Bak G, Choi J H, Jang H I, Jang J S, Jeon S H, Joo K K, Ju K, Jung D E, Kim J G, Kim J H, Kim J Y, Kim S B, Kim S Y, Kim W, Kwon E, Lee D H, Lee H G, Lee Y C, Lim I T, Moon D H, Pac M Y, Park Y S, Rott C, Seo H, Seo J W, Seo S H, Shin C D, Yang J Y, Yoo J, Yu I
Institute for Universe and Elementary Particles, Chonnam National University, Gwangju 61186, Korea.
Institute for High Energy Physics, Dongshin University, Naju 58245, Korea.
Phys Rev Lett. 2019 Jun 14;122(23):232501. doi: 10.1103/PhysRevLett.122.232501.
We report a fuel-dependent reactor electron antineutrino (ν[over ¯]{e}) yield using six 2.8 GW{th} reactors in the Hanbit nuclear power plant complex, Yonggwang, Korea. The analysis uses 850 666 ν[over ¯]_{e} candidate events with a background fraction of 2.0% acquired through inverse beta decay (IBD) interactions in the near detector for 1807.9 live days from August 2011 to February 2018. Based on multiple fuel cycles, we observe a fuel ^{235}U dependent variation of measured IBD yields with a slope of (1.51±0.23)×10^{-43} cm^{2}/fission and measure a total average IBD yield of (5.84±0.13)×10^{-43} cm^{2}/fission. The hypothesis of no fuel-dependent IBD yield is ruled out at 6.6σ. The observed IBD yield variation over ^{235}U isotope fraction does not show significant deviation from the Huber-Mueller (HM) prediction at 1.3 σ. The measured fuel-dependent variation determines IBD yields of (6.15±0.19)×10^{-43} and (4.18±0.26)×10^{-43} cm^{2}/fission for two dominant fuel isotopes ^{235}U and ^{239}Pu, respectively. The measured IBD yield per ^{235}U fission shows the largest deficit relative to the HM prediction. Reevaluation of the ^{235}U IBD yield per fission may mostly solve the reactor antineutrino anomaly (RAA) while ^{239}Pu is not completely ruled out as a possible contributor to the anomaly. We also report a 2.9 σ correlation between the fractional change of the 5 MeV excess and the reactor fuel isotope fraction of ^{235}U.
我们报告了在韩国荣光韩比特核电站综合体中使用六个2.8吉瓦热功率反应堆所得到的与燃料相关的反应堆电子反中微子(ν[上划线]ₑ)产额。该分析使用了850666个ν[上划线]ₑ候选事例,背景份额为2.0%,这些事例是在2011年8月至2018年2月期间,近探测器通过逆β衰变(IBD)相互作用在1807.9个活日中获取的。基于多个燃料循环,我们观察到测量的IBD产额随燃料²³⁵U的变化,斜率为(1.51±0.23)×10⁻⁴³平方厘米/裂变,并测量了总平均IBD产额为(5.84±0.13)×10⁻⁴³平方厘米/裂变。无燃料依赖IBD产额的假设在6.6σ水平被排除。观察到的IBD产额随²³⁵U同位素丰度的变化在1.3σ水平上与休伯 - 米勒(HM)预测没有显著偏差。测量的与燃料相关的变化分别确定了两种主要燃料同位素²³⁵U和²³⁹Pu的IBD产额为(6.15±0.19)×10⁻⁴³和(4.18±0.26)×10⁻⁴³平方厘米/裂变。每²³⁵U裂变测量的IBD产额相对于HM预测显示出最大的亏缺。对每裂变²³⁵U的IBD产额进行重新评估可能大部分解决反应堆反中微子异常(RAA)问题,而²³⁹Pu作为异常的可能贡献者并未被完全排除。我们还报告了5兆电子伏特过剩的分数变化与²³⁵U反应堆燃料同位素丰度之间存在2.9σ的相关性。