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光子计数六边形像素阵列碲化镉探测器:图像引导介入应用的空间分辨率特性

Photon-counting hexagonal pixel array CdTe detector: Spatial resolution characteristics for image-guided interventional applications.

作者信息

Vedantham Srinivasan, Shrestha Suman, Karellas Andrew, Shi Linxi, Gounis Matthew J, Bellazzini Ronaldo, Spandre Gloria, Brez Alessandro, Minuti Massimo

机构信息

Department of Radiology, University of Massachusetts Medical School, Worcester, Massachusetts 01655.

Istituto Nazionale di Fisica Nucleare (INFN), Pisa 56127, Italy and Pixirad Imaging Counters s.r.l., L. Pontecorvo 3, Pisa 56127, Italy.

出版信息

Med Phys. 2016 May;43(5):2118. doi: 10.1118/1.4944868.

Abstract

PURPOSE

High-resolution, photon-counting, energy-resolved detector with fast-framing capability can facilitate simultaneous acquisition of precontrast and postcontrast images for subtraction angiography without pixel registration artifacts and can facilitate high-resolution real-time imaging during image-guided interventions. Hence, this study was conducted to determine the spatial resolution characteristics of a hexagonal pixel array photon-counting cadmium telluride (CdTe) detector.

METHODS

A 650 μm thick CdTe Schottky photon-counting detector capable of concurrently acquiring up to two energy-windowed images was operated in a single energy-window mode to include photons of 10 keV or higher. The detector had hexagonal pixels with apothem of 30 μm resulting in pixel pitch of 60 and 51.96 μm along the two orthogonal directions. The detector was characterized at IEC-RQA5 spectral conditions. Linear response of the detector was determined over the air kerma rate relevant to image-guided interventional procedures ranging from 1.3 nGy/frame to 91.4 μGy/frame. Presampled modulation transfer was determined using a tungsten edge test device. The edge-spread function and the finely sampled line spread function accounted for hexagonal sampling, from which the presampled modulation transfer function (MTF) was determined. Since detectors with hexagonal pixels require resampling to square pixels for distortion-free display, the optimal square pixel size was determined by minimizing the root-mean-squared-error of the aperture functions for the square and hexagonal pixels up to the Nyquist limit.

RESULTS

At Nyquist frequencies of 8.33 and 9.62 cycles/mm along the apothem and orthogonal to the apothem directions, the modulation factors were 0.397 and 0.228, respectively. For the corresponding axis, the limiting resolution defined as 10% MTF occurred at 13.3 and 12 cycles/mm, respectively. Evaluation of the aperture functions yielded an optimal square pixel size of 54 μm. After resampling to 54 μm square pixels using trilinear interpolation, the presampled MTF at Nyquist frequency of 9.26 cycles/mm was 0.29 and 0.24 along the orthogonal directions and the limiting resolution (10% MTF) occurred at approximately 12 cycles/mm. Visual analysis of a bar pattern image showed the ability to resolve close to 12 line-pairs/mm and qualitative evaluation of a neurovascular nitinol-stent showed the ability to visualize its struts at clinically relevant conditions.

CONCLUSIONS

Hexagonal pixel array photon-counting CdTe detector provides high spatial resolution in single-photon counting mode. After resampling to optimal square pixel size for distortion-free display, the spatial resolution is preserved. The dual-energy capabilities of the detector could allow for artifact-free subtraction angiography and basis material decomposition. The proposed high-resolution photon-counting detector with energy-resolving capability can be of importance for several image-guided interventional procedures as well as for pediatric applications.

摘要

目的

具有快速成帧能力的高分辨率、光子计数、能量分辨探测器,可促进在无像素配准伪影的情况下同时采集减影血管造影的对比前和对比后图像,并有助于在图像引导介入过程中进行高分辨率实时成像。因此,本研究旨在确定六边形像素阵列光子计数碲化镉(CdTe)探测器的空间分辨率特性。

方法

一个厚度为650μm的CdTe肖特基光子计数探测器,能够同时采集多达两幅能量窗口图像,以单能量窗口模式运行,包括10keV及以上的光子。该探测器具有六边形像素,其边心距为30μm,在两个正交方向上的像素间距分别为60μm和51.96μm。该探测器在IEC-RQA5光谱条件下进行表征。在与图像引导介入程序相关的空气比释动能率范围为1.3nGy/帧至91.4μGy/帧内,确定探测器的线性响应。使用钨边缘测试装置确定预采样调制传递函数。边缘扩展函数和精细采样的线扩展函数考虑了六边形采样,由此确定预采样调制传递函数(MTF)。由于具有六边形像素的探测器需要重新采样为方形像素以实现无失真显示,通过最小化方形和六边形像素的孔径函数的均方根误差,直至奈奎斯特极限,来确定最佳方形像素大小。

结果

在沿边心距方向和垂直于边心距方向的奈奎斯特频率分别为8.33和9.62周期/mm时,调制因子分别为0.397和0.228。对于相应的轴,定义为10%MTF的极限分辨率分别出现在13.3和12周期/mm处。对孔径函数的评估得出最佳方形像素大小为54μm。使用三线性插值重新采样为54μm方形像素后,在奈奎斯特频率9.26周期/mm处,沿正交方向的预采样MTF分别为0.29和0.24,极限分辨率(10%MTF)出现在约12周期/mm处。对条形图案图像的视觉分析表明能够分辨接近12线对/mm,对神经血管镍钛诺支架的定性评估表明在临床相关条件下能够可视化其支柱。

结论

六边形像素阵列光子计数CdTe探测器在单光子计数模式下提供高空间分辨率。在重新采样为最佳方形像素大小以实现无失真显示后,空间分辨率得以保留。探测器的双能量能力可实现无伪影的减影血管造影和基物质分解。所提出的具有能量分辨能力的高分辨率光子计数探测器对于多种图像引导介入程序以及儿科应用可能具有重要意义。

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