Pub Date : 2024-07-25DOI: 10.1186/s40658-024-00671-x
Alessandra Zorz, Marco Andrea Rossato, Paolo Turco, Luca Maria Colombo Gomez, Andrea Bettinelli, Francesca De Monte, Marta Paiusco, Pietro Zucchetta, Diego Cecchin
Background: The application of semi-conductor detectors such as cadmium-zinc-telluride (CZT) in nuclear medicine improves extrinsic energy resolution and count sensitivity due to the direct conversion of gamma photons into electric signals. A 3D-ring pixelated CZT system named StarGuide was recently developed and implemented by GE HealthCare for SPECT acquisition. The system consists of 12 detector columns with seven modules of 16 × 16 CZT pixelated crystals, each with an integrated parallel-hole tungsten collimator. The axial coverage is 27.5 cm. The detector thickness is 7.25 mm, which allows acquisitions in the energy range [40-279] keV. Since there is currently no performance characterization specific to 3D-ring CZT SPECT systems, the National Electrical Manufacturers Association (NEMA) NU 1-2018 clinical standard can be tailored to these cameras. The aim of this study was to evaluate the performance of the SPECT/CT StarGuide system according to the NEMA NU 1-2018 clinical standard specifically adapted to characterize the new 3D-ring CZT.
Results: Due to the integrated collimator, the system geometry and the pixelated nature of the detector, some NEMA tests have been adapted to the features of the system. The extrinsic measured energy resolution was about 5-6% for the tested isotopes (99mTc, 123I and 57Co); the maximum count rate was 760 kcps and the observed count rate at 20% loss was 917 kcps. The system spatial resolution in air extrapolated at 10 cm with 99mTc was 7.2 mm, while the SPECT spatial resolutions with scatter were 4.2, 3.7 and 3.6 mm in a central, radial and tangential direction respectively. Single head sensitivity value for 99mTc was 97 cps/MBq; with 12 detector columns, the system volumetric sensitivity reached 520 kcps MBq-1 cc-1.
Conclusions: The performance tests of the StarGuide can be performed according to the NEMA NU 1-2018 standard with some adaptations. The system has shown promising results, particularly in terms of energy resolution, spatial resolution and volumetric sensitivity, potentially leading to higher quality clinical images.
{"title":"Performance evaluation of the 3D-ring cadmium-zinc-telluride (CZT) StarGuide system according to the NEMA NU 1-2018 standard.","authors":"Alessandra Zorz, Marco Andrea Rossato, Paolo Turco, Luca Maria Colombo Gomez, Andrea Bettinelli, Francesca De Monte, Marta Paiusco, Pietro Zucchetta, Diego Cecchin","doi":"10.1186/s40658-024-00671-x","DOIUrl":"10.1186/s40658-024-00671-x","url":null,"abstract":"<p><strong>Background: </strong>The application of semi-conductor detectors such as cadmium-zinc-telluride (CZT) in nuclear medicine improves extrinsic energy resolution and count sensitivity due to the direct conversion of gamma photons into electric signals. A 3D-ring pixelated CZT system named StarGuide was recently developed and implemented by GE HealthCare for SPECT acquisition. The system consists of 12 detector columns with seven modules of 16 × 16 CZT pixelated crystals, each with an integrated parallel-hole tungsten collimator. The axial coverage is 27.5 cm. The detector thickness is 7.25 mm, which allows acquisitions in the energy range [40-279] keV. Since there is currently no performance characterization specific to 3D-ring CZT SPECT systems, the National Electrical Manufacturers Association (NEMA) NU 1-2018 clinical standard can be tailored to these cameras. The aim of this study was to evaluate the performance of the SPECT/CT StarGuide system according to the NEMA NU 1-2018 clinical standard specifically adapted to characterize the new 3D-ring CZT.</p><p><strong>Results: </strong>Due to the integrated collimator, the system geometry and the pixelated nature of the detector, some NEMA tests have been adapted to the features of the system. The extrinsic measured energy resolution was about 5-6% for the tested isotopes (<sup>99m</sup>Tc, <sup>123</sup>I and <sup>57</sup>Co); the maximum count rate was 760 kcps and the observed count rate at 20% loss was 917 kcps. The system spatial resolution in air extrapolated at 10 cm with <sup>99m</sup>Tc was 7.2 mm, while the SPECT spatial resolutions with scatter were 4.2, 3.7 and 3.6 mm in a central, radial and tangential direction respectively. Single head sensitivity value for <sup>99m</sup>Tc was 97 cps/MBq; with 12 detector columns, the system volumetric sensitivity reached 520 kcps MBq<sup>-1</sup> cc<sup>-1</sup>.</p><p><strong>Conclusions: </strong>The performance tests of the StarGuide can be performed according to the NEMA NU 1-2018 standard with some adaptations. The system has shown promising results, particularly in terms of energy resolution, spatial resolution and volumetric sensitivity, potentially leading to higher quality clinical images.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"69"},"PeriodicalIF":3.0,"publicationDate":"2024-07-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11272762/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141757808","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-25DOI: 10.1186/s40658-024-00670-y
Min Jeong Cho, Donghwi Hwang, Si Young Yie, Jae Sung Lee
Purpose: Effective radiation therapy requires accurate segmentation of head and neck cancer, one of the most common types of cancer. With the advancement of deep learning, people have come up with various methods that use positron emission tomography-computed tomography to get complementary information. However, these approaches are computationally expensive because of the separation of feature extraction and fusion functions and do not make use of the high sensitivity of PET. We propose a new deep learning-based approach to alleviate these challenges.
Methods: We proposed a tumor region attention module that fully exploits the high sensitivity of PET and designed a network that learns the correlation between the PET and CT features using squeeze-and-excitation normalization (SE Norm) without separating the feature extraction and fusion functions. In addition, we introduce multi-scale context fusion, which exploits contextual information from different scales.
Results: The HECKTOR challenge 2021 dataset was used for training and testing. The proposed model outperformed the state-of-the-art models for medical image segmentation; in particular, the dice similarity coefficient increased by 8.78% compared to U-net.
Conclusion: The proposed network segmented the complex shape of the tumor better than the state-of-the-art medical image segmentation methods, accurately distinguishing between tumor and non-tumor regions.
