Denoising of 4D dynamic PET images using spatiotemporal regularization with integrated temporal restoration (SPRINTER).

IF 3.5 2区 医学 Q2 RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING
Hamed Yousefi, Mahdjoub Hamdi, Yujie Wang, Biwen Wang, Richard Laforest, Matthew Brier, Yasheng Chen, Hongyu An
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引用次数: 0

Abstract

Purpose: High-quality 4D dynamic PET imaging is often compromised by noise, especially in low-count frames, which limits clinical utility and quantitative accuracy. This study proposes a novel spatiotemporal denoising method (SPRINTER) that integrates anatomical priors, self-supervised adaptive principal component analysis (aPCA), and deep learning to enhance image quality and preserve time activity fidelity without relying on ground-truth data.

Methods: The method combines anatomically guided aPCA-based temporal smoothing with a supervised 3D ResUNet for spatial denoising. The resulting high signal-to-noise ratio, spatially denoised images are iteratively refined using a temporal regularization strategy to enhance contrast. The model was trained using brain scan datasets from 220 participants who were administered one of the following PET/MRI radiotracers: 18F-AV45, 18F-FDG, 15O-HO, 15O-OO, and 11C-PiB for generalizability testing. Evaluations were performed on synthetic simulations with known ground-truth data and real acquired brain scan data. We compared the proposed method against multiple baseline approaches, including conventional reconstruction (OSEM), spatial-only and temporal-only denoising strategies, and two unsupervised reference methods: Non-Local Means (NLM) filtering, a classical denoising approach, and Noise2Void (N2V). These baselines were selected to reflect both conventional and recent unsupervised deep learning denoising paradigms applicable to PET imaging. Performance was assessed using both synthetic simulations with known ground truth and real acquired PET data. In addition to voxel-level image quality metrics, the impact of denoising on downstream quantitative analysis was evaluated using Ki parametric imaging derived from simulation data. This enabled direct assessment of tracer kinetic estimation accuracy across different denoising strategies.

Results: We compared SPRINTER with OSEM, spatial-only, temporal-only, and two existing unsupervised denoising approaches, including NLM and Noise2Void. Across both simulation and acquired datasets, SPRINTER significantly outperformed all comparison methods (p < 0.05, ANOVA with Bonferroni multiple comparison corrections). The largest gains were observed for the noisiest data using 15O-HO and 15O-OO tracers, where SPRINTER achieved marked SNR improvements in acquired data (e.g., 15O-HO: 3.92 ± 1.28 vs. 2.68 ± 1.24; p = 0.096; 15O-OO: 3.71 ± 1.79 vs. 2.53 ± 1.15 for NLM; p = 0.082). These improvements were consistently superior to those obtained with NLM and Noise2Void, which showed either spatial blurring or limited performance in low-count frames. In simulation studies, SPRINTER significantly reduced voxel-wise reconstruction error compared to all baselines (NRMSE: 0.07 ± 0.04 and 0.09 ± 0.05 vs. 0.33 ± 0.08 to 0.07 and 0.37 ± 0.31 for NLM; p < 0.0001), while also outperforming NLM and Noise2Void, which exhibited higher residual error and reduced temporal consistency. Importantly, contrast was preserved and enhanced, with improved CNR particularly in 1⁸F-FDG and 11C-PiB (e.g., 1⁸F-FDG: 0.37 ± 0.33 vs. 0.18 ± 0.19; p < 0.0001; 11C-PiB: 0.54 ± 0.08 vs. 0.41 ± 0.12; p < 0.001), indicating effective denoising without loss of biologically relevant signal. While NLM and spatial-only methods achieved comparable SNR improvements, this was largely driven by oversmoothing. In contrast, with a similar level of SNR enhancement, the incorporation of temporal information further improved structural fidelity, as reflected by higher SSIM values across all tracers in simulation data (e.g., 1⁸F-AV45: 0.73 ± 0.14 vs. 0.17 ± 0.08 for NLM; p < 0.0001).

