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首页> 外文期刊>BARC Report >Effect of instrumental instability and detector parameters in positron annihilation Coincidence Doppler Broadening (CDB) measurements: A Monte Carlo simulation study
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Effect of instrumental instability and detector parameters in positron annihilation Coincidence Doppler Broadening (CDB) measurements: A Monte Carlo simulation study

机译:仪器不稳定性和探测器参数对正电子ni没重合多普勒展宽(CDB)测量的影响:蒙特卡洛模拟研究

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摘要

The momentum distribution of electrons around the site of positron annihilation is studied by Doppler broadening of annihilation radiation. The higher momentum region of Doppler broadening spectra are representative of the element irrespective of its chemical form. Conventional Doppler broadening suffers from poorer sensitivity in terms of elemental specificity due to large Compton background in the higher momentum region. Of late, this problem has been circumvented by the use of two-detector CDB technique. The difference spectra is taken with a gate on sum of the energies E_s to be equal to 2m_0C~2-Eb, where m_0 is the rest mass of electron and E_b is the binding energy of the electron. This reduces the background in the higher momentum region of the spectrum to a great extent, enabling the use of this technique to identify the element with which the positron is annihilating in a given chemical matrix. However, it is essential that the amplitude of the two electronic pulses corresponding to the energies E_(gamma 1) and E_(gamma 2). are exactly matched so that their difference would give the momentum distribution without parallax. Further, the actual annihilation gamma ray energy distribution is broadened by the detector resolution. Hence, it is important to understand the effect of the gain and resolution on the CDB spectra and corresponding information extracted from them.
机译:通过Do灭辐射的多普勒展宽研究了正电子an灭位置周围电子的动量分布。多普勒增宽光谱的较高动量区域代表该元素,无论其化学形式如何。由于在较高动量区域中的大康普顿背景,常规多普勒展宽在元素特异性方面灵敏度较差。最近,通过使用双检测器CDB技术解决了这个问题。差谱是在能量E_s的总和等于2m_0C〜2-Eb的情况下使用门得出的,其中m_0是电子的剩余质量,E_b是电子的结合能。这在很大程度上降低了光谱较高动量区域的背景,从而使该技术的使用可以识别正电子在给定化学基质中被an灭的元素。但是,至关重要的是,两个电子脉冲的幅度分别对应于能量E_(γ1)和E_(γ2)。完全匹配,因此它们的差异将使动量分布没有视差。此外,实际an灭伽马射线能量分布因探测器分辨率而变宽。因此,重要的是要了解增益和分辨率对CDB频谱以及从中提取的相应信息的影响。

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