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Marzec, E.*; 百々 拓; 羽賀 勝洋; 原田 正英; 長谷川 勝一; 春日井 好己; 木下 秀孝; 増田 志歩; 明午 伸一郎; 酒井 健二; et al.
Physical Review Letters, 134, p.081801_1 - 081801_9, 2025/00
被引用回数：0We present the first measurement of the missing energy due to nuclear effects in monoenergetic, muon neutrino charged-current interactions on carbon, originating from 
decay at rest (
), performed with the J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source liquid scintillator based experiment. Toward characterizing the neutrino interaction, ostensibly 
or 
C 
N, we define the missing energy as the energy transferred to the nucleus (
) minus the kinetic energy of the outgoing proton(s), 
, and relate this to visible energy in the detector, ![$$E_m = E_{nu_{mu}} (235.5 MeV) - m_{mu}(105.7 MeV) + [m_n - m_p(1.3 MeV)] - E_{vis}$$](/search/images/ERCV41JAHUQEKX11LRXHKX11LRWXK5L3EAUDEMZVFY0SATLFKYUSALJANVPXWXDNOV4SQMJQGUXDOICNMVLCSIBLEBNW0X1OEAWSA1K5OAUDCLRTEBGWKVRJLUQC0ICFL33XM0LTPUSA.gif)
. The missing energy, which is naively expected to be zero in the absence of nuclear effects (e.g., nucleon separation energy, Fermi momenta, and final-state interactions), is uniquely sensitive to many aspects of the interaction, and has previously been inaccessible with neutrinos. The shape-only, differential cross section measurement reported, based on a 
pure double-coincidence kaon decay-at-rest signal (621 total events), provides detailed insight into neutrino-nucleus interactions, allowing even the nuclear orbital shell of the struck nucleon to be inferred. The measurement provides an important benchmark for models and event generators at hundreds of MeV neutrino energies, characterized by the difficult-to-model transition region between neutrino-nucleus and neutrino-nucleon scattering, and relevant for applications in nuclear physics, neutrino oscillation measurements, and Type-II supernova studies.
spectroscopy via the in-flight 
reaction at the J-PARC K1.8BR川崎 新吾*; 橋本 直; 谷田 聖; 他72名*
JPS Conference Proceedings (Internet), 26, p.022009_1 - 022009_5, 2019/11
The spectral shape of the baryon was measured via the in-flight reaction at the J-PARC K1.8BR beam-line (J-PARC E31). The second E31 physics run was carried out in January and February, 2018. Approximately 
kaons were irradiated on the deuteron target. The missing mass spectrum for the where the residual final-state particles were 
and 
("
" spectrum) was measured for the first time.
(1405) resonance via the reaction at J-PARC浅野 秀光*; 橋本 直; 谷田 聖; 他72名*
AIP Conference Proceedings 2130, p.040018_1 - 040018_6, 2019/07
被引用回数：3 パーセンタイル：78.48(Physics, Nuclear)The structure of the hyperon is an important and long-standing issue related to the 
-nucleus interaction. The J-PARC E31 experiment has been performed to investigate the spectrum shape. Because it is hard to form the directly by a 
scattering in free space, E31 uses the reaction with an incident kaon momentum of 1 GeV/
. We will identify three final states - 
, 
, so that the isospin structure of hyperon resonance states produced can be decomposed. The first physics run of the E31 experiment was performed in 2016. To enhance the statistics of the data set, we have performed the second physics run in the beginning of 2018. During the second run of E31, around kaons impacted on the deuteron target.
