Mizuta Masayoshi, Sanada Shigeru, Akazawa Hiroyuki, Kasai Toshifumi, Abe Shuji, Ikeno Yasuhiro, Mitou Shigeki
Department of Radiology, University Hospital, Kyoto Prefectural University of Medicine, 465 Kajii-cho, Kawaramachi-Hirokoji, Kamigyo-ku, Kyoto 602-8566, Japan.
Radiol Phys Technol. 2012 Jan;5(1):46-52. doi: 10.1007/s12194-011-0134-1. Epub 2011 Oct 5.
Our purpose in this study was to establish a selection standard for anti-scatter grids for a direct conversion flat-panel detector (FPD) system. As indices for grid evaluation, we calculated the selectivity, Bucky factor, and the signal-to-noise ratio improvement factor (SIF) by measuring rates of scatter transmission, primary transmission, and total transmission (based on the digitally displayed measurement values of the FPD system), using 4 acrylic phantoms of different thicknesses. The results showed that the SIF was less than 1.0 when the phantom thickness was 5 cm. When the phantom thickness was 25 cm and the grid ratio was 16:1, the SIF was 1.505 and 1.518 (maximum value) at 90 and 120 kV, respectively. Compared with the grid ratio of 12:1, the SIF at the grid ratio 16:1 was improved by 6.1% at 90 kV, and by 7.0% at 120 kV. In a direct-conversion FPD system, the grid ratio of 16:1 is considered adequate for eliminating the scattered-radiation effect when much scattered radiation is present, such as with a thick imaged object or a high X-ray tube voltage.
本研究的目的是为直接转换平板探测器(FPD)系统建立防散射格栅的选择标准。作为格栅评估指标,我们使用4个不同厚度的丙烯酸体模,通过测量散射传输率、一次传输率和总传输率(基于FPD系统的数字显示测量值)来计算选择性、滤线栅因子和信噪比改善因子(SIF)。结果表明,当体模厚度为5 cm时,SIF小于1.0。当体模厚度为25 cm且格栅比为16:1时,在90 kV和120 kV时,SIF分别为1.505和1.518(最大值)。与格栅比为12:1相比,格栅比为16:1时,在90 kV时SIF提高了6.1%,在120 kV时提高了7.0%。在直接转换FPD系统中,当存在大量散射辐射时,如成像物体较厚或X射线管电压较高时,16:1的格栅比被认为足以消除散射辐射效应。