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Photon-counting X-ray computed tomography using a YAP(Ce)-PMT detector and beam hardening

机译:使用YAP(Ce)-PMT检测器和光束硬化的光子计数X射线计算机断层扫描

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To realize novel photon-counting energy-dispersive X-ray computed tomography (CT), we have developed a low-doseCT scanner using a detector consisting of a cerium-doped yttrium aluminum perovskite [YAP(Ce)] crystal and a smallphotomultiplier tube (PMT). X-ray photons are absorbed by the YAP(Ce) crystal, and negative outputs are produced fromthe PMT. The PMT outputs are amplified by an inverse voltage-to-voltage amplifier, and the event pulses are counted bythe counter with a low threshold energy of 20 keV. First, almost all the photons are counted without the photon-energydependence, since the scintillation-photon number produced by one X-ray photon is proportional to the photon energy.Second, the energy-dispersive imaging is performed using the self-beam hardening by the object. The maximum photoncount of the projection data is determined after the air absorption, and the effective photon energy increases withincreasing digital-amplification factor at the constant maximum count. In the triple-energy CT, the X-ray beam diameterwas 0.5 mm, and the spatial resolutions were approximately 0.3×0.3 mm2. The exposure time for DE-CT was 9.8 min ata total rotation angle of 180°.
机译:为了实现新型的光子计数能量色散X射线计算机断层扫描(CT),我们开发了一种低剂量 CT扫描仪,使用的探测器由掺铈的钇铝钛矿[YAP(Ce)]晶体和一小块 光电倍增管(PMT)。 X射线光子被YAP(Ce)晶体吸收,并且从中产生负输出 PMT。 PMT输出由反向电压电压放大器放大,事件脉冲由 具有20 keV的低阈值能量的计数器。首先,几乎所有的光子都被计算为没有光子能量 因为一个X射线光子产生的闪烁光子数与光子能量成正比,所以它具有一定的依赖性。 第二,利用被摄体的自光束硬化来执行能量色散成像。最大光子 吸收空气后确定投影数据的数量,有效光子能量随 以恒定的最大计数增加数字放大系数。在三能CT中,X射线束直径 分辨率为0.5 mm2,空间分辨率约为0.3×0.3 mm2。 DE-CT的曝光时间为9.8分钟(在 总旋转角度为180°。

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