English

Beam Charge Asymmetries for Deeply Virtual Compton Scattering on the Proton at CLAS12

Nuclear Experiment 2023-11-14 v2 High Energy Physics - Experiment

Abstract

The parameterization of the nucleon structure through Generalized Parton Distributions (GPDs) shed a new light on the nucleon internal dynamics. For its direct interpretation, Deeply Virtual Compton Scattering (DVCS) is the golden channel for GPDs investigation. The DVCS process interferes with the Bethe-Heitler (BH) mechanism to constitute the leading order amplitude of the eNeNγeN \to eN\gamma process. The study of the epγep\gamma reaction with polarized positron and electron beams gives a complete set of unique observables to unravel the different contributions to the epγep \gamma cross section. This separates the different reaction amplitudes, providing a direct access to their real and imaginary parts which procures crucial constraints on the model dependences and associated systematic uncertainties on GPDs extraction. The real part of the BH-DVCS interference amplitude is particularly sensitive to the DD-term which parameterizes the Gravitational Form Factors of the nucleon. The separation of the imaginary parts of the interference and DVCS amplitudes provides insights on possible higher-twist effects. We propose to measure the unpolarized and polarized Beam Charge Asymmetries (BCAs) of the e±pe±pγ\vec{e}^{\pm}p \to e^{\pm}p \gamma process on an unpolarized hydrogen target with {\tt CLAS12}, using polarized positron and electron beams at 10.6 GeV. The azimuthal and tt-dependences of the unpolarized and polarized BCAs will be measured over a large (xB,Q2)(x_B,Q^2) phase space using a 100 day run with a luminosity of 0.66×1035\times 10^{35}cm2^{-2}\cdots1^{-1}.

Keywords

Cite

@article{arxiv.2309.14041,
  title  = {Beam Charge Asymmetries for Deeply Virtual Compton Scattering on the Proton at CLAS12},
  author = {E. Voutier and V. Burkert and S. Niccolai and R. Paremuzyan and A. Afanasev and J. -S. Alvarado-Galeano and M. Atoui and L. Barion and M. Battaglieri and J. Bernauer and A. Bianconi and M. Bondi and W. Briscoe and A. Camsonne and R. Capobianco and A. Celentano and P. Chatagnon and T. Chetry and G. Ciullo and P. Cole and M. Contalbrigo and G. Costantini and M. Defurne and A. Deur and R. De Vita and S. Diehl and R. Dupré and L. Elouadrhiri and I. Fernando and A. Filippi and T. Forest and F. -X. Girod and G. Gosta and J. Grames and P. Gueye and S. Habet and M. Hattawy and D. Higinbotham and A. Hobart and C. Hyde and K. Joo and A. Kim and V. Klimenko and V. Kubarovsky and M. Leali and P. Lenisa and D. Marchand and L. Marsicano and V. Mascagna and D. Matamoros and M. McCaughan and B. McKinnon and S. Migliorati and H. S. Mitra and A. Movsisyan and C. Muñoz-Camacho and M. Osipenko and M. Ouillon and L. Pappalardo and B. Pasquini and E. Pasyuk and N. Pilleux and M. Poelker and B. Raue and M. Ripani and R. Santos and A. Schmidt and R. Singh and D. Sokhan and M. Spreafico and P. Stoler and I. Strakovsky and M. Taiuti and L. Venturelli and P. -K. Wang and X. Wei and Z. Zhao and the CLAS Collaboration and the Jefferson Lab Positron Working Group},
  journal= {arXiv preprint arXiv:2309.14041},
  year   = {2023}
}

Comments

Proposal to the Jefferson Lab Program Advisory Committee (PAC51)