependent $\ensuremath{\phi}(1020)/\ensuremath{\pi}$ and ${K}^{*}{(892)}^{0}/\ensuremath{\pi}$ ratios show an enhancement over $pp$ collisions for ${p}_{\mathrm{T}}\ensuremath{\approx}3\phantom{\rule{4pt}{0ex}}\mathrm{GeV}/c$, consistent with previous observations of strong radial flow. At high ${p}_{\mathrm{T}}$, particle ratios in Pb-Pb collisions are similar to those measured in $pp$ collisions. In central Pb-Pb collisions, the production of ${K}^{*}{(892)}^{0}$ and $\ensuremath{\phi}(1020)$ mesons is suppressed for ${p}_{\mathrm{T}}&gt;8\phantom{\rule{4pt}{0ex}}\mathrm{GeV}/c$. This suppression is similar to that of charged pions, kaons, and protons, indicating that the suppression does not depend on particle mass or flavor in the light quark sector.

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