目的:有效的放射治疗需要对头颈部癌症(最常见的癌症类型之一)进行精确分割。随着深度学习的发展,人们提出了各种利用正电子发射断层扫描-计算机断层扫描获取补充信息的方法。然而,由于特征提取和融合函数分离,这些方法计算成本高昂,而且无法利用正电子发射断层扫描的高灵敏度。我们提出了一种基于深度学习的新方法来缓解这些挑战:我们提出了一种能充分利用 PET 高灵敏度的肿瘤区域关注模块,并设计了一种网络,利用挤压-激发归一化(SE Norm)学习 PET 和 CT 特征之间的相关性,而无需分离特征提取和融合函数。此外,我们还引入了多尺度上下文融合,利用不同尺度的上下文信息:结果:我们使用 HECKTOR 挑战赛 2021 数据集进行训练和测试。在医学图像分割方面,所提出的模型优于最先进的模型;特别是,与 U-net 相比,骰子相似性系数提高了 8.78%:结论:与最先进的医学图像分割方法相比,提出的网络能更好地分割形状复杂的肿瘤,准确区分肿瘤和非肿瘤区域。
{"title":"Multi-modal co-learning with attention mechanism for head and neck tumor segmentation on <sup>18</sup>FDG PET-CT.","authors":"Min Jeong Cho, Donghwi Hwang, Si Young Yie, Jae Sung Lee","doi":"10.1186/s40658-024-00670-y","DOIUrl":"10.1186/s40658-024-00670-y","url":null,"abstract":"<p><strong>Purpose: </strong>Effective radiation therapy requires accurate segmentation of head and neck cancer, one of the most common types of cancer. With the advancement of deep learning, people have come up with various methods that use positron emission tomography-computed tomography to get complementary information. However, these approaches are computationally expensive because of the separation of feature extraction and fusion functions and do not make use of the high sensitivity of PET. We propose a new deep learning-based approach to alleviate these challenges.</p><p><strong>Methods: </strong>We proposed a tumor region attention module that fully exploits the high sensitivity of PET and designed a network that learns the correlation between the PET and CT features using squeeze-and-excitation normalization (SE Norm) without separating the feature extraction and fusion functions. In addition, we introduce multi-scale context fusion, which exploits contextual information from different scales.</p><p><strong>Results: </strong>The HECKTOR challenge 2021 dataset was used for training and testing. The proposed model outperformed the state-of-the-art models for medical image segmentation; in particular, the dice similarity coefficient increased by 8.78% compared to U-net.</p><p><strong>Conclusion: </strong>The proposed network segmented the complex shape of the tumor better than the state-of-the-art medical image segmentation methods, accurately distinguishing between tumor and non-tumor regions.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"67"},"PeriodicalIF":3.0,"publicationDate":"2024-07-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11272764/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141757807","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Background: Low-dose ungated CT is commonly used for total-body PET attenuation and scatter correction (ASC). However, CT-based ASC (CT-ASC) is limited by radiation dose risks of CT examinations, propagation of CT-based artifacts and potential mismatches between PET and CT. We demonstrate the feasibility of direct ASC for multi-tracer total-body PET in the image domain.
Methods: Clinical uEXPLORER total-body PET/CT datasets of [18F]FDG (N = 52), [18F]FAPI (N = 46) and [68Ga]FAPI (N = 60) were retrospectively enrolled in this study. We developed an improved 3D conditional generative adversarial network (cGAN) to directly estimate attenuation and scatter-corrected PET images from non-attenuation and scatter-corrected (NASC) PET images. The feasibility of the proposed 3D cGAN-based ASC was validated using four training strategies: (1) Paired 3D NASC and CT-ASC PET images from three tracers were pooled into one centralized server (CZ-ASC). (2) Paired 3D NASC and CT-ASC PET images from each tracer were individually used (DL-ASC). (3) Paired NASC and CT-ASC PET images from one tracer ([18F]FDG) were used to train the networks, while the other two tracers were used for testing without fine-tuning (NFT-ASC). (4) The pre-trained networks of (3) were fine-tuned with two other tracers individually (FT-ASC). We trained all networks in fivefold cross-validation. The performance of all ASC methods was evaluated by qualitative and quantitative metrics using CT-ASC as the reference.
Results: CZ-ASC, DL-ASC and FT-ASC showed comparable visual quality with CT-ASC for all tracers. CZ-ASC and DL-ASC resulted in a normalized mean absolute error (NMAE) of 8.51 ± 7.32% versus 7.36 ± 6.77% (p < 0.05), outperforming NASC (p < 0.0001) in [18F]FDG dataset. CZ-ASC, FT-ASC and DL-ASC led to NMAE of 6.44 ± 7.02%, 6.55 ± 5.89%, and 7.25 ± 6.33% in [18F]FAPI dataset, and NMAE of 5.53 ± 3.99%, 5.60 ± 4.02%, and 5.68 ± 4.12% in [68Ga]FAPI dataset, respectively. CZ-ASC, FT-ASC and DL-ASC were superior to NASC (p < 0.0001) and NFT-ASC (p < 0.0001) in terms of NMAE results.
Conclusions: CZ-ASC, DL-ASC and FT-ASC demonstrated the feasibility of providing accurate and robust ASC for multi-tracer total-body PET, thereby reducing the radiation hazards to patients from redundant CT examinations. CZ-ASC and FT-ASC could outperform DL-ASC for cross-tracer total-body PET AC.
