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First Demonstration of a Scintillating Xenon Bubble Chamber for Detecting Dark Matter and Coherent Elastic Neutrino-Nucleus Scattering

机译:闪烁氙气泡室的首次演示   探测暗物质和相干弹性中微子核散射

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摘要

A 30-g xenon bubble chamber, operated at Northwestern University in June andNovember 2016, has for the first time observed simultaneous bubble nucleationand scintillation by nuclear recoils in a superheated liquid. This chamber isinstrumented with a CCD camera for near-IR bubble imaging, a solar-blindphotomultiplier tube to detect 175-nm xenon scintillation light, and apiezoelectric acoustic transducer to detect the ultrasonic emission from agrowing bubble. The time of nucleation determined from the acoustic signal isused to correlate specific scintillation pulses with bubble-nucleating events.We report on data from this chamber for thermodynamic "Seitz" thresholds from4.2 to 15.0 keV. The observed single- and multiple-bubble rates when exposed toa $^{252}$Cf neutron source indicate that, for an 8.3-keV thermodynamicthreshold, the minimum nuclear recoil energy required to nucleate a bubble is$19\pm6$ keV (1$\sigma$ uncertainty). This is consistent with the observedscintillation spectrum for bubble-nucleating events. We see no evidence forbubble nucleation by gamma rays at any of the thresholds studied, setting a 90%C.L. upper limit of $6.3\times10^{-7}$ bubbles per gamma interaction at a4.2-keV thermodynamic threshold. This indicates stronger gamma discriminationthan in CF$_3$I bubble chambers, supporting the hypothesis that scintillationproduction suppresses bubble nucleation by electron recoils while nuclearrecoils nucleate bubbles as usual. These measurements establish thenoble-liquid bubble chamber as a promising new technology for the detection ofweakly interacting massive particle dark matter and coherent elasticneutrino-nucleus scattering.
机译:西北大学于2016年6月和2016年11月运行的30 g氙气气泡室首次观察到过热液体中的核后座力同时使气泡成核和闪烁。该腔室装有用于近红外气泡成像的CCD摄像机,用于检测175 nm氙闪烁光的日光盲光电倍增管和用于检测正在生长的气泡的超声发射的压电声换能器。根据声波信号确定的成核时间可用于将特定的闪烁脉冲与气泡成核事件相关联。我们报告了该腔室的热力学“塞兹”阈值(4.2至15.0 keV)的数据。当暴露于$ ^ {252} $ Cf中子源时观察到的单气泡和多气泡速率表明,对于8.3keV的热力学阈值,使气泡成核所需的最小核反冲能量为$ 19 \ pm6 $ keV(1 $ \ sigma $不确定性)。这与观察到的气泡成核事件的闪烁光谱一致。在设定的90%C.L。下,我们没有发现证据表明在任何研究的阈值下伽马射线都能使气泡成核。在g4.2 keV热力学阈值下,每个伽马相互作用的上限为$ 6.3 \ times10 ^ {-7} $个气泡。这表明比在CF $ -3 $ I气泡腔中强的γ分辨力,支持了闪烁产生抑制电子反冲而使气泡成核而核回旋照常使气泡成核的假说。这些测量结果将稀有液体气泡室确立为一种用于检测弱相互作用的块状暗物质和相干弹性中微子核散射的有前途的新技术。

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