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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >Track reconstruction and performance of DRIFT directional dark matter detectors using alpha particles
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Track reconstruction and performance of DRIFT directional dark matter detectors using alpha particles

机译:使用alpha粒子跟踪DRIFT定向暗物质探测器的重建和性能

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First results are presented from an analysis of data from the DRIFT-IIa and DRIFT-IIb directional dark matter detectors at Boulby Mine in which alpha particle tracks were reconstructed and used to characterise detector performance-an important step towards optimising directional technology. The drift velocity in DRIFT-IIa was 59.3 ± 0.2 (stat) ± 7.5 (sys)ms~(-1) based on an analysis of naturally occurring alpha-emitting background. The drift velocity in DRIFT-IIb was 57 ± 1 (stat) ± 3 (sys)ms~(-1) determined by the analysis of alpha particle tracks from a ~(210)Po source. Three-dimensional range reconstruction and range spectra were used to identify alpha particles from the decay of ~(222)Rn, ~(218)Po, ~(220)Rn and ~(216)Po. This study found that (22 ± 2)% of ~(218)Po progeny (from ~(222)Rn decay) did not plate out and remained suspended in the 40 Torr CS_2 gas fill until they decayed. A likely explanation for this is that some of the polonium progeny are produced in an uncharged state. For ~(216)Po progeny (from ~(220)Rn decay) the undeposited fraction was apparently much higher at (100_(-35)~(+0)% most likely due to a shorter lifetime, causing a larger fraction of the progeny to decay whilst drifting to the cathode plane. This explanation implies a much slower drift time for positively charged polonium progeny compared to CS_2~- ions.
机译:通过对Boulby矿DRIFT-IIa和DRIFT-IIb定向暗物质探测器的数据进行分析,得出了初步结果,其中重建了α粒子轨道并用于表征探测器性能,这是优化定向技术的重要一步。根据对自然产生的α发射背景的分析,DRIFT-IIa中的漂移速度为59.3±0.2(stat)±7.5(sys)ms〜(-1)。 DRIFT-IIb中的漂移速度为57±1(标准)±3(sys)ms〜(-1),这是通过分析来自〜(210)Po源的α粒子轨迹确定的。三维距离重建和距离光谱用于根据〜(222)Rn,〜(218)Po,〜(220)Rn和〜(216)Po的衰减来识别α粒子。这项研究发现〜(218)Po后代的22%(2±2)%(来自〜(222)Rn衰变)没有沉积出来,并一直悬浮在40 Torr CS_2气体填充物中,直到它们腐烂为止。对此的可能解释是某些the子代是在不带电荷的状态下产生的。对于〜(216)Po后代(从〜(220)Rn衰减而来),未沉积的分数明显更高,最有可能是(100 _(-35)〜(+0)%,这是由于寿命较短,造成了更大的分数。当CS_2〜-离子带正电荷的lon后代漂移时,其后代的衰变时间要慢得多。

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