{"title":"Artificial intelligence-based joint attenuation and scatter correction strategies for multi-tracer total-body PET.","authors":"Hao Sun, Yanchao Huang, Debin Hu, Xiaotong Hong, Yazdan Salimi, Wenbing Lv, Hongwen Chen, Habib Zaidi, Hubing Wu, Lijun Lu","doi":"10.1186/s40658-024-00666-8","DOIUrl":"10.1186/s40658-024-00666-8","url":null,"abstract":"<p><strong>Background: </strong>Low-dose ungated CT is commonly used for total-body PET attenuation and scatter correction (ASC). However, CT-based ASC (CT-ASC) is limited by radiation dose risks of CT examinations, propagation of CT-based artifacts and potential mismatches between PET and CT. We demonstrate the feasibility of direct ASC for multi-tracer total-body PET in the image domain.</p><p><strong>Methods: </strong>Clinical uEXPLORER total-body PET/CT datasets of [<sup>18</sup>F]FDG (N = 52), [<sup>18</sup>F]FAPI (N = 46) and [<sup>68</sup>Ga]FAPI (N = 60) were retrospectively enrolled in this study. We developed an improved 3D conditional generative adversarial network (cGAN) to directly estimate attenuation and scatter-corrected PET images from non-attenuation and scatter-corrected (NASC) PET images. The feasibility of the proposed 3D cGAN-based ASC was validated using four training strategies: (1) Paired 3D NASC and CT-ASC PET images from three tracers were pooled into one centralized server (CZ-ASC). (2) Paired 3D NASC and CT-ASC PET images from each tracer were individually used (DL-ASC). (3) Paired NASC and CT-ASC PET images from one tracer ([<sup>18</sup>F]FDG) were used to train the networks, while the other two tracers were used for testing without fine-tuning (NFT-ASC). (4) The pre-trained networks of (3) were fine-tuned with two other tracers individually (FT-ASC). We trained all networks in fivefold cross-validation. The performance of all ASC methods was evaluated by qualitative and quantitative metrics using CT-ASC as the reference.</p><p><strong>Results: </strong>CZ-ASC, DL-ASC and FT-ASC showed comparable visual quality with CT-ASC for all tracers. CZ-ASC and DL-ASC resulted in a normalized mean absolute error (NMAE) of 8.51 ± 7.32% versus 7.36 ± 6.77% (p < 0.05), outperforming NASC (p < 0.0001) in [<sup>18</sup>F]FDG dataset. CZ-ASC, FT-ASC and DL-ASC led to NMAE of 6.44 ± 7.02%, 6.55 ± 5.89%, and 7.25 ± 6.33% in [<sup>18</sup>F]FAPI dataset, and NMAE of 5.53 ± 3.99%, 5.60 ± 4.02%, and 5.68 ± 4.12% in [<sup>68</sup>Ga]FAPI dataset, respectively. CZ-ASC, FT-ASC and DL-ASC were superior to NASC (p < 0.0001) and NFT-ASC (p < 0.0001) in terms of NMAE results.</p><p><strong>Conclusions: </strong>CZ-ASC, DL-ASC and FT-ASC demonstrated the feasibility of providing accurate and robust ASC for multi-tracer total-body PET, thereby reducing the radiation hazards to patients from redundant CT examinations. CZ-ASC and FT-ASC could outperform DL-ASC for cross-tracer total-body PET AC.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"66"},"PeriodicalIF":3.0,"publicationDate":"2024-07-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11264498/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141723247","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-18DOI: 10.1186/s40658-024-00658-8
Laure Vergnaud, Yuni K Dewaraja, Anne-Laure Giraudet, Jean-Noël Badel, David Sarrut
radiopharmaceutical therapy is a standardized systemic treatment, with a typical dose of 7.4 GBq per injection, but its response varies from patient to patient. Dosimetry provides the opportunity to personalize treatment, but it requires multiple post-injection images to monitor the radiopharmaceutical's biodistribution over time. This imposes an additional imaging burden on centers with limited resources. This review explores methods to lessen this burden by optimizing acquisition types and minimizing the number and duration of imaging sessions. After summarizing the different steps of dosimetry and providing examples of dosimetric workflows for -DOTATATE and -PSMA, we examine dosimetric workflows based on a reduced number of acquisitions, or even just one. We provide a non-exhaustive description of simplified methods and their assumptions, as well as their limitations. Next, we detail the specificities of each normal tissue and tumors, before reviewing dose-response relationships in the literature. In conclusion, we will discuss the current limitations of dosimetric workflows and propose avenues for improvement.
177 Lu 放射性药物治疗是一种标准化的全身治疗方法,每次注射的典型剂量为 7.4 GBq,但其反应因人而异。剂量测定为个性化治疗提供了机会,但它需要多次注射后成像,以监测放射性药物在一段时间内的生物分布。这给资源有限的中心带来了额外的成像负担。本综述探讨了通过优化采集类型、尽量减少成像次数和缩短成像时间来减轻这种负担的方法。在总结了剂量测定的不同步骤并提供了 177 Lu -DOTATATE 和 177 Lu -PSMA 的剂量测定工作流程示例后,我们研究了基于减少采集次数甚至只采集一次的剂量测定工作流程。我们对简化方法及其假设和局限性进行了非详尽的描述。接下来,我们将详细介绍每种正常组织和肿瘤的特异性,然后回顾文献中的剂量-反应关系。最后,我们将讨论目前剂量测定工作流程的局限性,并提出改进途径。
{"title":"A review of 177Lu dosimetry workflows: how to reduce the imaging workloads?","authors":"Laure Vergnaud, Yuni K Dewaraja, Anne-Laure Giraudet, Jean-Noël Badel, David Sarrut","doi":"10.1186/s40658-024-00658-8","DOIUrl":"10.1186/s40658-024-00658-8","url":null,"abstract":"<p><p><math> <mrow><msup><mrow></mrow> <mn>177</mn></msup> <mtext>Lu</mtext></mrow> </math> radiopharmaceutical therapy is a standardized systemic treatment, with a typical dose of 7.4 GBq per injection, but its response varies from patient to patient. Dosimetry provides the opportunity to personalize treatment, but it requires multiple post-injection images to monitor the radiopharmaceutical's biodistribution over time. This imposes an additional imaging burden on centers with limited resources. This review explores methods to lessen this burden by optimizing acquisition types and minimizing the number and duration of imaging sessions. After summarizing the different steps of dosimetry and providing examples of dosimetric workflows for <math> <mrow><msup><mrow></mrow> <mn>177</mn></msup> <mtext>Lu</mtext></mrow> </math> -DOTATATE and <math> <mrow><msup><mrow></mrow> <mn>177</mn></msup> <mtext>Lu</mtext></mrow> </math> -PSMA, we examine dosimetric workflows based on a reduced number of acquisitions, or even just one. We provide a non-exhaustive description of simplified methods and their assumptions, as well as their limitations. Next, we detail the specificities of each normal tissue and tumors, before reviewing dose-response relationships in the literature. In conclusion, we will discuss the current limitations of dosimetric workflows and propose avenues for improvement.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"65"},"PeriodicalIF":3.0,"publicationDate":"2024-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11554969/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141633039","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-17DOI: 10.1186/s40658-024-00664-w
Sejin Ha, Byung Soo Park, Sangwon Han, Jungsu S Oh, Sun Young Chae, Jae Seung Kim, Dae Hyuk Moon
Purpose: To develop a deep learning (DL) model for generating automated regions of interest (ROIs) on 99mTc-diethylenetriamine pentaacetic acid (DTPA) renal scans for glomerular filtration rate (GFR) measurement.
Methods: Manually-drawn ROIs retrieved from a Picture Archiving and Communications System were used as ground-truth (GT) labels. A two-dimensional U-Net convolutional neural network architecture with multichannel input was trained to generate DL ROIs. The agreement between GFR values from GT and DL ROIs was evaluated using Lin's concordance correlation coefficient (CCC) and slope coefficients for linear regression analyses. Bias and 95% limits of agreement (LOA) were assessed using Bland-Altman plots.
