Ottawa Medical Physics Institute and Department of Physics, Carleton University, 1125 Colonel By Drive, Ottawa, Ontario K1S 5B6, Canada.
Phys Med Biol. 2010 Feb 7;55(3):855-71. doi: 10.1088/0031-9155/55/3/020. Epub 2010 Jan 14.
The material-dependent x-ray scattering properties of amorphous substances such as tissues and phantom materials used in imaging are determined by their scattering form factors, measured as a function of the momentum transfer argument, x. Incoherent scattering form factors, F(inc), are calculable for all values of x while coherent scattering form factors, F(coh), cannot be calculated except at large x because of their dependence on long-range order. As a result, measuring F(coh) is very important to the developing field of x-ray scatter imaging. Previous measurements of F(coh), based on crystallographic techniques, have shown significant variability, as these techniques are not optimal for amorphous materials. We have developed an energy-dispersive technique that uses a polychromatic x-ray beam and an energy-sensitive detector. We show that F(coh) can be measured directly, with no scaling parameters, by computing the ratio of two spectra: the first, measured at a given scattering angle and the second, the direct transmission spectrum with no scattering. Experiments have been constructed on this principle and used to measure F(coh) for water and polyethylene to explore the reliability of the technique. A 121 kVp x-ray spectrum and seven different scattering angles between 1.67 and 15.09 degrees were used, resulting in a measurable range of x between 0.5 and 9.5 nm(-1). These are the first measurements of F(coh) made without the need for a scaling factor. Resolution in x varies between 10% for small scattering angles and 2% for large scattering angles. Accuracy in F(coh) is shown to be strongly dependent on the precision of the experimental geometry and varies between 5% and 15%. Comparison with previous published measurements for water shows values of the average absolute relative difference between 8% and 14%.
物质的 X 射线散射性质取决于其散射形态因子,这些因子是作为动量传递参数 x 的函数来测量的。非相干散射形态因子 F(inc)可以计算出所有 x 值,而相干散射形态因子 F(coh)则不能计算,除非在 x 很大时,因为它们取决于长程有序。因此,测量 F(coh)对于 X 射线散射成像这一正在发展的领域非常重要。以前基于晶体学技术的 F(coh)测量显示出很大的可变性,因为这些技术对非晶材料不是最优的。我们开发了一种能量色散技术,该技术使用多色 X 射线束和能量敏感探测器。我们表明,可以通过计算两个光谱的比值来直接测量 F(coh),无需缩放参数:第一个光谱是在给定散射角下测量的,第二个光谱是没有散射的直接透射光谱。根据这一原理构建了实验,并用于测量水和聚乙烯的 F(coh),以探索该技术的可靠性。使用了 121 kVp X 射线光谱和 1.67 到 15.09 度之间的七个不同散射角,从而在 0.5 到 9.5 nm(-1)之间产生了可测量的 x 值范围。这些是无需缩放因子即可进行的 F(coh)首次测量。x 的分辨率在小散射角下为 10%,在大散射角下为 2%。F(coh)的准确性强烈依赖于实验几何形状的精度,在 5%到 15%之间变化。与水的以前发表的测量值相比,平均绝对相对差在 8%到 14%之间。