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[26] 2.5 MeV质子反冲边缘用钴-60和铯-137单能g射线源[24]测定.对255通道能量定标,发现2.5 MeV阈值处于通道40附近,14 MeV的肩部在通道110附近.位于LS探测器面附近的2×106中子/s Pu-Be同位素源的探测效率为～5×10-3.修正LS探测器与空化区的实际距离(～5～7 cm),此效率得出的估算效率为1～2×10-4

[27] 微音器固定于烧杯径向的相对两侧.气泡脉冲产生的频率为15～35个脉冲/s以上,根据调谐状态而定.各气泡脉冲的激波踪迹持续～5 ms

[28] 使用Beckman LS6500闪烁计数器,标定至探测T的5～18 keV b射线衰变

[29] 用PMT(岛津R212,2 ns上升时间)进行的SL探测随偏压而强烈变化.在-300 V处每10 s探测到一次SL闪光.只在-450 V偏压处,探测到约1～5次闪光/s.在中子产生期间,只有在-450 V偏压时发生PNG运转造成的伪SL闪光;SL闪光的时间谱[25]表明记录下的SL闪光约有30%在PNG运转期间产生.

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