Contribution List

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  1. Franziska Hagelstein, Randolf Pohl (University of Mainz)
    26/06/2023, 10:00
  2. Jorge Moreno (Max-Planck-Institut für Quantenoptik)
    26/06/2023, 11:00
  3. Kjeld Eikema (Vrije Universiteit Amsterdam)
    26/06/2023, 11:30
  4. Pauline YZOMBARD (Laboratoire Kastler Brossel, Sorbonne Université, CNRS, ENS, College de France)
    26/06/2023, 12:00
  5. Prof. Stephan Schiller (Heinrich-Heine-Universität Düsseldorf)
    26/06/2023, 16:30
  6. Jeroen Koelemeij (Vrije Universiteit Amsterdam)
    26/06/2023, 17:00
  7. Daniel Kienzler (ETH Zurich)
    26/06/2023, 17:30
  8. Andreas Knecht (Paul Scherrer Institut)
    27/06/2023, 09:00
  9. Frederik Wauters
    27/06/2023, 09:30
  10. Thomas Richardson
    27/06/2023, 10:00
  11. Vadim Lensky (JGU Mainz)
    27/06/2023, 11:00
  12. Yang Fu (Peking University)
    27/06/2023, 11:30
  13. Simone LiMuli
    27/06/2023, 12:00
  14. Carl Carlson (William & Mary)
    27/06/2023, 14:30
  15. Simon Sirca (U of Ljubljana)
    27/06/2023, 15:00
  16. David Ruth (University of New Hampshire)
    27/06/2023, 15:30
  17. Evgeny Epelbaum (Ruhr University Bochum)
    27/06/2023, 16:30
  18. Niels Walet (University of Manchester)
    27/06/2023, 17:00
  19. Yong-Hui Lin (University of Bonn, HISKP)
    27/06/2023, 17:30
  20. Dmitry Budker
    28/06/2023, 09:00
  21. Anna Viatkina (PTB, Braunschweig; TU Braunschweig)
    28/06/2023, 09:30
  22. Claudia Frugiuele
    28/06/2023, 10:00
  23. Adrian Signer (PSI / UZH)
    28/06/2023, 11:00
  24. Jan Bernauer (Stony Brook University / RIKEN BNL Research Center)
    28/06/2023, 11:30
  25. Tigran Rostomyan (Paul Scherrer Institut)
    28/06/2023, 12:00
  26. Jan Friedrich (TU Munich)
    28/06/2023, 14:30
  27. Michael Kohl (Hampton University)
    28/06/2023, 15:00
  28. Egle Tomasi (IRFU/SPhN)
    28/06/2023, 15:30
  29. Maxim Pospelov (University of Minnesota)
    28/06/2023, 16:30
  30. Sven Sturm (MPIK)
    28/06/2023, 17:00
  31. Yotam Soreq (Technion)
    28/06/2023, 17:30
  32. Krzysztof Pachucki (University of Warsaw)
    29/06/2023, 09:00
    Talk
    QED
  33. Prof. Paul Indelicato (Laboratoire Kastler Brossel-CNRS)
    29/06/2023, 09:30
    Talk
    QED
  34. Michael Eides (University of Kentucky)
    29/06/2023, 10:00
    Talk
    QED
  35. Ashot Gasparian (NC A and T State University)
    29/06/2023, 11:00
  36. Clement Legris (ELPH, Tohoku University (Japan))
    29/06/2023, 11:30
  37. Toshimi Suda (ELPH, Tohoku University)
    29/06/2023, 12:00
  38. Andrea Vacchi (Department of Mathematics, Computer Science and Physics University of Udine & INFN Trieste)
    29/06/2023, 14:30
  39. Prof. Aldo Antognini (ETH Zurich and PSI, Switzerland)
    29/06/2023, 15:00
  40. Ahmed Ouf (JGU Mainz & Paul Scherrer institute)
    29/06/2023, 15:30
  41. Hamza Atac, Nikos Sparveris (Temple University)
    29/06/2023, 16:30
  42. Vahe Sokhoyan
    29/06/2023, 17:00
  43. Kevin McFarland (University of Rochester)
    29/06/2023, 17:30
  44. Mr Miguel Salg (University of Mainz)
    30/06/2023, 09:00
    Talk
  45. Harald Merkel
    30/06/2023, 09:30
    Talk
  46. Mariam ATOUI (IJCLab)
    30/06/2023, 10:00
    Talk
  47. Frank Maas
    30/06/2023, 11:00
    Talk
    PV
  48. Misha Gorshteyn (JGU Mainz)
    30/06/2023, 11:30
    Talk
    PV
  49. Mariam ATOUI (IJCLab)
    Talk

    The internal structure of the nucleon is a field of intensive study. This structure can be experimentally probed through electron elastic scattering off a proton target. This allows the extraction of the proton electric and the magnetic form factors which characterize the charge and the magnetization densities. The spatial moments of the proton charge density are extracted using the electric...

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  50. Vladimir Pascalutsa (JGU Mainz)
  51. Vahe Sokhoyan
    Talk

    Polarizabilities are fundamental properties related to the internal dynamics of the nucleon. They play a crucial role not only in our understanding of the nucleon, but also in other areas such as precision atomic physics. The experimental program performed by the A2 Collaboration at the MAMI accelerator facility in Mainz aims for an accurate extraction of the nucleon polarizabilities using...

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  52. Clement Legris (ELPH, Tohoku University (Japan))
    Talk

    Since 2010, the proton charge radius has been measured using electron scattering, atomic and muonic hydrogen spectroscopy and the results of these measurements tend to fit with a 0.84-fm or 0.88-fm radius. The cause of the discrepancy is not fully understood but some inconsistent results are pointed out: different radii are determined from the same transition of the hydrogen atom (1S-3S) [1,2]...

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  53. Dr Vadim Lensky (JGU Mainz)
  54. Thomas Richardson
    Talk

    Muonic atom spectroscopy provides a precision probe of electroweak physics and possible sources of Beyond the Standard Model physics such as dark matter and the violation of lepton flavor universality. However, uncertainties from nuclear theory are the main bottleneck in calculations of the energy levels for muonic atoms. Therefore, it is necessary to reduce these uncertainties in order to...

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  55. Matthew Bohman (Max Planck Institute for Nuclear Physics)
    Poster

    Molecular hydrogen ions offer a unique opportunity for testing fundamental physics at high precision. As simple three-body systems, the energy levels and properties of H2+, and its isotopologue HD+, are exactly calculable and precision spectroscopy enables measurement of fundamental constants such as the proton-to-electron mass ratio [1], including possible...

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  56. Dr Michael Kohl (Hampton University)
    Talk

    Lepton universality (LU) typically refers to the lepton coupling, which is
    considered to be the same for all charged leptons, if the interaction is
    electroweak according to the Standard Model.
    Lepton universality tests are hence a compelling probe for New Physics.
    I will review the current status of mu-e universality and recent testing
    efforts, with some emphasis on TREK/E36 at J-PARC and...

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  57. Dr Tigran Rostomyan (Paul Scherrer Institut)
    Talk

    The MUon proton Scattering Experiment (MUSE) at the PiM1 beam line of the Paul Scherrer Institute was created a decade ago in response to the Proton Radius Puzzle, the difference observed between muonic hydrogen measurements of the proton charge radius and the existing electronic measurements. To date, MUSE has commissioned its experimental systems to the level needed for the measurements and...

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