TY - JOUR
T1 - Measurement of proton, deuteron, triton, and α particle emission after nuclear muon capture on Al, Si, and Ti with the AlCap experiment
AU - Collaboration, AlCap
AU - Edmonds, Andrew
AU - Quirk, John
AU - Wong, Ming-Liang
AU - Alexander, Damien
AU - Daniel, Aji
AU - Diociaiuti, Eleonora
AU - Donghia, Raffaella
AU - Gillies, Ewen L.
AU - Hungerford, Ed V.
AU - Kammel, Peter
AU - Krikler, Benjamin E.
AU - Kuno, Yoshitaka
AU - Lancaster, Mark
AU - Litchfield, R. Phillip
AU - Palladino, Anthony
AU - Repond, Jose
AU - Sato, Akira
AU - Sarra, Ivano
AU - Soleti, Stefano Roberto
AU - Tishchenko, Vladimir
AU - Tran, Nam H.
AU - Uchida, Yoshi
N1 - Funding Information:
The work was supported in part by the Japan Society for the Promotion of Science (JSPS) KAKENHI Grants No. 25000004 and No. 18H0523; the US Department of Energy Office of Science, Office of Nuclear Physics under Award No. DE-FG02-97ER41020; the US Department of Energy, Office of Science, Office of High Energy Physics under Contract No. DE-AC02-05CH11231; and, the Science and Technology Facilities Council, UK.
Publisher Copyright:
© 2022 American Physical Society.
PY - 2022/3/28
Y1 - 2022/3/28
N2 - Background: Heavy charged particles after nuclear muon capture are an important nuclear physics background to the muon-To-electron conversion experiments Mu2e and COMET, which will search for charged lepton flavor violation at an unprecedented level of sensitivity. Purpose: The AlCap experiment aimed to measure the yield and energy spectra of protons, deuterons, tritons, and α particles emitted after the nuclear capture of muons stopped in Al, Si, and Ti in the low-energy range relevant for the muon-To-electron conversion experiments. Methods: Individual charged particle types were identified in layered silicon detector packages and their initial energy distributions were unfolded from the observed energy spectra. Results: The proton yields per muon capture were determined as Yp(Al)=26.64(28stat.)(77syst.)×10-3 and Yp(Ti)=26.48(35)(80)×10-3 in the energy range 3.5-20.0 MeV, and as Yp(Si)=52.5(6)(18)×10-3 in the energy range 4.0-20.0 MeV. Detailed information on yields and energy spectra for all observed nuclei are presented in the paper. Conclusions: The yields in the candidate muon stopping targets, Al and Ti, are approximately half of that in Si, which was used in the past to estimate this background. The reduced background allows for less shielding and a better energy resolution in these experiments. It is anticipated that the comprehensive information presented in this paper will stimulate modern theoretical calculations of the rare process of muon capture with charged particle emission and inform the design of future muon-To-electron conversion experiments.
AB - Background: Heavy charged particles after nuclear muon capture are an important nuclear physics background to the muon-To-electron conversion experiments Mu2e and COMET, which will search for charged lepton flavor violation at an unprecedented level of sensitivity. Purpose: The AlCap experiment aimed to measure the yield and energy spectra of protons, deuterons, tritons, and α particles emitted after the nuclear capture of muons stopped in Al, Si, and Ti in the low-energy range relevant for the muon-To-electron conversion experiments. Methods: Individual charged particle types were identified in layered silicon detector packages and their initial energy distributions were unfolded from the observed energy spectra. Results: The proton yields per muon capture were determined as Yp(Al)=26.64(28stat.)(77syst.)×10-3 and Yp(Ti)=26.48(35)(80)×10-3 in the energy range 3.5-20.0 MeV, and as Yp(Si)=52.5(6)(18)×10-3 in the energy range 4.0-20.0 MeV. Detailed information on yields and energy spectra for all observed nuclei are presented in the paper. Conclusions: The yields in the candidate muon stopping targets, Al and Ti, are approximately half of that in Si, which was used in the past to estimate this background. The reduced background allows for less shielding and a better energy resolution in these experiments. It is anticipated that the comprehensive information presented in this paper will stimulate modern theoretical calculations of the rare process of muon capture with charged particle emission and inform the design of future muon-To-electron conversion experiments.
KW - physics.ins-det
KW - hep-ex
U2 - 10.1103/PhysRevC.105.035501
DO - 10.1103/PhysRevC.105.035501
M3 - Article
SN - 2469-9985
VL - 105
JO - Physical Review C
JF - Physical Review C
IS - 3
M1 - 035501
ER -