Results: A total of 24,364 scans (12,822 patients) were included. Excellent concordance between GT and DL GFR was found for left (CCC 0.982, 95% confidence interval [CI] 0.981-0.982; slope 1.004, 95% CI 1.003-1.004), right (CCC 0.969, 95% CI 0.968-0.969; slope 0.954, 95% CI 0.953-0.955) and both kidneys (CCC 0.978, 95% CI 0.978-0.979; slope 0.979, 95% CI 0.978-0.979). Bland-Altman analysis revealed minimal bias between GT and DL GFR, with mean differences of - 0.2 (95% LOA - 4.4-4.0), 1.4 (95% LOA - 3.5-6.3) and 1.2 (95% LOA - 6.5-8.8) mL/min/1.73 m² for left, right and both kidneys, respectively. Notably, 19,960 scans (81.9%) showed an absolute difference in GFR of less than 5 mL/min/1.73 m².
Conclusion: Our DL model exhibited excellent performance in the generation of ROIs on 99mTc-DTPA renal scans. This automated approach could potentially reduce manual effort and enhance the precision of GFR measurement in clinical practice.
目的:开发一种深度学习(DL)模型,用于在99m锝-二乙烯三胺五乙酸(DTPA)肾脏扫描中自动生成感兴趣区(ROI),以测量肾小球滤过率(GFR):从图片存档和通信系统中手动绘制的 ROI 作为地面实况(GT)标签。对具有多通道输入的二维 U-Net 卷积神经网络架构进行了训练,以生成 DL ROI。使用Lin's concordance correlation coefficient (CCC)和线性回归分析的斜率系数评估GT和DL ROI的GFR值之间的一致性。使用Bland-Altman图评估偏差和95%的一致性界限(LOA):共纳入 24,364 次扫描(12,822 名患者)。左肾(CCC 0.982,95% 置信区间 [CI] 0.981-0.982;斜率 1.004,95% 置信区间 1.003-1.004)、右肾(CCC 0.969,95% 置信区间 0.968-0.969;斜率 0.954,95% 置信区间 0.953-0.955)和双肾(CCC 0.978,95% 置信区间 0.978-0.979;斜率 0.979,95% 置信区间 0.978-0.979)GT 和 DL GFR 的一致性极佳。Bland-Altman分析显示,GT和DL GFR之间的偏差极小,左肾、右肾和双肾的平均差异分别为-0.2(95% LOA - 4.4-4.0)、1.4(95% LOA - 3.5-6.3)和1.2(95% LOA - 6.5-8.8) mL/min/1.73 m²。值得注意的是,有 19,960 次扫描(81.9%)显示 GFR 的绝对差异小于 5 mL/min/1.73 m²:我们的 DL 模型在生成 99mTc-DTPA 肾扫描的 ROI 方面表现出色。这种自动化方法有可能减少人工操作,提高临床实践中 GFR 测量的精确度。
{"title":"Deep learning-based measurement of split glomerular filtration rate with <sup>99m</sup>Tc-diethylenetriamine pentaacetic acid renal scan.","authors":"Sejin Ha, Byung Soo Park, Sangwon Han, Jungsu S Oh, Sun Young Chae, Jae Seung Kim, Dae Hyuk Moon","doi":"10.1186/s40658-024-00664-w","DOIUrl":"10.1186/s40658-024-00664-w","url":null,"abstract":"<p><strong>Purpose: </strong>To develop a deep learning (DL) model for generating automated regions of interest (ROIs) on <sup>99m</sup>Tc-diethylenetriamine pentaacetic acid (DTPA) renal scans for glomerular filtration rate (GFR) measurement.</p><p><strong>Methods: </strong>Manually-drawn ROIs retrieved from a Picture Archiving and Communications System were used as ground-truth (GT) labels. A two-dimensional U-Net convolutional neural network architecture with multichannel input was trained to generate DL ROIs. The agreement between GFR values from GT and DL ROIs was evaluated using Lin's concordance correlation coefficient (CCC) and slope coefficients for linear regression analyses. Bias and 95% limits of agreement (LOA) were assessed using Bland-Altman plots.</p><p><strong>Results: </strong>A total of 24,364 scans (12,822 patients) were included. Excellent concordance between GT and DL GFR was found for left (CCC 0.982, 95% confidence interval [CI] 0.981-0.982; slope 1.004, 95% CI 1.003-1.004), right (CCC 0.969, 95% CI 0.968-0.969; slope 0.954, 95% CI 0.953-0.955) and both kidneys (CCC 0.978, 95% CI 0.978-0.979; slope 0.979, 95% CI 0.978-0.979). Bland-Altman analysis revealed minimal bias between GT and DL GFR, with mean differences of - 0.2 (95% LOA - 4.4-4.0), 1.4 (95% LOA - 3.5-6.3) and 1.2 (95% LOA - 6.5-8.8) mL/min/1.73 m² for left, right and both kidneys, respectively. Notably, 19,960 scans (81.9%) showed an absolute difference in GFR of less than 5 mL/min/1.73 m².</p><p><strong>Conclusion: </strong>Our DL model exhibited excellent performance in the generation of ROIs on <sup>99m</sup>Tc-DTPA renal scans. This automated approach could potentially reduce manual effort and enhance the precision of GFR measurement in clinical practice.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"64"},"PeriodicalIF":3.0,"publicationDate":"2024-07-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11254887/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141626312","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-17DOI: 10.1186/s40658-024-00668-6
Amir Karimzadeh, Linus Schatz, Markus Sauer, Ivayla Apostolova, Ralph Buchert, Susanne Klutmann, Wencke Lehnert
Background: Internal dosimetry in individual patients is essential for safe and effective radioligand therapy. Multiple time point imaging for accurate dosimetry is time consuming and hence can be demanding for nuclear medicine departments as well as patients. The objectives of this study were (1) to assess absorbed doses to organs at risk and tumor lesions for [177Lu]Lu-PSMA-I&T using whole body SPECT imaging and (2) to investigate possible simplified dosimetry protocols.
Methods: This study included 16 patients each treated with 4 cycles of [177Lu]Lu-PSMA-I&T. They underwent quantitative whole body SPECT/CT imaging (3 bed positions) at four time points (TP) comprising 2 h, 24 h, 48 h and 72-168 h post-injection (p.i.). Full 3D dosimetry (reference method) was performed for all patients and dose cycles for organs at risk (kidneys, parotid glands and submandibular glands) and up to ten tumor lesions per patient (resulting in 90 lesions overall). The simplified dosimetry methods (SM) included (1) generating time activity curves for subsequent cycles using a single TP of imaging applying the kinetics of dose cycle 1, and for organs at risk also (2) simple extrapolation from dose cycle 1 and (3) from both, dose cycle 1 and 2.
