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碲化镉X射线探测器在强辐照下的信号形成与衰减

Signal formation and decay in CdTe x-ray detectors under intense irradiation.

作者信息

Jahnke A, Matz R

机构信息

Siemens Corporate Technology, Munich, Germany.

出版信息

Med Phys. 1999 Jan;26(1):38-48. doi: 10.1118/1.598475.

Abstract

The response of Cd(Zn)Te Schottky and resistive detectors to intense x-rays is investigated in a commercial computed tomography (CT) system to assess their potential for medical diagnostics. To describe their signal height, responsivity, signal-to-noise ratio (SNR), and detective quantum efficiency the devices are modeled as solid-state ionization chambers with spatially varying electric field and charge collection efficiency. The thicknesses and pixel areas of the discrete detector elements are 0.5-2 mm and a few mm2, respectively. The incident spectrum extends from 26 to 120 keV and comprises 10(10) quanta/s cm2. It photogenerates a carrier concentration in the semiconductor that is two to three orders of magnitude above the intrinsic concentration, but remains to a similar extent below the charge densities on the device electrodes. Stable linear operation is achieved with the Schottky-type devices under high bias. Their behavior can be modeled well if negatively charged near-midgap bulk defects with a concentration of 10(11)-10(13) cm-3 are assumed. The bulk defects explain the amount and time constant (about 100 ms) of the detrapping current measured after x-ray pulses (afterglow). To avoid screening by the trapped space charge the bias voltage should exceed 100(V) x [detector thickness/mm]2. Dark currents are of the order of the generation-recombination current, i.e., 300 pA/mm3 detector volume. With proper device design the signal height approaches the theoretical maximum of 0.2 A/W. This high responsivity, however, is not exploited in CT since the SNR is determined here by the incident quantum noise. As a consequence of the detrapping current, the response speed does not meet CT requirements. A medium-term effort for crystal growth appears necessary to achieve the required reduction of the trap density by an order of magnitude. Scintillation based detectors are, therefore, still preferred in fast operating medical diagnostic systems.

摘要

在商用计算机断层扫描(CT)系统中研究了碲镉锌(Cd(Zn)Te)肖特基探测器和电阻探测器对强X射线的响应,以评估它们在医学诊断方面的潜力。为了描述它们的信号高度、响应度、信噪比(SNR)和探测量子效率,将这些器件建模为具有空间变化电场和电荷收集效率的固态电离室。离散探测器元件的厚度和像素面积分别为0.5 - 2毫米和几平方毫米。入射光谱范围从26 keV到120 keV,包含10(10)个量子/(秒·平方厘米)。它在半导体中产生的载流子浓度比本征浓度高两到三个数量级,但在类似程度上仍低于器件电极上的电荷密度。肖特基型器件在高偏压下实现了稳定的线性操作。如果假设存在浓度为10(11)-10(13)立方厘米-3的带负电的近能隙体缺陷,则可以很好地模拟它们的行为。这些体缺陷解释了X射线脉冲后(余辉)测量的去俘获电流的大小和时间常数(约100毫秒)。为了避免被俘获的空间电荷屏蔽,偏置电压应超过100(伏)×[探测器厚度/毫米]2。暗电流约为产生 - 复合电流的量级,即300皮安/立方毫米探测器体积。通过适当的器件设计,信号高度接近理论最大值0.2安/瓦。然而,在CT中并未利用这种高响应度,因为这里的SNR由入射量子噪声决定。由于去俘获电流,响应速度不符合CT要求。为了将陷阱密度按数量级降低到所需水平,似乎需要进行中期的晶体生长努力。因此,在快速运行的医学诊断系统中,基于闪烁的探测器仍然更受青睐。

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