Fredin P, Boreman G D
Appl Opt. 1995 Nov 1;34(31):7179-82. doi: 10.1364/AO.34.007179.
It is desirable for design purposes to model a signal-processing-in-the-element (SPRITE) detector simply as a discrete-element detector with an integration-enhanced D*. We present a method for normalization of measured D* for SPRITE detectors to yield an equivalent-discrete D*. The multiplicative factor is the square root of the ratio of two noise-equivalent bandwidths: one is that of the SPRITE detector with no boost filter, and the other is that of the SPRITE detector with a boost filter that approximately compensates for carrier diffusion, yielding a spatial resolution that approaches that of a discrete detector the same size as the readout. This approach allows a resolution-equivalent D* comparison of SPRITE detectors with discrete-element detectors and facilitates such comparisons among SPRITE detectors. We find that, to obtain the D* of an equivalent-discrete detector, a measured SPRITE D* should typically be multiplied by a factor ranging from 0.85 to 0.57 for 8- to 12-µm SPRITE detectors and by a factor ranging from 0.50 to 0.23 for 3- to 5-µm SPRITE detectors.
出于设计目的,理想的做法是将元件内信号处理(SPRITE)探测器简单地建模为具有积分增强D的离散元件探测器。我们提出了一种对SPRITE探测器测量的D进行归一化的方法,以得到等效离散D*。乘法因子是两个噪声等效带宽之比的平方根:一个是没有增强滤波器的SPRITE探测器的噪声等效带宽,另一个是具有近似补偿载流子扩散的增强滤波器的SPRITE探测器的噪声等效带宽,其产生的空间分辨率接近与读出部分尺寸相同的离散探测器的空间分辨率。这种方法允许对SPRITE探测器和离散元件探测器进行分辨率等效的D比较,并便于在SPRITE探测器之间进行此类比较。我们发现,为了获得等效离散探测器的D,对于8至12μm的SPRITE探测器,测量的SPRITE D*通常应乘以0.85至0.57的因子;对于3至5μm的SPRITE探测器,应乘以0.50至0.23的因子。