Bulletin of the American Physical Society
APS April Meeting 2022
Volume 67, Number 6
Saturday–Tuesday, April 9–12, 2022; New York
Session X10: Electromagnetic Interactions
10:45 AM–12:21 PM,
Tuesday, April 12, 2022
Room: Lyceum
Sponsoring
Unit:
DNP
Chair: Evangeline Downie, George Washington University
Abstract: X10.00005 : PRad II: An Upgraded Electron-Proton Scattering Experiment for High Precision Measurement of the Charge Radius of the Proton at Jefferson Lab*
11:33 AM–11:45 AM
Presenter:
Vladimir Khachatryan
(Duke University)
Author:
Vladimir Khachatryan
(Duke University)
Collaboration:
Vladimir Khachatryan for the PRad Collaboration
The PRad experiment at Jefferson Lab has performed an electron $e-p$ scattering experiment in 2016 by utilizing a magnetic-spectrometer-free approach with a hybrid electromagnetic calorimeter, gas electron multipliers and a windowless hydrogen gas target to measure the proton root-mean-square charge radius, $r_{p}$, with a good accuracy. Although the PRad result, within its experimental uncertainties, was a critical input in the recent revision of the CODATA recommendation for $r_{p}$, the experiment did not reach the highest precision allowed by the calorimetric technique. Besides, the PRad $r_{p}$ value is 5.8\% smaller than that extracted from the most precise electron scattering experiment to date. In order to resolve such a tension with modern $e-p$ scattering results, the PRad collaboration proposed PRad-II (PR12-20-004), an upgraded experiment that was approved by the JLab program advisory committee with the highest scientific rating A. PRad-II has its goal to reach an ultra-high precision in the radius measurement with $\sim 4$ times smaller total uncertainty than what PRad has reported. Furthermore, PRad-II will reach a $Q^{2}$ range of $\sim 10^{-5}\,{\rm (GeV/c)^{2}}$, enabling a more accurate and robust extraction of $r_{p}$. In this talk, we will present how PRad-II will open up a new precision frontier in electron scattering, by discussing a number of critical upgrades to the PRad sub-detectors and DAQ along with improving radiative correction calculations, as well as by discussing how PRad-II will measure $r_{p}$ in general.
*This work is supported in part by the U.S. Department of Energy under Grants No. DE-FG02-03ER41231 and No. DE-AC05-06OR23177, under which the Jefferson Science Associates operates the Thomas Jefferson National Accelerator Facility, and by NSF-MRI grant PHY-1229153.
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