Results: Normalized absorbed doses were 0.71 ± 0.32 mGy/MBq, 0.28 ± 0.12 mGy/MBq and 0.22 ± 0.08 mGy/MBq for kidneys, parotid glands and submandibular glands, respectively. Tumor doses decreased from 3.86 ± 3.38 mGy/MBq in dose cycle 1 to 2.01 ± 2.65 mGy/MBq in dose cycle 4. Compared to the full dosimetry approach the SM 1 using single TP imaging at 48 h p.i. resulted in the most accurate and precise results for the organs at risk in terms of absorbed doses per cycle and total cumulated dose. For tumor lesions better results were achieved using the fourth TP (≥ 72 h p.i.).
Conclusion: Simplification of safety dosimetry protocols is possible for [177Lu]Lu-PSMA-I&T therapy. If tumor dosimetry is of interest a later imaging TP (≥ 72 h p.i.) should be used/added to account for the slower kinetics of tumors compared to organs at risk.
{"title":"Organ and tumor dosimetry including method simplification for [<sup>177</sup>Lu]Lu-PSMA-I&T for treatment of metastatic castration resistant prostate cancer.","authors":"Amir Karimzadeh, Linus Schatz, Markus Sauer, Ivayla Apostolova, Ralph Buchert, Susanne Klutmann, Wencke Lehnert","doi":"10.1186/s40658-024-00668-6","DOIUrl":"10.1186/s40658-024-00668-6","url":null,"abstract":"<p><strong>Background: </strong>Internal dosimetry in individual patients is essential for safe and effective radioligand therapy. Multiple time point imaging for accurate dosimetry is time consuming and hence can be demanding for nuclear medicine departments as well as patients. The objectives of this study were (1) to assess absorbed doses to organs at risk and tumor lesions for [<sup>177</sup>Lu]Lu-PSMA-I&T using whole body SPECT imaging and (2) to investigate possible simplified dosimetry protocols.</p><p><strong>Methods: </strong>This study included 16 patients each treated with 4 cycles of [<sup>177</sup>Lu]Lu-PSMA-I&T. They underwent quantitative whole body SPECT/CT imaging (3 bed positions) at four time points (TP) comprising 2 h, 24 h, 48 h and 72-168 h post-injection (p.i.). Full 3D dosimetry (reference method) was performed for all patients and dose cycles for organs at risk (kidneys, parotid glands and submandibular glands) and up to ten tumor lesions per patient (resulting in 90 lesions overall). The simplified dosimetry methods (SM) included (1) generating time activity curves for subsequent cycles using a single TP of imaging applying the kinetics of dose cycle 1, and for organs at risk also (2) simple extrapolation from dose cycle 1 and (3) from both, dose cycle 1 and 2.</p><p><strong>Results: </strong>Normalized absorbed doses were 0.71 ± 0.32 mGy/MBq, 0.28 ± 0.12 mGy/MBq and 0.22 ± 0.08 mGy/MBq for kidneys, parotid glands and submandibular glands, respectively. Tumor doses decreased from 3.86 ± 3.38 mGy/MBq in dose cycle 1 to 2.01 ± 2.65 mGy/MBq in dose cycle 4. Compared to the full dosimetry approach the SM 1 using single TP imaging at 48 h p.i. resulted in the most accurate and precise results for the organs at risk in terms of absorbed doses per cycle and total cumulated dose. For tumor lesions better results were achieved using the fourth TP (≥ 72 h p.i.).</p><p><strong>Conclusion: </strong>Simplification of safety dosimetry protocols is possible for [<sup>177</sup>Lu]Lu-PSMA-I&T therapy. If tumor dosimetry is of interest a later imaging TP (≥ 72 h p.i.) should be used/added to account for the slower kinetics of tumors compared to organs at risk.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"63"},"PeriodicalIF":3.0,"publicationDate":"2024-07-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11255161/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141626313","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-15DOI: 10.1186/s40658-024-00669-5
Carlos Vinícius Gomes, Bruno Melo Mendes, Lucas Paixão, Silvano Gnesin, Cristina Müller, Nicholas P van der Meulen, Klaus Strobel, Telma Cristina Ferreira Fonseca, Thiago Viana Miranda Lima
Background: Several research groups have explored the potential of scandium radionuclides for theragnostic applications due to their longer half-lives and equal or similar coordination chemistry between their diagnostic and therapeutic counterparts, as well as lutetium-177 and terbium-161, respectively. Unlike the gallium-68/lutetium-177 pair, which may show different in-vivo uptake patterns, the use of scandium radioisotopes promises consistent behaviour between diagnostic and therapeutic radiopeptides. An advantage of scandium's longer half-life over gallium-68 is the ability to study radiopeptide uptake over extended periods and its suitability for centralized production and distribution. However, concerns arise from scandium-44's decay characteristics and scandium-43's high production costs. This study aimed to evaluate the dosimetric implications of using scandium radioisotopes with somatostatin analogues against gallium-68 for PET imaging of neuroendocrine tumours.
Methods: Absorbed dose per injected activity (AD/IA) from the generated time-integrated activity curve (TIAC) were estimated using the radiopeptides [43/44/44mSc]Sc- and [68Ga]Ga-DOTATATE. The kidneys, liver, spleen, and red bone marrow (RBM) were selected for dose estimation studies. The EGSnrc and MCNP6.1 Monte Carlo (MC) codes were used with female (AF) and male (AM) ICRP phantoms. The results were compared to Olinda/EXM software, and the effective dose concentrations assessed, varying composition between the scandium radioisotopes.
Results: Our findings showed good agreement between the MC codes, with - 3 ± 8% mean difference. Kidneys, liver, and spleen showed differences between the MC codes (min and max) in a range of - 4% to 8%. This was observed for both phantoms for all radiopeptides used in the study. Compared to Olinda/EXM the largest observed difference was for the RBM, of 21% for the AF and 16% for the AM for scandium- and gallium-based radiopeptides. Despite the differences, our findings showed a higher absorbed dose on [43/44Sc]Sc-DOTATATE compared to its 68Ga-based counterpart.
