User evaluation of detector performance in clinical photon-counting and energy-integrating CT scanners using DICOM images.

IF 3.2
Medical physics Pub Date : 2025-10-01 DOI:10.1002/mp.70045
Ke Li, Xinming Liu, Megan C Jacobsen, John Rong, Corey T Jensen, Eric P Tamm, Frank Dong
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引用次数: 0

Abstract

Background: Clinical users have a critical need to routinely assess the performance of photon-counting detectors (PCDs) in PCD-CT scanners. Such assessments provide insights into detector characteristics, support protocol optimization, and inform decisions on future scanner acquisitions. Historically, this has been challenging due to limited access to raw detector data, which restricts direct evaluation of PCD performance.

Purpose: To evaluate the zero-frequency detective quantum efficiency ( DQE 0 ${\rm DQE}_0$ ) and detector deadtime of PCDs from an end-user perspective using reconstructed DICOM images.

Methods: Detector performance was evaluated on two Siemens NAEOTOM Alpha PCD-CT scanners and one Siemens SOMATOM Force energy-integrating detector CT (EID-CT) scanner. Air-only scans were performed in service mode across a range of tube potentials (70-140 kV) and tube currents (4-1200 mA). DICOM images were reconstructed on the scanner using a linear algorithm with a soft-tissue kernel (Br44). The noise power spectrum (NPS) of the images was used to estimate the mean detector output counts. Mean input photon numbers were estimated based on beam quality and exposure measurements. For the PCD-CT systems, tube current-sweep experiments were used to generate image variance-mA curves, from which detector deadtime was estimated using a previously validated parametric model.

Results: The EID and PCD demonstrated comparable DQE 0 ${\rm DQE}_0$ values (EID: 72%-74%; PCD: 72%-77%). DQE 0 ${\rm DQE}_0$ showed no significant dependence on tube potential. The estimated PCD deadtime ranged from 5.3 to 7.0 ns. Detector performance was consistent across both PCD-CT systems. Additionally, the ultra-high-resolution (UHR) and standard acquisition modes exhibited equivalent deadtime.

Conclusions: The DQE 0 ${\rm DQE}_0$ of the PCD-CT and EID-CT detectors are comparable, with performance primarily limited by geometric efficiency rather than sensor absorption efficiency. Under clinically relevant conditions, pileup-induced count losses in the evaluated PCD-CT scanners are minimal and appear to be effectively corrected by the manufacturer.

使用DICOM图像的临床光子计数和能量积分CT扫描仪中检测器性能的用户评价。
背景:临床用户迫切需要常规评估光子计数检测器(PCDs)在PCD-CT扫描仪中的性能。这样的评估提供了对探测器特性的深入了解,支持协议优化,并为未来的扫描仪获取决策提供信息。从历史上看,由于对原始探测器数据的访问有限,这限制了对PCD性能的直接评估,因此这一直具有挑战性。目的:利用重建的DICOM图像,从终端用户的角度评估pcd的零频率检测量子效率(DQE 0$ {\rm DQE}_0$)和检测器死区时间。方法:对两台西门子NAEOTOM Alpha型PCD-CT和一台西门子SOMATOM Force能量积分检测器CT (EID-CT)进行性能评价。在工作模式下,在管电位(70-140千伏)和管电流(4-1200毫安)范围内进行纯空气扫描。DICOM图像在扫描仪上使用带软组织核(Br44)的线性算法重建。利用图像的噪声功率谱(NPS)估计检测器的平均输出计数。根据光束质量和曝光测量估计平均输入光子数。对于PCD-CT系统,使用管电流扫描实验生成图像方差- ma曲线,利用先前验证的参数模型估计探测器死区时间。结果:EID和PCD具有相当的DQE 0$ {\rm DQE}_0$值(EID: 72%-74%; PCD: 72%-77%)。DQE 0$ {\rm DQE}_0$对管电位无显著依赖性。估计PCD死区时间为5.3 ~ 7.0 ns。在两种PCD-CT系统中,探测器的性能是一致的。此外,超高分辨率(UHR)和标准采集模式具有相同的死区时间。结论:PCD-CT与EID-CT探测器的DQE 0$ {\rm DQE}_0$具有可比性,其性能主要受几何效率而非传感器吸收效率的限制。在临床相关条件下,在评估的PCD-CT扫描仪中,堆积引起的计数损失是最小的,并且似乎可以由制造商有效地纠正。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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