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The production of the prompt charmed mesonsD0,D+, and D∗+ relative to the reaction plane was measured in
Pb-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of √sNN = 2.76 TeV with the ALICE
detector at the CERN Large Hadron Collider. D mesons were reconstructed via their hadronic decays at central
rapidity in the transverse-momentum (pT) interval 2–16 GeV/c. The azimuthal anisotropy is quantified in terms of
the second coefficient v2 in a Fourier expansion of the D-meson azimuthal distribution and in terms of the nuclear
modification factor RAA, measured in the direction of the reaction plane and orthogonal to it. The v2 coefficient
was measured with three different methods and in three centrality classes in the interval 0%–50%. A positive v2 is
observed in midcentral collisions (30%–50% centrality class), with a mean value of 0.204+0.099−0.036 (tot. unc.) in the interval 2 < pT < 6 GeV/c, which decreases towards more central collisions (10%–30% and 0%–10% classes). The positive v2 is also reflected in the nuclear modification factor, which shows a stronger suppression in the direction orthogonal to the reaction plane for midcentral collisions. The measurements are compared to theoretical calculations of charm-quark transport and energy loss in high-density strongly interacting matter at high temperature. The models that include substantial elastic interactions with an expanding medium provide a good description of the observed anisotropy. However, they are challenged to simultaneously describe the strong suppression of high-pT yield of D mesons in central collisions and their azimuthal anisotropy in noncentral collisions.
B. Abelev, J. Adam, D. Adamová, M. M. Aggarwal, M. Agnello, A. Agostinelli, et al. (2014). Azimuthal anisotropy of D-meson production in Pb-Pb collisions at sqrt(s_NN) = 2.76 TeV. PHYSICAL REVIEW. C, NUCLEAR PHYSICS, 90(3), 1-25 [10.1103/PhysRevC.90.034904].
Azimuthal anisotropy of D-meson production in Pb-Pb collisions at sqrt(s_NN) = 2.76 TeV
B. Abelev;J. Adam;D. Adamová;M. M. Aggarwal;M. Agnello;A. Agostinelli;N. Agrawal;Z. Ahammed;N. Ahmad;I. Ahmed;S. U. Ahn;S. A. Ahn;I. Aimo;S. Aiola;M. Ajaz;A. Akindinov;S. N. Alam;D. Aleksandrov;B. Alessandro;D. Alexandre;A. Alici;A. Alkin;J. Alme;T. Alt;S. Altinpinar;I. Altsybeev;C. Alves Garcia Prado;C. Andrei;A. Andronic;V. Anguelov;J. Anielski;T. Antičić;F. Antinori;P. Antonioli;L. Aphecetche;H. Appelshäuser;ARCELLI, SILVIA;N. Armesto;R. Arnaldi;T. Aronsson;I. C. Arsene;M. Arslandok;A. Augustinus;R. Averbeck;T. C. Awes;M. D. Azmi;M. Bach;A. Badalà;Y. W. Baek;S. Bagnasco;R. Bailhache;R. Bala;A. Baldisseri;F. Baltasar Dos Santos Pedrosa;R. C. Baral;R. Barbera;F. Barile;G. G. Barnaföldi;L. S. Barnby;V. Barret;J. Bartke;BASILE, MAURIZIO;N. Bastid;S. Basu;B. Bathen;G. Batigne;A. Batista Camejo;B. Batyunya;P. C. Batzing;C. Baumann;I. G. Bearden;H. Beck;C. Bedda;N. K. Behera;I. Belikov;BELLINI, FRANCESCA;R. Bellwied;E. Belmont Moreno;R. Belmont;V. Belyaev;G. Bencedi;S. Beole;I. 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2014
Abstract
The production of the prompt charmed mesonsD0,D+, and D∗+ relative to the reaction plane was measured in
Pb-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of √sNN = 2.76 TeV with the ALICE
detector at the CERN Large Hadron Collider. D mesons were reconstructed via their hadronic decays at central
rapidity in the transverse-momentum (pT) interval 2–16 GeV/c. The azimuthal anisotropy is quantified in terms of
the second coefficient v2 in a Fourier expansion of the D-meson azimuthal distribution and in terms of the nuclear
modification factor RAA, measured in the direction of the reaction plane and orthogonal to it. The v2 coefficient
was measured with three different methods and in three centrality classes in the interval 0%–50%. A positive v2 is
observed in midcentral collisions (30%–50% centrality class), with a mean value of 0.204+0.099−0.036 (tot. unc.) in the interval 2 < pT < 6 GeV/c, which decreases towards more central collisions (10%–30% and 0%–10% classes). The positive v2 is also reflected in the nuclear modification factor, which shows a stronger suppression in the direction orthogonal to the reaction plane for midcentral collisions. The measurements are compared to theoretical calculations of charm-quark transport and energy loss in high-density strongly interacting matter at high temperature. The models that include substantial elastic interactions with an expanding medium provide a good description of the observed anisotropy. However, they are challenged to simultaneously describe the strong suppression of high-pT yield of D mesons in central collisions and their azimuthal anisotropy in noncentral collisions.
B. Abelev, J. Adam, D. Adamová, M. M. Aggarwal, M. Agnello, A. Agostinelli, et al. (2014). Azimuthal anisotropy of D-meson production in Pb-Pb collisions at sqrt(s_NN) = 2.76 TeV. PHYSICAL REVIEW. C, NUCLEAR PHYSICS, 90(3), 1-25 [10.1103/PhysRevC.90.034904].
B. Abelev;J. Adam;D. Adamová;M. M. Aggarwal;M. Agnello;A. Agostinelli;N. Agrawal;Z. Ahammed;N. Ahmad;I. Ahmed;S. U. Ahn;S. A. Ahn;I. Aimo;S. Aiola;M. ...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/429169
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
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