2021
DOI: 10.1140/epja/s10050-021-00474-z
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Beam charge asymmetries for deeply virtual Compton scattering off the proton

Abstract: The unpolarized and polarized Beam Charge Asymmetries (BCAs) of the e ± p → e ± pγ process off unpolarized hydrogen are discussed. The measurement of BCAs with the CLAS12 spectrometer at the Thomas Jefferson National Accelerator Facility, using polarized positron and electron beams at 10.6 GeV is investigated. This experimental configuration allows to measure azimuthal and tdependences of the unpolarized and polarized BCAs over a large (x B , Q 2 ) phase space, providing a direct access to the real part of the… Show more

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Cited by 18 publications
(8 citation statements)
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“…In this work, we follow the previous setup and extend it to non-zero skewness, which allows us to also include the exclusive measurements in the global analysis. With such a program, we perform the global analysis of GPDs that includes global PDFs [19][20][21], FFs [22] and DVCS measurements from both JLab [9][10][11][12] and previous H1 [37] experiments at Hadron-Electron Ring Accelerator (HERA) along with the relevant lattice calculations related to GPDs [17,23] for the first time.…”
Section: Jhep05(2023)150mentioning
confidence: 99%
See 1 more Smart Citation
“…In this work, we follow the previous setup and extend it to non-zero skewness, which allows us to also include the exclusive measurements in the global analysis. With such a program, we perform the global analysis of GPDs that includes global PDFs [19][20][21], FFs [22] and DVCS measurements from both JLab [9][10][11][12] and previous H1 [37] experiments at Hadron-Electron Ring Accelerator (HERA) along with the relevant lattice calculations related to GPDs [17,23] for the first time.…”
Section: Jhep05(2023)150mentioning
confidence: 99%
“…Several recent breakthroughs have made this possible. Large data sets of exclusive measurements are generated at Jefferson Lab (JLab) [9][10][11][12], and more will come from the planned Electron-Ion Collider (EIC) [13,14] at Brookhaven National Lab (BNL). Additionally, novel developments in lattice QCD allow the access to the nucleon structures from first principle calculation [15][16][17][18], providing information almost impossible to get with current and future experiments.…”
Section: Introductionmentioning
confidence: 99%
“…where ⊕ denotes quadrature addition (a ⊕ b = √ a 2 + b 2 ), an uncorrelated 3% systematic uncertainty has been added [41], and N i is the number of expected BH/DVCS events in the bin. This number of events is given by the product of the luminosity, data taking duration, differential cross-section and phase space volume element.…”
Section: Generation Of Pseudo Datamentioning
confidence: 99%
“…Encoded in this process are the important information of the nucleon such as the mass, angular momentum and mechanical properties [1,4,5] and the three-dimensional structure of the nucleon [6][7][8]. There have been numerous measurements from HERA (H1 [9][10][11][12], ZEUS [13,14] and HERMES [15,16]) and Jefferson Lab (JLab) (CLAS [17][18][19][20][21][22][23][24] and Hall A [25][26][27][28][29]) spanning decades, and more programs are planned in the future such as the JLab 24 GeV, EIcC [30] and EIC [31].…”
Section: Introductionmentioning
confidence: 99%