Munro P, Bouius D C
Department of Oncology, University of Western Ontario, London, Canada.
Med Phys. 1998 May;25(5):689-702. doi: 10.1118/1.598252.
We have measured the linearity, spatial resolution (MTF), noise (NPS), and signal-to-noise characteristics (DQE) of an electronic portal imaging device (EPID) based on an amorphous silicon flat-panel array. The array has a 128 x 128-pixel matrix and each pixel is 0.75 x 0.75 mm2 in dimension so the array covers an area of 96 x 96 mm2. The array acts like a large area light sensor and records the optical signals generated in a metal plate/phosphor screen x-ray detector when the detector is irradiated by a megavoltage x-ray beam. In addition, approximately 0.5% of the total signal is generated by nonoptical processes. The noise measurements show that the device is quantum noise limited with the noise power generated by the x-ray quanta being up to 100 times greater than the noise added by the external readout electronics and flat-panel light sensor itself. However, the flat-panel light sensor does reduce the spatial resolution (compared to a perfect optical sensor with infinitesimal pixel size) because of its moderate pixel size and because optical spread can occur in the transparent glues used to attach the phosphor screen to the flat-panel light sensor. The response of the sensor is very linear and does not suffer from the glare phenomenon associated with TV camera-based EPIDs--characteristics which suggest that the amorphous silicon EPID will be well suited to transit dosimetry. Nevertheless, some limitations need to be overcome before these devices can be used clinically. These include developing larger flat-panel light sensors, the elimination of "noisy" pixels with high dark signal, and improvements in the uniform sensitivity of the sensors. This last requirement is only needed for transit dosimetry applications where it would greatly simplify calibration of the device. In addition, an image acquisition scheme must be developed to eliminate artifacts created by the pulsed x-ray beam generated by linear accelerators. Despite these limitations, our studies suggest that the amorphous silicon EPIDs are very well suited to portal imaging.
我们已测量了基于非晶硅平板探测器阵列的电子射野影像装置(EPID)的线性度、空间分辨率(调制传递函数,MTF)、噪声(噪声功率谱,NPS)以及信噪特性(量子探测效率,DQE)。该阵列具有128×128像素矩阵,每个像素尺寸为0.75×0.75平方毫米,因此阵列覆盖面积为96×96平方毫米。该阵列就像一个大面积光传感器,当探测器受到兆伏级X射线束照射时,记录在金属板/磷光屏X射线探测器中产生的光信号。此外,总信号的约0.5%由非光学过程产生。噪声测量表明,该装置受量子噪声限制,X射线量子产生的噪声功率比外部读出电子设备和平板光传感器本身添加的噪声大100倍。然而,由于平板光传感器的像素尺寸适中,且在将磷光屏附着到平板光传感器所用的透明胶中会发生光扩散,所以它确实会降低空间分辨率(与具有无限小像素尺寸的理想光学传感器相比)。传感器的响应非常线性,且不存在与基于电视摄像机的EPID相关的眩光现象,这些特性表明非晶硅EPID非常适合用于传输剂量测定。尽管如此,在这些装置能够用于临床之前,还需要克服一些限制。这些限制包括开发更大的平板光传感器、消除具有高暗信号的“噪声”像素以及提高传感器的均匀灵敏度。最后一项要求仅在传输剂量测定应用中需要,因为这将大大简化装置的校准。此外,必须开发一种图像采集方案,以消除由直线加速器产生的脉冲X射线束造成的伪影。尽管存在这些限制,但我们的研究表明,非晶硅EPID非常适合用于射野成像。