Matscheko G, Carlsson G A, Ribberfors R
Department of Radiation Physics, University of Linköping, Sweden.
Phys Med Biol. 1989 Feb;34(2):199-208. doi: 10.1088/0031-9155/34/2/004.
The overall performance of a Compton spectrometer and, in particular, its energy resolution are investigated both experimentally and theoretically for different scattering materials. Using low-Z (less than or equal to 8) scatterers of moderate sizes (scatterer diameter d less than or equal to 5 mm), there are negligible disturbances due to coherent and/or multiple scattering at 90 degrees scattering angle and photon energies above 20 keV. Two factors contribute to decreasing the energy resolution compared with that in direct measurements: (i) the velocity distribution of the electrons in the scatterer and (ii) the scattering geometry. Of these, (i) is dominant for photon energies less than or equal to 100 keV. The optimal scattering material is a metal of as low Z as possible, i.e. beryllium. However, polyethylene and lucite are normally sufficiently good scatterers. The scattering geometry may become the dominating factor decreasing energy resolution at high photon energies hv greater than or equal to 150 keV.
针对不同的散射材料,对康普顿光谱仪的整体性能,尤其是其能量分辨率进行了实验和理论研究。使用中等尺寸(散射体直径d≤5mm)的低Z(小于或等于8)散射体,在90度散射角和高于20keV的光子能量下,相干和/或多次散射引起的干扰可忽略不计。与直接测量相比,有两个因素导致能量分辨率降低:(i)散射体中电子的速度分布和(ii)散射几何结构。其中,(i)在光子能量小于或等于100keV时占主导地位。最佳的散射材料是尽可能低Z的金属,即铍。然而,聚乙烯和有机玻璃通常是足够好的散射体。在高光子能量hv≥150keV时,散射几何结构可能成为降低能量分辨率的主导因素。