8–12 Apr 2024
Maison MINATEC, Grenoble, FRANCE
Europe/Paris timezone

Session

WG2

9 Apr 2024, 08:55
Maison MINATEC, Grenoble, FRANCE

Maison MINATEC, Grenoble, FRANCE

3 Parv. Louis Néel, 38054 Grenoble

Presentation materials

There are no materials yet.

  1. Cristian Baldenegro (Sapienza Università di Roma (IT)), Pieter Taels (University of Antwerp), Renaud Boussarie (CPHT, CNRS, Ecole polytechnique, IP Paris)
    09/04/2024, 09:00
  2. Cesar Da Silva (Los Alamos National Laboratory), Cesar da Silva (Los Alamos National Lab)
    09/04/2024, 09:10
  3. Zhoudunming Tu (BNL)
    09/04/2024, 09:30
  4. Kate Lynch (UC Dublin and Paris-Saclay University IJClab)
    09/04/2024, 09:50
  5. Michael Pitt (Ben Gurion University of the Negev (IL))
    09/04/2024, 11:00
  6. Michal Praszalowicz (Jagiellonian University)
    09/04/2024, 11:20
  7. Anna Stasto (Penn State)
    09/04/2024, 11:40
  8. Tuomas Lappi (University of Jyväskylä)
    09/04/2024, 12:00
  9. Sigtryggur Hauksson (IPhT, CEA, Université Paris-Saclay)
    09/04/2024, 12:20
  10. Francesco Giovanni Celiberto (UAH Madrid)
    09/04/2024, 14:30
  11. Alex Prygarin (Ariel University)
    09/04/2024, 14:50
  12. Dimitri Colferai (University of Florence)
    09/04/2024, 15:10
  13. Afnan Shatat (Universite Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France)
    09/04/2024, 16:00
  14. Guillermo Contreras (Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic), Guillermo Contreras (Czech Technical University in Prague)
    09/04/2024, 16:20
  15. Sanjin Benic (University of Zagreb)
    09/04/2024, 16:40
  16. Maxim Nefedov (IJClab, Orsay)
    09/04/2024, 17:00
  17. Eric Andreas Vivoda (Physics department, Faculty of Science, University of Zagreb)
    09/04/2024, 17:40
  18. Yossathorn Tawabutr (University of Jyväskylä)
    09/04/2024, 18:00
  19. Antonio Riggio (INFN, University of Messina)
    09/04/2024, 18:20
  20. Tobias Toll (IIT Delhi)
    10/04/2024, 09:10
  21. Alexandra Ridzikova
    10/04/2024, 09:30
  22. Pit Duwentäster (University of Jyväskylä)
    10/04/2024, 09:50
  23. Matěj Vaculčiak (Czech Technical University in Prague)
    10/04/2024, 10:10
  24. Andrea Giovanni Riffero (University and INFN Torino (IT))
    10/04/2024, 11:00
  25. Heikki Mäntysaari (University of Jyväskylä)
    10/04/2024, 11:20
  26. David Grund (Czech Technical University in Prague)
    10/04/2024, 11:40
  27. Carlisle Aurabelle Casuga
    10/04/2024, 12:00
  28. Minjung Kim (UC Berkeley)
    10/04/2024, 12:20
  29. Yair Mulian (Saclay CEA)
    10/04/2024, 14:10
  30. Michael Fucilla (Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405, Orsay, France)
    10/04/2024, 14:30
  31. Jamal Jalilian-Marian (Baruch College, City University of New York)
    10/04/2024, 14:50
  32. Alexander Bylinkin (University of Bergen)
    10/04/2024, 15:10
  33. Jose Garrido (Universidad Técnica Federico Santa María)
    10/04/2024, 16:00
  34. Michael Lublinsky
    10/04/2024, 16:20
  35. Piotr Korcyl (Institute of Theoretical Physics, Jagiellonian University)
    10/04/2024, 16:40
  36. Swagato Mukherjee (Brookhaven National Laboratory)
    10/04/2024, 17:00
  37. Jani Penttala (UCLA), Jani Penttala
    10/04/2024, 17:20
  38. Xuanbo Tong
    10/04/2024, 17:40
  39. 10/04/2024, 18:00
  40. Pedro Agostini (NCBJ and IGFAE)
    11/04/2024, 09:10
  41. Guillaume Beuf (National Centre for Nuclear Research (NCBJ), Warsaw), Guillaume Beuf (National Centre for Nuclear Research (NCBJ), Warsaw, Poland), Guillaume Beuf
    11/04/2024, 09:30
  42. M Gabriel Santiago (SURA Center for Nuclear Femtography)
    11/04/2024, 09:50
  43. Swaleha Mulani (National Centre for Nuclear Research (NCBJ), Warsaw, Poland)
    11/04/2024, 10:10
  44. Tobias Toll (IIT Delhi)
    WG2: Small-x, Diffraction and Vector Mesons
    Regular parallel talk