Conclusion: This study introduces a robust, self-supervised spatiotemporal denoising method for 4D dynamic PET imaging of the brain. SPRINTER spatiotemporal denoising leverages anatomical guidance and temporal dynamics to enhance spatial clarity and temporal consistency. Its radiotracer-agnostic design and rigorous self-supervision make it well-suited for clinical applications where high-quality reference data are unavailable.

基于时空正则化和综合时间恢复的四维动态PET图像去噪。
目的:高质量的四维动态PET成像经常受到噪声的影响,特别是在低计数帧时,这限制了临床应用和定量准确性。该研究提出了一种新的时空去噪方法(SPRINTER),该方法集成了解剖先验、自监督自适应主成分分析(aPCA)和深度学习,以提高图像质量并保持时间活动保真度,而不依赖于真实数据。方法:该方法结合了解剖引导的基于apca的时间平滑和有监督的三维ResUNet进行空间去噪。由此产生的高信噪比,空间去噪图像迭代细化使用时间正则化策略,以增强对比度。该模型使用来自220名参与者的脑扫描数据集进行训练,这些参与者使用以下PET/MRI示踪剂之一:18F-AV45, 18F-FDG, 15O-HO, 15O-OO和11C-PiB进行泛化测试。利用已知的真值数据和真实获取的脑扫描数据对合成模拟进行了评估。我们将该方法与多种基线方法进行了比较,包括传统重建(OSEM)、纯空间和纯时间去噪策略,以及两种无监督参考方法:非局部均值(NLM)滤波、经典去噪方法和Noise2Void (N2V)。选择这些基线来反映适用于PET成像的传统和最新的无监督深度学习去噪范式。性能评估使用合成模拟与已知的地面真相和真实获得的PET数据。除了体素级图像质量指标外,还使用模拟数据衍生的Ki参数成像来评估去噪对下游定量分析的影响。这使得可以直接评估不同去噪策略的示踪剂动力学估计精度。结果:我们将SPRINTER与OSEM、纯空间、纯时间和两种现有的无监督去噪方法(包括NLM和Noise2Void)进行了比较。在模拟和获取的数据集中,SPRINTER显著优于所有比较方法(p 15O-HO和15O-OO示踪剂),其中SPRINTER在获取的数据中取得了显着的信噪比改善(例如,15O-HO: 3.92±1.28比2.68±1.24;p = 0.096; 15O-OO: 3.71±1.79比2.53±1.15 NLM; p = 0.082)。这些改进始终优于NLM和Noise2Void,后者在低计数帧中显示空间模糊或性能有限。在仿真研究中,短跑运动员显著降低voxel-wise重建误差相比,所有基线(NRMSE: 0.07±0.04,0.09±0.05和0.33±0.08,0.07和0.37±0.31 NLM; p 1⁸F-FDG和11 c-pib(例如,1⁸F-FDG: 0.37±0.33和0.18±0.19;p 11 c-pib: 0.54±0.08和0.41±0.12;p 1⁸F-AV45: NLM 0.73±0.14和0.17±0.08;p结论:本研究引入了一个健壮的、self-supervised时空四维去噪方法动态PET成像的大脑。SPRINTER时空去噪利用解剖指导和时间动态来增强空间清晰度和时间一致性。其放射性示踪不可知的设计和严格的自我监督使其非常适合临床应用,高质量的参考数据是不可用的。
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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来源期刊
EJNMMI Physics
EJNMMI Physics Physics and Astronomy-Radiation
CiteScore
6.70
自引率
10.00%
发文量
78
审稿时长
13 weeks
期刊介绍: EJNMMI Physics is an international platform for scientists, users and adopters of nuclear medicine with a particular interest in physics matters. As a companion journal to the European Journal of Nuclear Medicine and Molecular Imaging, this journal has a multi-disciplinary approach and welcomes original materials and studies with a focus on applied physics and mathematics as well as imaging systems engineering and prototyping in nuclear medicine. This includes physics-driven approaches or algorithms supported by physics that foster early clinical adoption of nuclear medicine imaging and therapy.
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