Conclusion: This study found that [43/44Sc]Sc-DOTATATE delivers a higher absorbed dose to organs at risk compared to [68Ga]Ga-DOTATATE, assuming equal distribution. This is due to the longer half-life of scandium radioisotopes compared to gallium-68. However, calculated doses are within acceptable ranges, making scandium radioisotopes a feasible replacement for gallium-68 in PET imaging, potentially offering enhanced diagnostic potential with later timepoint imaging.
{"title":"Comparison of the dosimetry of scandium-43 and scandium-44 patient organ doses in relation to commonly used gallium-68 for imaging neuroendocrine tumours.","authors":"Carlos Vinícius Gomes, Bruno Melo Mendes, Lucas Paixão, Silvano Gnesin, Cristina Müller, Nicholas P van der Meulen, Klaus Strobel, Telma Cristina Ferreira Fonseca, Thiago Viana Miranda Lima","doi":"10.1186/s40658-024-00669-5","DOIUrl":"10.1186/s40658-024-00669-5","url":null,"abstract":"<p><strong>Background: </strong>Several research groups have explored the potential of scandium radionuclides for theragnostic applications due to their longer half-lives and equal or similar coordination chemistry between their diagnostic and therapeutic counterparts, as well as lutetium-177 and terbium-161, respectively. Unlike the gallium-68/lutetium-177 pair, which may show different in-vivo uptake patterns, the use of scandium radioisotopes promises consistent behaviour between diagnostic and therapeutic radiopeptides. An advantage of scandium's longer half-life over gallium-68 is the ability to study radiopeptide uptake over extended periods and its suitability for centralized production and distribution. However, concerns arise from scandium-44's decay characteristics and scandium-43's high production costs. This study aimed to evaluate the dosimetric implications of using scandium radioisotopes with somatostatin analogues against gallium-68 for PET imaging of neuroendocrine tumours.</p><p><strong>Methods: </strong>Absorbed dose per injected activity (AD/IA) from the generated time-integrated activity curve (TIAC) were estimated using the radiopeptides [<sup>43/44/44m</sup>Sc]Sc- and [<sup>68</sup>Ga]Ga-DOTATATE. The kidneys, liver, spleen, and red bone marrow (RBM) were selected for dose estimation studies. The EGSnrc and MCNP6.1 Monte Carlo (MC) codes were used with female (AF) and male (AM) ICRP phantoms. The results were compared to Olinda/EXM software, and the effective dose concentrations assessed, varying composition between the scandium radioisotopes.</p><p><strong>Results: </strong>Our findings showed good agreement between the MC codes, with - 3 ± 8% mean difference. Kidneys, liver, and spleen showed differences between the MC codes (min and max) in a range of - 4% to 8%. This was observed for both phantoms for all radiopeptides used in the study. Compared to Olinda/EXM the largest observed difference was for the RBM, of 21% for the AF and 16% for the AM for scandium- and gallium-based radiopeptides. Despite the differences, our findings showed a higher absorbed dose on [<sup>43/44</sup>Sc]Sc-DOTATATE compared to its <sup>68</sup>Ga-based counterpart.</p><p><strong>Conclusion: </strong>This study found that [<sup>43/44</sup>Sc]Sc-DOTATATE delivers a higher absorbed dose to organs at risk compared to [<sup>68</sup>Ga]Ga-DOTATATE, assuming equal distribution. This is due to the longer half-life of scandium radioisotopes compared to gallium-68. However, calculated doses are within acceptable ranges, making scandium radioisotopes a feasible replacement for gallium-68 in PET imaging, potentially offering enhanced diagnostic potential with later timepoint imaging.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"61"},"PeriodicalIF":3.0,"publicationDate":"2024-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11247068/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141616156","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-15DOI: 10.1186/s40658-024-00667-7
Johan Gustafsson, Erik Larsson, Michael Ljungberg, Katarina Sjögreen Gleisner
Background: The aim was to investigate the noise and bias properties of quantitative 177Lu-SPECT with respect to the number of projection angles, and the number of subsets and iterations in the OS-EM reconstruction, for different total acquisition times.
Methods: Experimental SPECT acquisition of six spheres in a NEMA body phantom filled with 177Lu was performed, using medium-energy collimators and 120 projections with 180 s per projection. Bootstrapping was applied to generate data sets representing acquisitions with 20 to 120 projections for 10 min, 20 min, and 40 min, with 32 noise realizations per setting. Monte Carlo simulations were performed of 177Lu-DOTA-TATE in an anthropomorphic computer phantom with three tumours (2.8 mL to 40.0 mL). Projections representing 24 h and 168 h post administration were simulated, each with 32 noise realizations. Images were reconstructed using OS-EM with compensation for attenuation, scatter, and distance-dependent resolution. The number of subsets and iterations were varied within a constrained range of the product number of iterations number of projections . Volumes-of-interest were defined following the physical size of the spheres and tumours, the mean activity-concentrations estimated, and the absolute mean relative error and coefficient of variation (CV) over noise realizations calculated. Pareto fronts were established by analysis of CV versus mean relative error.
Results: Points at the Pareto fronts with low CV and high mean error resulted from using a low number of subsets, whilst points at the Pareto fronts associated with high CV but low mean error resulted from reconstructions with a high number of subsets. The number of projection angles had limited impact.
Conclusions: For accurate estimation of the 177Lu activity-concentration from SPECT images, the number of projection angles has limited importance, whilst the total acquisition time and the number of subsets and iterations are parameters of importance.
