Bulletin of the American Physical Society
5th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Volume 63, Number 12
Tuesday–Saturday, October 23–27, 2018; Waikoloa, Hawaii
Session 1WEB: Proton Charge Radius Puzzle II
11:00 AM–12:30 PM,
Tuesday, October 23, 2018
Hilton
Room: King's 1
Chair: Ashot Gasparian, NC AT&T State University
Abstract ID: BAPS.2018.HAW.1WEB.3
Abstract: 1WEB.00003 : Elastic electron-proton scattering with low-energy electron beam at ELPH*
12:00 PM–12:30 PM
Presenter:
Yuki Honda
(ELPH, Tohoku Univ.)
Authors:
Yuki Honda
(ELPH, Tohoku Univ.)
Taihei Aoyagi
(ELPH, Tohoku Univ.)
Keita Kasama
(ELPH, Tohoku Univ.)
Hidetoshi Kikunaga
(ELPH, Tohoku Univ.)
Yukie Maeda
(Miyazaki University)
Manabu Miyabe
(ELPH, Tohoku Univ.)
Toshiya Muto
(ELPH, Tohoku Univ.)
Kazuki Namba
(ELPH, Tohoku Univ.)
Ken'ichi Nanbu
(ELPH, Tohoku Univ.)
Shoichi Sasaki
(Tohoku University)
Toshimi Suda
(ELPH, Tohoku Univ.)
Ken Takahashi
(ELPH, Tohoku Univ.)
Shota Takayama
(ELPH, Tohoku Univ.)
Tadaaki Tamae
(Tohoku University)
Atsushi Tokiyasu
(ELPH, Tohoku Univ.)
Kyo Tsukada
(ELPH, Tohoku Univ.)
Natsuki Tsukamoto
(Tohoku University)
Electron scattering is a very powerful tool to study the structure of nuclei. The proton, which is the most fundamental nucleus, has also been investigated by electron scattering for more than half century. In recent years, it becomes clear that the proton charge radius determined by muonic hydrogen spectroscopy is 4% (7 SD) smaller than that determined from electron scattering and hydrogen spectroscopy. This is called the proton radius puzzle.
The electron elastic scattering cross section depends on the charge and magnetic form factors (GE(Q2), GM(Q2)), where Q2 is the four momentum transfer. The charge radius is defined by the gradient of the GE(Q2) at Q2 = 0. We will carry out the e+p elastic scattering experiment in ultra-low Q2 region (Q2=0.0003-0.008 (GeV/c)2) at ELPH, Tohoku University. The accelerator at ELPH provides a low-energy (E=20-60 MeV) electron beam. It makes possible to do the Rosenbluth separation which separates the GE(Q2) and GM(Q2) experimentally. In our Q2 region, the change in the GE(Q2) is only about 2 %, thus, we aim at performing the measurements with systematic uncertainty around 10-3. To cancel the ambiguity in luminosity and solid angle, the e+p and e+C scatterings will be measured simultaneously by using a polyethylene ([CH2]n) target. Because the e+C has been measured very precisely, the absolute cross sections for the e+p can be determined from the ratio of those.
A spectrometer for the low-energy electrons and a new beam line for the experiment are under construction. In my presentation, I will talk about the details and preparation status of our experiment.
*This work was supported by JSPS KAKENHI Grant Numbers JP16H06340 and JP18K13553
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.HAW.1WEB.3
Follow Us |
Engage
Become an APS Member |
My APS
Renew Membership |
Information for |
About APSThe American Physical Society (APS) is a non-profit membership organization working to advance the knowledge of physics. |
© 2024 American Physical Society
| All rights reserved | Terms of Use
| Contact Us
Headquarters
1 Physics Ellipse, College Park, MD 20740-3844
(301) 209-3200
Editorial Office
100 Motor Pkwy, Suite 110, Hauppauge, NY 11788
(631) 591-4000
Office of Public Affairs
529 14th St NW, Suite 1050, Washington, D.C. 20045-2001
(202) 662-8700