Williams M B, Simoni P U, Smilowitz L, Stanton M, Phillips W, Stewart A
University of Virginia, Charlottesville 22908, USA.
Med Phys. 1999 Nov;26(11):2273-85. doi: 10.1118/1.598741.
We are developing a modular detector for applications in full field digital mammography and for diagnostic breast imaging. The detector is based on a design that has been refined over the past decade for applications in x-ray crystallography [Kalata et al., Proc. SPIE 1345, 270-279 (1990); Phillips et al. ibid. 2009, 133-138 (1993), Phillips et al., Nucl. Instrum. Methods Phys. Rev. A 334, 621-630 (1993)]. The full field mammographic detector, currently undergoing clinical evaluation, is formed from a 19 cm x 28 cm phosphor screen, read out by a 2 x 3 array of butted charge-coupled device (CCD) modules. Each 2k x 2k CCD is optically coupled to the phosphor via a fiber optic taper with dimensions of 9.4 cm x 9.4cm at the phosphor. This paper describes the imaging performance of a two-module prototype, built using a similar design. In this paper we use cascaded linear systems analysis to develop a model for calculating the spatial frequency dependent noise power spectrum (NPS) and detective quantum efficiency (DQE) of the detector using the measured modulation transfer function (MTF). We compare results of the calculation with the measured NPS and DQE of the prototype. Calculated and measured DQEs are compared over a range of clinically relevant x-ray exposures and kVps. We find that for x-ray photon energies between 10 and 28 keV, the detector gain ranges between 2.5 and 3.7 CCD electrons per incident x-ray, or approximately 5-8 electrons per absorbed x ray. Using a Mo/Mo beam and acrylic phantom, over a detector entrance exposure range of approximately 10 to 80 mR, the volume under the measured 2-d NPS of the prototype detector is proportional to the x-ray exposure, indicating quantum limited performance. Substantial agreement between the calculated and measured values was obtained for the frequency and exposure dependent NPS and DQE over a range of tube voltage from 25 to 30 kVp.
我们正在开发一种模块化探测器,用于全场数字化乳腺摄影及乳腺诊断成像。该探测器基于一种在过去十年中为X射线晶体学应用而不断完善的设计[卡拉塔等人,《国际光学工程学会汇刊》1345卷,第270 - 279页(1990年);菲利普斯等人,同上,2009年,第133 - 138页(1993年),菲利普斯等人,《核仪器与方法:物理研究A》334卷,第621 - 630页(1993年)]。目前正在进行临床评估的全场乳腺摄影探测器由一个19厘米×28厘米的荧光屏构成,通过一个由对接电荷耦合器件(CCD)模块组成的2×3阵列进行读出。每个2k×2k的CCD通过一个在荧光屏处尺寸为9.4厘米×9.4厘米的光纤锥与荧光屏光学耦合。本文描述了采用类似设计构建的双模块原型的成像性能。在本文中,我们使用级联线性系统分析来开发一个模型,以便利用测量的调制传递函数(MTF)计算探测器的空间频率相关噪声功率谱(NPS)和探测量子效率(DQE)。我们将计算结果与原型的测量NPS和DQE进行比较。在一系列临床相关的X射线曝光量和千伏峰值下,对计算得到的和测量得到的DQE进行比较。我们发现,对于10至28千电子伏特之间的X射线光子能量,探测器增益在每入射一个X射线产生2.5至3.7个CCD电子之间,即每吸收一个X射线约产生5至8个电子。使用钼/钼射线束和丙烯酸体模,在探测器入口曝光量约为10至80毫伦琴的范围内,原型探测器测量得到的二维NPS下方的面积与X射线曝光量成正比,表明其性能受量子限制。在25至30千伏峰值的管电压范围内,对于频率和曝光量相关的NPS和DQE,计算值与测量值之间取得了相当程度的一致性。