论文标题

使用$ν_μ$ $ $ $ $ geverrent横截面的核乳液检测器的第一次测量

First measurement using a nuclear emulsion detector of the $ν_μ$ charged-current cross section on iron around the 1$\,$GeV energy region

论文作者

Oshima, H., Matsuo, T., Ali, A., Aoki, S., Berns, L., Fukuda, T., Hanaoka, Y., Hayato, Y., Hiramoto, A., Ichikawa, A. K., Kawahara, H., Kikawa, T., Komatani, R., Komatsu, M., Kuretsubo, K., Marushima, T., Matsumoto, H., Mikado, S., Minamino, A., Mizuno, K., Morimoto, Y., Morishima, K., Naganawa, N., Naiki, M., Nakamura, M., Nakamura, Y., Nakano, N., Nakano, T., Nakaya, T., Nishio, A., Odagawa, T., Ogawa, S., Rokujo, H., Sato, O., Shibuya, H., Sugimura, K., Suzui, L., Suzuki, Y., Takagi, H., Takahashi, S., Takao, T., Tanihara, Y., Watanabe, R., Yamada, K., Yasutome, K., Yokoyama, M.

论文摘要

我们使用暴露于J-PARC中微子设施中T2K中微子束的乳液检测器对铁进行了$ν_μ$充电的交互测量。数据样本对应于目标上的4.0 $ \ times $ 10 $^{19} $质子,中微子平均能量为1.49 $ \,$ GEV。乳液检测器适用于在中微子铁相互作用中产生的带有较低动量阈值的带电颗粒的精确测量,这要归功于薄层的结构和$ $ $ $ $ M $ M的空间分辨率。成功检测到带电的颗粒,并使用乳液检测器测量其多重性。横截面的测量为$σ^{\ Mathrm {fe}} _ {\ Mathrm {cc}}} =(1.28 \ pm 0.11({\ Mathrm {stat。}}}}}}) 10^{ - 38} \,{\ mathrm {cm}}}^{2}/{\ mathrm {nucleon}} $。在有限的诱导Muons的有限运动相空间中的横截面,$θ_μ<45^{\ circ} $和$p_μ> 400 \,{\ rm mev}/c $,on Iron为$σ^{\ mathrm {fe Mathrm {fe}} _ {fe}} _ { \ hspace {0.5mm} space}}} =(0.84 \ pm 0.07({\ mathrm {stat。}}}) {\ Mathrm {cm}}}^{2}/{\ mathrm {nucleon}} $。横截面结果与使用相同光束线通过不同技术获得的先前值一致,并且通过当前的中微子相互作用模型很好地复制了它们。这些结果证明了检测器在1 $ \,$ GEV能量区域周围中微子核相互作用的详细测量中的能力。

We have carried out $ν_μ$ charged-current interaction measurement on iron using an emulsion detector exposed to the T2K neutrino beam in the J-PARC neutrino facility. The data samples correspond to 4.0$\times$10$^{19}$ protons on target, and the neutrino mean energy is 1.49$\,$GeV. The emulsion detector is suitable for precision measurements of charged particles produced in neutrino-iron interactions with a low momentum threshold thanks to thin-layered structure and sub-$μ$m spatial resolution. The charged particles are successfully detected, and their multiplicities are measured using the emulsion detector. The cross section was measured to be $σ^{\mathrm{Fe}}_{\mathrm{CC}} = (1.28 \pm 0.11({\mathrm{stat.}})^{+0.12}_{-0.11}({\mathrm{syst.}})) \times 10^{-38} \, {\mathrm{cm}}^{2}/{\mathrm{nucleon}}$. The cross section in a limited kinematic phase space of induced muons, $θ_μ < 45^{\circ}$ and $p_μ > 400 \, {\rm MeV}/c$, on iron was $σ^{\mathrm{Fe}}_{\mathrm{CC \hspace{1mm} phase \hspace{0.5mm} space}} = (0.84 \pm 0.07({\mathrm{stat.}})^{+0.07}_{-0.06}({\mathrm{syst.}})) \times 10^{-38} \, {\mathrm{cm}}^{2}/{\mathrm{nucleon}}$. The cross-section results are consistent with previous values obtained via different techniques using the same beamline, and they are well reproduced by current neutrino interaction models. These results demonstrate the capability of the detector towards the detailed measurements of the neutrino-nucleus interactions around the 1$\,$GeV energy region.

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