An Unique Application of Pnccd X-Ray Detector in Material Characterization

M. Khan
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Abstract

In the current work, the principle focus is to analyze the measurements of X-rays by the application of Fast Readout Charge-Coupled Device (pnCCD), which is a special form of CCD developed for the purpose of spectroscopy & imaging of X-radiation with high time resolution. As a part of this work, two phases are taken into consideration. In the first phase, highly accelerated electrons induced by high voltage are collided with a metal target (anode material-Mo in this case) in X-ray tube and emitted X-rays from the tube are measured by pnCCD. In this phase, the X-ray spectrum depends on the anode material and accelerating voltage. During the phase 1 experiment, various elements are noticed in the X-ray spectra, which are originated from the experimental apparatus (X-ray tube only) and its surrounding materials. Through proper energy calibration technique, elemental composition of the materials have been determined. In the second phase, fluorescence X-radiation (secondary radiation), emitted by the secondary target source (MnO2) is measured by pnCCD where, Mn is excited by being bombarded with high energy X-rays from X-ray tube. It is to be noted that MnO2 source is guarded by pure Al sheet foil that protects X-rays from other materials. That is why background radiation is decreased and as a result, clean Mn spectrum is observed. To avoid distortion of the intensity determination, the detector’s degree of illumination is maintained less than 2% in both phases by using Al filters with required thickness. In terms of intensity, it can be concluded that the intensity of K X-rays released from MnO2 source is approximately 0.06% in compare to the total intensity of direct emission spectra from experimental apparatus (X-ray tube) for 25 keV.
Pnccd x射线探测器在材料表征中的独特应用
在目前的工作中,主要重点是利用快速读出电荷耦合器件(pnCCD)来分析x射线的测量,pnCCD是一种特殊形式的CCD,用于高时间分辨率的x射线光谱和成像。作为这项工作的一部分,考虑了两个阶段。在第一阶段,高电压诱导的高加速电子与x射线管中的金属靶(阳极材料为mo)碰撞,用pccd测量x射线管发射的x射线。在这个阶段,x射线光谱取决于阳极材料和加速电压。在第一阶段实验中,在x射线光谱中注意到各种元素,这些元素来源于实验装置(仅x射线管)及其周围材料。通过适当的能量校准技术,确定了材料的元素组成。在第二阶段,通过pccd测量由次级靶源(MnO2)发射的荧光x射线(二次辐射),其中Mn被x射线管的高能x射线轰击激发。值得注意的是,MnO2源是由纯铝箔保护的,可以保护x射线不受其他材料的影响。这就是背景辐射减少的原因,因此可以观察到干净的Mn光谱。为了避免强度测定失真,在两相中,通过使用所需厚度的铝滤光片,使探测器的照度保持在2%以下。在强度方面,可以得出MnO2源释放的K x射线强度约为25 keV实验装置(x射线管)直接发射光谱总强度的0.06%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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