25–28 Jun 2023
Prague, Czechia
Europe/Prague timezone

Invited Contribution List

38 out of 38 displayed
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  1. Jan Matousek (Charles University (CZ)), Mr Kamil Augsten (Czech Technical University (CZ))
    26/06/2023, 09:00
  2. Nils Huesken (Johannes Gutenberg U. Mainz, Germany)
    26/06/2023, 09:20
  3. Cristian Pisano
    26/06/2023, 09:55
  4. Marco Radici
    26/06/2023, 10:30
  5. Jinlong Zhang (Shandong University)
    26/06/2023, 11:30
  6. Balazs Ujvari (University of Debrecen (HU))
    26/06/2023, 11:55
  7. Mr Thomas Poeschl (Technische Universitaet Muenchen (DE))
    26/06/2023, 12:20
  8. Dr Patrizia Rossi (Jefferson Lab/LNF-INFN)
    26/06/2023, 14:35
  9. Dr Genki Nukazuka (RIKEN BNL Research Center)
    26/06/2023, 15:05
  10. Marco Santimaria (INFN e Laboratori Nazionali di Frascati (IT))
    26/06/2023, 15:30

    The goal of LHCspin is to develop, in the next few years, innovative solutions and cutting-edge technologies to access spin physics in high-energy polarized fixed-target collisions, by exploring a unique kinematic regime given by the LHC beam and by exploiting new probes. This ambitious task poses its basis on the recent installation of SMOG2, the unpolarized gas target in front of the LHCb...

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  11. Bjoern Seitz
    26/06/2023, 15:55
  12. Nobuo Sato
    26/06/2023, 16:45
  13. Joseph Karpie (Jefferson Lab)
    26/06/2023, 17:10
  14. Kei Nagai (Los Alamos National Laboratory)
    26/06/2023, 17:35
  15. Andreas Metz
    27/06/2023, 09:00
  16. Alexey Vladimirov (Universidad Complutense de Madrid)
    27/06/2023, 09:25
  17. Asmita Mukherjee (Indian Institute of Technology, Bombay, India)
    27/06/2023, 09:50

    We present a calculation of the azimuthal asymmetries in back-to-back production of $J/\psi - \mathrm{jet}$ and $J/\psi-\gamma$ in eP collision. We use NRQCD to estimate the $J/\psi$ production, and assume TMD factorization for the back-to-back kinematics. We show that these asymmetries will be useful for probing the the gluon TMDs, like the linearly polarizaed gluon TMD, in unpolarized...

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  18. Albi Kerbizi (Universita e INFN Trieste (IT))
    27/06/2023, 10:15
  19. Isabella Garzia
    27/06/2023, 11:00
  20. harut avakian
    27/06/2023, 11:30
  21. Anna Martin (Trieste University and INFN (IT))
    27/06/2023, 12:00
  22. Dr Silvia Niccolai (CNRS)
    27/06/2023, 14:30
  23. Charlotte Van Hulse (Universidade de Santiago de Compostela (ES))
    27/06/2023, 14:55
  24. Karolina Lavickova (Czech Technical University in Prague (CZ))
    27/06/2023, 15:20
  25. Shohini Bhattacharya
    27/06/2023, 16:15

    Recent advancements have facilitated the approximate computation of light-cone correlation functions in lattice QCD through the evaluation of their Euclidean counterparts. In this presentation, we will provide a brief overview of these significant developments that have direct implications for Generalized Parton Distributions (GPDs). Additionally, we will delve into our latest work, where we...

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  26. Jose Manuel Morgado Chávez (LSN/DPhN/Irfu CEA-Saclay)
    27/06/2023, 16:45
  27. Marija Čuić
    27/06/2023, 17:10
  28. Zhite Yu
    27/06/2023, 17:35
  29. Andrei Gridin (Joint Institute for Nuclear Research (RU))
    28/06/2023, 09:00
  30. Malgorzata Rozalia Niemiec (University of Warsaw (PL))
    28/06/2023, 09:25
  31. Daniel Winney (South China Normal U.)
    28/06/2023, 10:20

    The near threshold region of heavy quarkonium has received a lot of attention with possible applications to a wide breadth of physics. I will discuss the recent JPAC analysis of new Jefferson Lab data from the GlueX and Jpsi-007 experiments. I will discuss the still wide array of physics scenarios that may underpin the near threshold data including strong coupled channel effects to open charm...

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  32. Beijiang Liu
    28/06/2023, 10:45
  33. Dr Peter Hurck (University of Glasgow (GB))
    28/06/2023, 11:10
  34. Philipp Haas (Technische Universitaet Muenchen (DE))
    28/06/2023, 11:40
  35. Mr Zehua Xu (LPC Clermont CNRS/IN2P3 (FR))
    28/06/2023, 12:10
  36. Gagik Gavalian (Jefferson National Lab)
    28/06/2023, 14:00
  37. Matthew McEneaney
    28/06/2023, 14:25
  38. Fernando Torales Acosta (Lawrence Berkeley National Lab)
    28/06/2023, 14:50