Jing Z, Huda W, Walker J K
Department of Radiology, University of Florida, Gainesville 32610-0374, USA.
Med Phys. 1998 Jul;25(7 Pt 1):1111-7. doi: 10.1118/1.598433.
Monte Carlo simulations were used to quantify the amount of scattered radiation a scanning slot detector geometry designed for use in digital mammography. Ratios of the scatter to primary (S/P) x-ray photon energy absorbed in the detector were obtained for a Lucite phantom, and were investigated as a function of photon energy, phantom thickness, and slot detector width. Over a Lucite phantom thickness range of 2-6 cm, the S/P ratios range from about 0.10 to 0.17 for a 4 mm wide slot detector at the x-ray photon energies used in mammography. These ratios increased by a factor of approximately 1.8 when the slot width was increased to 10 mm. In general, 20 keV photons gave S/P ratios similar to those of a 30 kVp x-ray spectrum (Mo target + 30 microns Mo filtration). The use of a 3 cm air gap reduced the S/P ratios by a factor of between 2.5 and 3.4, depending on the phantom thickness. For a constant primary energy fluence, coherent scatter was reduced as photon energy increased, whereas Compton scatter increased with increasing photon energy. With no air gap, the contributions of coherent and Compton scatter were found to be equal at 25 keV, whereas the introduction of a 3 cm air gap resulted in equal contributions for the two scatter processes at 36 keV. A 10 mm wide slot detector consisting of a 36.7 mg/cm2 thick Gd2O2S:Tb phosphor screen was compared to an ideal detector absorbing all incident primary/scatter photons. Average differences in the S/P ratios for these two detectors were 7% with no air gap and approximately 4% with a 3 cm air gap. The results obtained in this study will assist in the design of an optimal slot detector for use in digital mammography.
采用蒙特卡罗模拟来量化一种设计用于数字乳腺摄影的扫描狭缝探测器几何结构的散射辐射量。针对一种有机玻璃体模,获得了探测器中吸收的散射与原发射线光子能量的比值(S/P),并研究了该比值随光子能量、体模厚度和狭缝探测器宽度的变化情况。在乳腺摄影所用的X射线光子能量下,对于一个4毫米宽的狭缝探测器,在2至6厘米厚的有机玻璃体模厚度范围内,S/P比值约为0.10至0.17。当狭缝宽度增加到10毫米时,这些比值增加了约1.8倍。一般来说,20千电子伏的光子给出的S/P比值与30千伏峰值X射线光谱(钼靶 + 30微米钼滤过)的比值相似。使用3厘米的气隙可使S/P比值降低2.5至3.4倍,具体取决于体模厚度。对于恒定的原发射线能量注量,相干散射随光子能量增加而减少,而康普顿散射随光子能量增加而增加。在没有气隙的情况下,发现相干散射和康普顿散射在25千电子伏时的贡献相等,而引入3厘米的气隙后,这两个散射过程在36千电子伏时的贡献相等。将一个由36.7毫克/平方厘米厚的Gd2O2S:Tb磷光屏组成的10毫米宽狭缝探测器与一个吸收所有入射原发射线/散射光子的理想探测器进行了比较。这两种探测器的S/P比值平均差异在没有气隙时为7%,在有3厘米气隙时约为4%。本研究获得的结果将有助于设计用于数字乳腺摄影的最佳狭缝探测器。