论文标题

部分可观测时空混沌系统的无模型预测

Puzzling time properties of proportional electroluminescence in two-phase argon detectors for dark matter searches

论文作者

Buzulutskov, A., Frolov, E., Borisova, E., Nosov, V., Oleynikov, V., Sokolov, A.

论文摘要

贵重气体中的比例电致发光(EL)是一种物理过程,通常用于低能肌粒子体物理学实验中的两相(液体)探测器。在这项工作中,首次系统地研究了两相氩检测器中可见光EL的时间属性。特别是,观察到EL信号中的两个异常的慢速分量,其贡献和时间常数随电场的增加而增加。在两阶段介质中的任何已知的光子和电子发射机理中,这种令人困惑的特性都不是预期的。这些组件的时间常数约为4-5 $μ$ S和50 $ $ $ s。此外,揭示了缓慢组件的特定阈值行为:无论气相密度如何,它们在降低的电场降低4.8 $ \ pm $ 0.2 TD的阈值中出现,该阈值高于标准(优先级)EL的发作约1 TD。 NIR中EL的此阈值和降低的场阈值之间存在明显的相似性,该阈值是通过高原子激发态出现的Ar $^{*}(3p^{5} 4p)$。还观察到了慢组分的意外温度依赖性:它们的贡献随温度而降低,实际上在室温下消失。我们表明,可以在假设的框架中解释慢组分的令人困惑的性能,即由于在亚稳态负氩离子上捕获电子电子,这些假设是在电荷信号本身中产生的。

Proportional electroluminescence (EL) in noble gases is a physical process routinely used in two-phase (liquid-gas) detectors for low-energy astroparticle-physics experiments. In this work, the time properties of visible-light EL in two-phase argon detectors have been systematically studied for the first time. In particular, two unusual slow components in the EL signal, with their contributions and time constants increasing with electric field, were observed. This puzzling property is not expected in any of the known mechanisms of photon and electron emission in two-phase media. Time constants of these components is about 4-5 $μ$s and 50 $μ$s. In addition, a specific threshold behavior of the slow components was revealed: they emerged at a threshold in reduced electric field of 4.8 $\pm$ 0.2 Td regardless of the gas phase density, which is about 1 Td above the onset of standard (excimer) EL. There is a conspicuous similarity between this threshold and reduced field threshold of EL in NIR occurring via higher atomic excited states Ar$^{*}(3p^{5}4p)$. An unexpected temperature dependence of slow components was also observed: their contribution decreased with temperature, practically disappearing at room temperature. We show that the puzzling properties of slow components can be explained in the framework of hypothesis that these are produced in the charge signal itself due to trapping of drifting electrons on metastable negative argon ions.

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