Contribution List

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  1. Enrico Scomparin (Universita e INFN Torino (IT)), Francesco Prino (Universita e INFN Torino (IT)), Roberta Arnaldi (Universita e INFN Torino (IT))
    14/07/2022, 10:30
  2. Francesco Tresso
    14/07/2022, 10:40
  3. Angelo Rivetti (INFN - National Institute for Nuclear Physics)
    14/07/2022, 10:50
  4. Federico Antinori (Universita e INFN, Padova (IT))
    14/07/2022, 11:00
  5. Rasmus Larsen (University of Stavanger)
    14/07/2022, 11:30
  6. Nestor Armesto Perez (Universidade de Santiago de Compostela (ES))
    14/07/2022, 12:00
  7. Fabio Catalano (University and INFN Torino (IT))
    14/07/2022, 14:00
  8. Marco Ruggieri
    14/07/2022, 14:20

    Heavy quarks are considered potential probes of the QCD matter produced in high-energy heavy-ion collisions. In the pre-equilibrium stage of relativistic heavy-ion collisions, strong quasi-classical gluon fields emerge at about $\tau_0=0.08$ fm/c which evolves according to the classical Yang-Mills (CYM) equations. These set of classical fields are known as Glasma. We study the diffusion of the...

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  9. Martin Spousta (Charles University)
    14/07/2022, 14:40
  10. Jing Wang (Massachusetts Inst. of Technology (US))
    14/07/2022, 15:00
  11. Dr Bojana Ilic (Blagojevic)
    14/07/2022, 15:20

    One of the intrinsic features of parton's energy loss is the evident flavor dependence. Inspired by the dead-cone effect in radiative energy loss and experimentally detected suppression mass hierarchy, we address the mass ordering in heavy flavor suppression.

    While mass hierarchy is analyzed within radiative models, collisional interpretation is still lacking. To this end, we apply...

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  12. Sonia Kabana (Instituto De Alta Investigación - Universidad de Tarapacá (CL))
    14/07/2022, 15:40
  13. Joerg Aichelin (SUBATECH)
    14/07/2022, 16:30

    A new Model for J/psi Production in Heavy Ion Collisions
    Denys Yen Arrebato Villar, Joerg Aichelin, Pol Gossiaux
    SUBATECH, Universit?e de Nantes, IMT Atlantique, IN2P3/CNRS,
    4 rue Alfred Kastler, 44307 Nantes cedex 3, France

    The experimental observation of J/psi and Bc mesons multiplicities, distributions and azimuthal flows plays a key role in understanding of the properties of the...

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  14. Krista Lizbeth Smith (Los Alamos National Laboratory (US))
    14/07/2022, 16:50
  15. Dr Xiaojun Yao (Massachusetts Institute of Technology)
    14/07/2022, 17:10

    Quarkonium has been used as an important probe of the quark-gluon plasma in heavy ion collisions. With more precise experimental measurements of quarkonium production conducted at RHIC and LHC, we are able to learn in a more quantitative way how quarkonium interacts with the hot medium. In this talk, I will review the framework of coupled Boltzmann equations to describe quarkonium production...

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  16. Florian Damas (LLR - Centre National de la Recherche Scientifique (FR))
    14/07/2022, 17:30
  17. Georg Wolschin
    14/07/2022, 17:50

    The respective contributions of cold-matter and hot-medium effects to the suppression of $\Upsilon(1S)$ and $\Upsilon(2S)$ mesons in p-Pb collisions at energies reached at the Large Hadron Collider (LHC) are investigated [1]. Whereas known alterations of the parton density functions in the lead nucleus and coherent parton energy loss [2] account for the leading fraction of the modifications in...

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  18. Giuseppe Bruno (Universita e INFN, Bari (IT))
    14/07/2022, 18:10
  19. Jinfeng Liao
    15/07/2022, 09:30

    For heavy ion collisions in the TeV beam energy region, the large number of initial hard scatterings create a richly “doped” hot quark-gluon plasma embedding an unparalleled abundance of charm quarks/anti-quarks. This provides a uniquely “charming” environment for the massive production of exotic hadrons in nuclear collisions and possibly helps solve puzzles about their intrinsic structures,...

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  20. Biaogang Wu (Texas A&M University)
    15/07/2022, 09:50

    We investigate the in-medium kinetics of heavy quarkonia focusing on recent developments and results for the $\psi(2S)$, X(3872), and $B_c$ particles in ultra-relativistic heavy-ion collisions (URHICs). Based on our previous calculations, our approach is governed by two transport parameters for each quarkonium state: the equilibrium limit and inelastic reaction rate. The equilibrium limits are...

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  21. Jiaxing Zhao (Tsinghua University)
    15/07/2022, 10:10

    The deconfined quark-gluon plasma (QGP) created in relativistic heavy-ion collisions is not only a perfect fluid with very small $\eta/s$ but also a most "charming" system with hundreds of charm quarks. Meanwhile, it is widely accepted that the quark hadronization mechanism changes with the appearance of QGP. The production of charmed hadrons differs significantly in $A$-$A$ collisions from...