{"title":"Pareto optimization of SPECT acquisition and reconstruction settings for <sup>177</sup>Lu activity quantification.","authors":"Johan Gustafsson, Erik Larsson, Michael Ljungberg, Katarina Sjögreen Gleisner","doi":"10.1186/s40658-024-00667-7","DOIUrl":"10.1186/s40658-024-00667-7","url":null,"abstract":"<p><strong>Background: </strong>The aim was to investigate the noise and bias properties of quantitative <sup>177</sup>Lu-SPECT with respect to the number of projection angles, and the number of subsets and iterations in the OS-EM reconstruction, for different total acquisition times.</p><p><strong>Methods: </strong>Experimental SPECT acquisition of six spheres in a NEMA body phantom filled with <sup>177</sup>Lu was performed, using medium-energy collimators and 120 projections with 180 s per projection. Bootstrapping was applied to generate data sets representing acquisitions with 20 to 120 projections for 10 min, 20 min, and 40 min, with 32 noise realizations per setting. Monte Carlo simulations were performed of <sup>177</sup>Lu-DOTA-TATE in an anthropomorphic computer phantom with three tumours (2.8 mL to 40.0 mL). Projections representing 24 h and 168 h post administration were simulated, each with 32 noise realizations. Images were reconstructed using OS-EM with compensation for attenuation, scatter, and distance-dependent resolution. The number of subsets and iterations were varied within a constrained range of the product number of iterations <math><mo>×</mo></math> number of projections <math><mrow><mo>≤</mo> <mn>2400</mn></mrow> </math> . Volumes-of-interest were defined following the physical size of the spheres and tumours, the mean activity-concentrations estimated, and the absolute mean relative error and coefficient of variation (CV) over noise realizations calculated. Pareto fronts were established by analysis of CV versus mean relative error.</p><p><strong>Results: </strong>Points at the Pareto fronts with low CV and high mean error resulted from using a low number of subsets, whilst points at the Pareto fronts associated with high CV but low mean error resulted from reconstructions with a high number of subsets. The number of projection angles had limited impact.</p><p><strong>Conclusions: </strong>For accurate estimation of the <sup>177</sup>Lu activity-concentration from SPECT images, the number of projection angles has limited importance, whilst the total acquisition time and the number of subsets and iterations are parameters of importance.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"62"},"PeriodicalIF":3.0,"publicationDate":"2024-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11247071/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141616124","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-10DOI: 10.1186/s40658-024-00651-1
Han Jiang, Yu Du, Zhonglin Lu, Bingjie Wang, Yonghua Zhao, Ruibing Wang, Hong Zhang, Greta S P Mok
Purpose: 123I-Ioflupane SPECT is an effective tool for the diagnosis and progression assessment of Parkinson's disease (PD). Radiomics and deep learning (DL) can be used to track and analyze the underlying image texture and features to predict the Hoehn-Yahr stages (HYS) of PD. In this study, we aim to predict HYS at year 0 and year 4 after the first diagnosis with combined imaging, radiomics and DL-based features using 123I-Ioflupane SPECT images at year 0.
Methods: In this study, 161 subjects from the Parkinson's Progressive Marker Initiative database underwent baseline 3T MRI and 123I-Ioflupane SPECT, with HYS assessment at years 0 and 4 after first diagnosis. Conventional imaging features (IF) and radiomic features (RaF) for striatum uptakes were extracted from SPECT images using MRI- and SPECT-based (SPECT-V and SPECT-T) segmentations respectively. A 2D DenseNet was used to predict HYS of PD, and simultaneously generate deep features (DF). The random forest algorithm was applied to develop models based on DF, RaF, IF and combined features to predict HYS (stage 0, 1 and 2) at year 0 and (stage 0, 1 and ≥ 2) at year 4, respectively. Model predictive accuracy and receiver operating characteristic (ROC) analysis were assessed for various prediction models.
Results: For the diagnostic accuracy at year 0, DL (0.696) outperformed most models, except DF + IF in SPECT-V (0.704), significantly superior based on paired t-test. For year 4, accuracy of DF + RaF model in MRI-based method is the highest (0.835), significantly better than DF + IF, IF + RaF, RaF and IF models. And DL (0.820) surpassed models in both SPECT-based methods. The area under the ROC curve (AUC) highlighted DF + RaF model (0.854) in MRI-based method at year 0 and DF + RaF model (0.869) in SPECT-T method at year 4, outperforming DL models, respectively. And then, there was no significant differences between SPECT-based and MRI-based segmentation methods except for the imaging feature models.
Conclusion: The combination of radiomic and deep features enhances the prediction accuracy of PD HYS compared to only radiomics or DL. This suggests the potential for further advancements in predictive model performance for PD HYS at year 0 and year 4 after first diagnosis using 123I-Ioflupane SPECT images at year 0, thereby facilitating early diagnosis and treatment for PD patients. No significant difference was observed in radiomics results obtained between MRI- and SPECT-based striatum segmentations for radiomic and deep features.
{"title":"Radiomics incorporating deep features for predicting Parkinson's disease in <sup>123</sup>I-Ioflupane SPECT.","authors":"Han Jiang, Yu Du, Zhonglin Lu, Bingjie Wang, Yonghua Zhao, Ruibing Wang, Hong Zhang, Greta S P Mok","doi":"10.1186/s40658-024-00651-1","DOIUrl":"10.1186/s40658-024-00651-1","url":null,"abstract":"<p><strong>Purpose: </strong><sup>123</sup>I-Ioflupane SPECT is an effective tool for the diagnosis and progression assessment of Parkinson's disease (PD). Radiomics and deep learning (DL) can be used to track and analyze the underlying image texture and features to predict the Hoehn-Yahr stages (HYS) of PD. In this study, we aim to predict HYS at year 0 and year 4 after the first diagnosis with combined imaging, radiomics and DL-based features using <sup>123</sup>I-Ioflupane SPECT images at year 0.