| 1. | An energy calibration instrument based on uc os - h 的电能校验仪的研究 |
| 2. | The energy calibration is around 1 . 1 mev per channel for oxygen ion and iron ions when energy deposition is less than 50 mev in each detector 从重离子的能谱中我们可以看到,在半导体探测器中的能量沉积大于50mev时,将引起电荷灵敏前置放大器饱和。 |
| 3. | The linear least square fit is used in energy calibration and geometry calibration , and the nonlinear least square fit is used in peak fitting and region fitting 其中能量刻度与几何刻度时采用了线性最小二乘法,而能峰拟合与谱段拟合时采用了非线性最小二乘法。 |
| 4. | The in - flight energy calibration system for hxmt was developed and verified by experiment . several factors that affect its performance were discussed 摘要提出了用于硬x射线调制望远镜的能谱标定方案,并进行了原理实验验证,同时讨论了影响能谱标定系统性能的几个因素。 |
| 5. | The scintillation csi was also calibrated with protons of 15 , 20 , 23 mev . the average energy calibration is 1 . 047 mev per channel . energy calibration for heavy ions was completed with multiplication factor 1 / 12 . 75 根据能量刻度实验的结果,我们对四种带电粒子进行了测试,方法是首先计算粒子的总能量,确定该粒子所属的能区并计算e ,根据e一e方法来鉴别带电粒子的种类。 |
| 6. | The irradiation experimental results show that the resolution of thin detector e1 is higher than that of other thick detectors for ex - particles and protons detection . energy calibration for a - particles was completed with multiplication factor 1 / 3 . energy calibrations of a - particles in detector e1 and e1 , are 0 . 107 mev and 0 . 123 mev per channel , respectively 质子能量刻度采用1档,每道能量h约在0 . 0167mev道,但是在e _ 1探测器中的能量刻度随着能量的增加略有所下降,这是由于高能质子伴随有较多的核反应道对粒子探测产生了干扰,从而增加了在e _ 1探测器中的能量沉积道数,使得每道能量略有所下降,另一个因素可能是探测器厚度的不均匀性的影响,但这并不影响对粒子的鉴别。 |
| 7. | The energy calibration is more accuracy and almost constant with the injected energy of proton . however , the energy calibration in e1 detector has a slight decrease with increasing the energy of protons . the reasons are attributed to the non - uniformity in thickness and disturbing from surrounding r , b ray and secondary particles 对氧离子的能量刻度采用的是l八2 . 75的挡别,在能量范围o一50mev有很好的线性关系,刻度出的每道能量h是1 . 1mev /道,然而当束流能量达到80mev /道时,在e ,探测器中h值与前面能量点的数据符合较好,但在e :探测器中沉积能量高于50mev时,电子学系统进入饱和状态。 |