    In colour dipole models, the small-x gluon structure in transverse coordinate space can be described by a so-called thickness function. In unsaturated models this has a straighforward interpretation as the thickness of the proton, while in saturated models it is directly related to the saturation scale. In the hotspot model, this thickness at small magnitudes of the Mandelstam-t variable, is...

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  45. Michael Fucilla (Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405, Orsay, France)
    WG2: Small-x, Diffraction and Vector Mesons
    Regular parallel talk

    The center-of-mass energies available at modern accelerators, such as the Large Hadron Collider (LHC), and at future generation accelerators, such as the Electron-Ion Collider (EIC) and Future Circular Collider (FCC), offer us a unique opportunity to investigate hadronic matter under the most extreme conditions ever reached. One of the most intriguing phenomena of strong interaction is the...

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  46. Francesco Giovanni Celiberto (UAH Madrid)
    WG2: Small-x, Diffraction and Vector Mesons
    Regular parallel talk

    Precision physics in the Higgs sector has been one of the main challenges in recent years. The pure fixed-order calculations entering in the collinear factorization framework, which have been pushed up to N3LO, are not able to describe the entire kinematic spectrum. In particular conditions, they must be necessarily supplemented by all-order resummations; for instance, in the so called Regge...

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  47. Antonio Riggio (INFN, University of Messina)
    WG2: Small-x, Diffraction and Vector Mesons
    Regular parallel talk

    An investigation on η’ photoproduction on quasi-free neutron (Deuterium target) is presented, by showing a preliminary estimation of Beam Asimmetry Σ as function of polar angle in the center-of-mass system near the threshold by analyzing the experimental data of GRAAL experiment. The η’ photoproduction channel is useful because it acts as an isospin filter, allowing to select only resonant...

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  48. Grigorios Chachamis (LIP Lisbon)
  49. Yair Mulian (Saclay CEA)
    WG2: Small-x, Diffraction and Vector Mesons
    Regular parallel talk

    Using the CGC effective theory together with the hybrid factorisation, we study forward photon+jet production in proton-nucleus collisions beyond leading order. We first compute the "real" next-to-leading order (NLO) corrections, i.e. the radiative corrections associated with a three-parton final state, out of which only two are being measured. Then we move to the "virtual" NLO corrections to...

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  50. Maciej Lewicki (Institute of Nuclear Physics, Polish Academy of Sciences, Krakow)
  51. Pit Duwentäster (University of Jyväskylä)
    WG2: Small-x, Diffraction and Vector Mesons
    Regular parallel talk

    With the advent of the Electron-Ion Collider (EIC) and plans for the Large Hadron Electron Collider (LHeC), a clear understanding of the small-x regime of parton distribution functions (PDFs) is becoming increasingly important. In this kinematic region, the PDFs become very large and the linear Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equations are expected to become insufficient to...

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  52. Paul Caucal (Subatech, Nantes Université, IN2P3)
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