</p><p><strong>Methods: </strong>In this study, 161 subjects from the Parkinson's Progressive Marker Initiative database underwent baseline 3T MRI and <sup>123</sup>I-Ioflupane SPECT, with HYS assessment at years 0 and 4 after first diagnosis. Conventional imaging features (IF) and radiomic features (RaF) for striatum uptakes were extracted from SPECT images using MRI- and SPECT-based (SPECT-V and SPECT-T) segmentations respectively. A 2D DenseNet was used to predict HYS of PD, and simultaneously generate deep features (DF). The random forest algorithm was applied to develop models based on DF, RaF, IF and combined features to predict HYS (stage 0, 1 and 2) at year 0 and (stage 0, 1 and ≥ 2) at year 4, respectively. Model predictive accuracy and receiver operating characteristic (ROC) analysis were assessed for various prediction models.</p><p><strong>Results: </strong>For the diagnostic accuracy at year 0, DL (0.696) outperformed most models, except DF + IF in SPECT-V (0.704), significantly superior based on paired t-test. For year 4, accuracy of DF + RaF model in MRI-based method is the highest (0.835), significantly better than DF + IF, IF + RaF, RaF and IF models. And DL (0.820) surpassed models in both SPECT-based methods. The area under the ROC curve (AUC) highlighted DF + RaF model (0.854) in MRI-based method at year 0 and DF + RaF model (0.869) in SPECT-T method at year 4, outperforming DL models, respectively. And then, there was no significant differences between SPECT-based and MRI-based segmentation methods except for the imaging feature models.</p><p><strong>Conclusion: </strong>The combination of radiomic and deep features enhances the prediction accuracy of PD HYS compared to only radiomics or DL. This suggests the potential for further advancements in predictive model performance for PD HYS at year 0 and year 4 after first diagnosis using <sup>123</sup>I-Ioflupane SPECT images at year 0, thereby facilitating early diagnosis and treatment for PD patients. No significant difference was observed in radiomics results obtained between MRI- and SPECT-based striatum segmentations for radiomic and deep features.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"11 1","pages":"60"},"PeriodicalIF":3.0,"publicationDate":"2024-07-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11236833/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141563014","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-09DOI: 10.1186/s40658-024-00661-z
Jens Maus, Pavel Nikulin, Frank Hofheinz, Jan Petr, Anja Braune, Jörg Kotzerke, Jörg van den Hoff
<p><strong>Background: </strong>Residual image noise is substantial in positron emission tomography (PET) and one of the factors limiting lesion detection, quantification, and overall image quality. Thus, improving noise reduction remains of considerable interest. This is especially true for respiratory-gated PET investigations. The only broadly used approach for noise reduction in PET imaging has been the application of low-pass filters, usually Gaussians, which however leads to loss of spatial resolution and increased partial volume effects affecting detectability of small lesions and quantitative data evaluation. The bilateral filter (BF) - a locally adaptive image filter - allows to reduce image noise while preserving well defined object edges but manual optimization of the filter parameters for a given PET scan can be tedious and time-consuming, hampering its clinical use. In this work we have investigated to what extent a suitable deep learning based approach can resolve this issue by training a suitable network with the target of reproducing the results of manually adjusted case-specific bilateral filtering.</p><p><strong>Methods: </strong>Altogether, 69 respiratory-gated clinical PET/CT scans with three different tracers ( <math> <mrow><msup><mo>[</mo> <mn>18</mn></msup> <mtext>F</mtext> <mo>]</mo></mrow> </math> FDG, <math> <mrow><msup><mo>[</mo> <mn>18</mn></msup> <mtext>F</mtext> <mo>]</mo></mrow> </math> L-DOPA, <math> <mrow><msup><mo>[</mo> <mn>68</mn></msup> <mtext>Ga</mtext> <mo>]</mo></mrow> </math> DOTATATE) were used for the present investigation. Prior to data processing, the gated data sets were split, resulting in a total of 552 single-gate image volumes. For each of these image volumes, four 3D ROIs were delineated: one ROI for image noise assessment and three ROIs for focal uptake (e.g. tumor lesions) measurements at different target/background contrast levels. An automated procedure was used to perform a brute force search of the two-dimensional BF parameter space for each data set to identify the "optimal" filter parameters to generate user-approved ground truth input data consisting of pairs of original and optimally BF filtered images. For reproducing the optimal BF filtering, we employed a modified 3D U-Net CNN incorporating residual learning principle. The network training and evaluation was performed using a 5-fold cross-validation scheme. The influence of filtering on lesion SUV quantification and image noise level was assessed by calculating absolute and fractional differences between the CNN, manual BF, or original (STD) data sets in the previously defined ROIs.</p><p><strong>Results: </strong>The automated procedure used for filter parameter determination chose adequate filter parameters for the majority of the data sets with only 19 patient data sets requiring manual tuning. Evaluation of the focal uptake ROIs revealed that CNN as well as BF based filtering essentially maintain the focal <math><msub><mtext>SUV</
背景:正电子发射计算机断层扫描(PET)的残留图像噪声很大,是限制病灶检测、定量和整体图像质量的因素之一。因此,改善降噪效果仍是一个相当重要的问题。对于呼吸门控正电子发射计算机断层扫描研究来说尤其如此。PET 成像中唯一广泛使用的降噪方法是应用低通滤波器,通常是高斯滤波器,但这会导致空间分辨率的损失和部分容积效应的增加,影响小病灶的检测能力和定量数据的评估。双边滤波器(BF)是一种局部自适应图像滤波器,可在保留清晰物体边缘的同时降低图像噪声,但针对特定 PET 扫描手动优化滤波器参数的工作既繁琐又耗时,妨碍了其临床应用。在这项工作中,我们研究了基于深度学习的合适方法能在多大程度上解决这一问题,方法是训练一个合适的网络,目标是再现手动调整特定病例双边滤波的结果:本研究共使用了69个呼吸门控临床PET/CT扫描,使用了三种不同的示踪剂([ 18 F ] FDG、[ 18 F ] L-DOPA、[ 68 Ga ] DOTATATE)。在进行数据处理之前,对门控数据集进行了拆分,共得到 552 个单门图像卷。每个图像卷都划分了四个三维 ROI:一个 ROI 用于图像噪声评估,三个 ROI 用于不同目标/背景对比度水平下的病灶摄取(如肿瘤病灶)测量。使用自动程序对每个数据集的二维 BF 参数空间进行暴力搜索,以确定 "最佳 "滤波参数,从而生成用户认可的基本真实输入数据,包括原始图像和最佳 BF 滤波图像对。为了再现最佳 BF 滤波,我们采用了一种结合残差学习原理的改进型 3D U-Net CNN。网络的训练和评估采用 5 倍交叉验证方案。通过计算 CNN、手动 BF 或原始(STD)数据集在先前定义的 ROI 中的绝对差异和分数差异,评估了过滤对病变 SUV 定量和图像噪声水平的影响:结果:用于确定滤波参数的自动程序为大多数数据集选择了适当的滤波参数,只有 19 个患者数据集需要手动调整。对病灶摄取 ROI 的评估显示,基于 CNN 和 BF 的滤波基本上保持了未滤波图像的病灶 SUV 最大值,平均±标准差较低,δ SUV max CNN , STD = (-3.9 ± 5.2) %,δ SUV max BF , STD = (-4.4 ± 5.3) %。关于 CNN 与 BF 的相对性能,这两种方法在绝大多数情况下得出的 SUV 最大值非常相似,总体平均差异为 δ SUV max CNN , BF = (0.5 ± 4.8)%。对噪声特性的评估显示,CNN 滤波能令人满意地再现 BF 的噪声水平和特性,δ Noise CNN , BF = (5.6 ± 10.5)%。CNN 和 BF 之间没有观察到明显的示踪剂依赖性差异:我们的研究结果表明,基于神经网络的去噪技术能够以完全自动化的方式重现逐个优化 BF 的结果。除了极少数情况外,它所得到的图像在噪声水平、边缘保留和信号恢复方面的质量几乎相同。我们相信,这种网络在改进呼吸门控 PET 研究的运动校正方面可能特别有用,但也有助于在临床 PET 中建立与 BF 相当的边缘保留 CNN 滤波,因为它避免了耗时的手动 BF 参数调整。
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