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  22. Fernando Navarra, Marina Nielsen (Universidade de São paulo)
    15/07/2022, 10:30

    Using the coalescence model, we calculate the multiplicities of X(3872) and $T_{cc}^+$ at the end of the quark gluon plasma phase in nucleus-nucleus collisions at the LHC. Then, using effective lagrangians and a rate equation, we calculate the changes in these multiplicities during the hadron gas phase. Finally, we present the multiplicities at the end of the collisions and also plot them as a...

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  23. Krista Lizbeth Smith (Los Alamos National Laboratory (US))
    15/07/2022, 11:10
  24. Chenxi Gu (Tsinghua University (CN))
    15/07/2022, 11:30
  25. Milan Stojanovic (Purdue University (US))
    15/07/2022, 11:50
  26. Elena Gonzalez Ferreiro
    15/07/2022, 12:10
  27. Stefano Trogolo (CERN)
    15/07/2022, 12:30
  28. Alexander Milov (Weizmann Institute of Science (IL))
    15/07/2022, 12:50

    Multiparton interactions in proton-proton collisions have long been a topic of great interest. A new look at them has begun to emerge from work being done to understand the dynamics of ‘small systems’, a topic that is taking center stage in the physics of relativistic heavy-ion interactions. Numerous studies conducted at the LHC and lower energies reveal that proton-proton collisions at high...

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  29. Ralf Rapp
    15/07/2022, 14:30
  30. Nora brambilla
    15/07/2022, 15:00
  31. Anton Andronic (Westfaelische Wilhelms-Universitaet Muenster (DE))
    15/07/2022, 15:30
  32. Pietro Antonioli (Universita e INFN, Bologna (IT))
    15/07/2022, 16:30
  33. Ivan Vitev
    15/07/2022, 16:50
  34. Gianluca Usai (Universita e INFN, Cagliari (IT))
    15/07/2022, 17:10
  35. Ramona Vogt
    15/07/2022, 17:30

    Open heavy flavors and quarkonium have played important roles in the understanding of the QCD matter produced at high temperatures and low baryon densities. However, they could also provide crucial information about QCD at the lowe center of mass energies employed to probe high baryon density matter at existing or planned facilities.

    For example, a nonperturbative contribution to charm...

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  36. Christoph Blume (Goethe University Frankfurt (DE))
    15/07/2022, 17:50
  37. Santosh Kumar Das (School of Physical Science, Indian Institute of Technology Goa, India)
    16/07/2022, 09:30
  38. Taesoo Song
    16/07/2022, 09:50

    We apply the Low's theorem to soft gluon emission from the heavy quark scattering in nonperturbative strongly interacting quark-gluon plasma (sQGP). The sQGP is described in terms of the DQPM (dynamical quasiparticle model) based on propagator representation in 2PI representation and adjusted to reproduce the EoS from lQCD at finite temperature and chemical potential. Since emitted gluon is...

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  39. Juan Torres-Rincon (Universitat de Barcelona)
    16/07/2022, 10:10

    We have investigated the many-body equations of $D$ and $\overline{B}$ mesons in a thermal medium by applying an effective field theory based on chiral and heavy-quark spin symmetries. Exploiting the same symmetries for the construction of the kinetic theory, we have derived an off-shell Fokker-Planck equation which incorporates information of the full spectral function of these states.

    I...

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  40. laura fabbietti (Technische Universität München)
    16/07/2022, 10:35
  41. Lucia Oliva (Università di Catania, INFN Catania)
    16/07/2022, 11:15
  42. Luca Micheletti (Universita e INFN Torino (IT))
    16/07/2022, 11:35
  43. Lucas Anne Vermunt (Ruprecht Karls Universitaet Heidelberg (DE))
    16/07/2022, 11:55
  44. Salvatore Plumari
    16/07/2022, 12:15
  45. Magdalena Djordjevic
    16/07/2022, 14:00

    High-pt theory and data are traditionally used to explore parton interactions with QGP, while QGP parameters are commonly constrained through low-pt data and corresponding models. However, rare high-pt probes can also be a powerful tool for inferring bulk QGP properties, providing a proper description of high-pt parton-medium interactions.

    We here advocate a novel QGP tomography approach,...

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  46. Marianna Mazzilli (CERN)
    16/07/2022, 14:20
  47. Weiyao Ke (Los Alamos National Laboratory)
    16/07/2022, 14:40
  48. Helena Santos (LIP - Lisbon)
    16/07/2022, 15:00
  49. Patrick Robbe (Université Paris-Saclay (FR))
    16/07/2022, 15:50
  50. Gian Michele Innocenti (CERN)
    16/07/2022, 16:10
  51. Yasser Corrales Morales (Los Alamos National Laboratory (US))
    16/07/2022, 16:30
  52. Yen-Jie Lee (Massachusetts Institute of Technology)
    16/07/2022, 16:50
  53. Enrico Scomparin (Universita e INFN Torino (IT)), Francesco Prino (Universita e INFN Torino (IT)), Roberta Arnaldi (Universita e INFN Torino (IT))
    16/07/2022, 17:20