{"title":"用于评估小动物SPECT和PET冷热区域图像质量和部分体积效应的模型的开发。","authors":"Takayuki Shibutani, Masahisa Onoguchi","doi":"10.2967/jnmt.125.271314","DOIUrl":null,"url":null,"abstract":"<p><p>The partial-volume effect (PVE) is a major factor affecting quantitative accuracy in small-animal SPECT and PET imaging, leading to underestimation of activity in hot-rod images and overestimation in cold-rod images. However, a phantom capable of assessing image quality, including the PVE in both hot and cold regions, has not been available. This study aimed to determine whether a newly developed phantom can accurately evaluate image quality, including the PVE of hot- and cold-rod images, in small-animal SPECT and PET systems. <b>Methods:</b> The phantom consisted of a cylindric pool and rod sections. The rod section included 6 hot rods and 6 cold rods with diameters of 1-6 mm. The rod and pool sections were filled with solutions containing <sup>99m</sup>Tc and <sup>18</sup>F, respectively. In the hot-rod section, the radioactive concentration ratio between rods and background was set to 4:1. Images were acquired for 30 min and reconstructed with a voxel size of 0.8 mm using a pixel-based ordered-subset expectation maximization algorithm. Image contrast, absolute and inverse recovery coefficients (RCs) (indicators of the PVE), and percent coefficient of variation (%CV) and signal-to-noise ratio (indicators of uniformity) were evaluated for both hot and cold rods. <b>Results:</b> The contrast of the hot rod for <sup>99m</sup>Tc and <sup>18</sup>F showed lower values with decreasing rod diameters. Furthermore, the <sup>99m</sup>Tc image demonstrated a higher contrast than the <sup>18</sup>F image and approached the true contrast. The cold-rod contrasts with <sup>99m</sup>Tc and <sup>18</sup>F followed a similar trend. The RCs of <sup>99m</sup>Tc and <sup>18</sup>F were lower as rod diameters decreased. The radioactive concentration in the 40-mm pool section was similar to that of the 6-mm hot rod for both radionuclides. The inverse RC was lower with a decreasing cold-rod diameter. Moreover, cold-rod images with <sup>18</sup>F demonstrated lower inverse RCs than with <sup>99m</sup>Tc. The %CVs for the <sup>99m</sup>Tc and <sup>18</sup>F images were 3.49% ± 0.03% and 6.29% ± 0.07%, respectively, with the <sup>99m</sup>Tc image displaying a lower %CV compared with the <sup>18</sup>F image. <b>Conclusion:</b> We developed a phantom that allows the evaluation of physical phenomena in small-animal SPECT and PET images, providing reliable assessment of image contrast, PVE, and uniformity in both hot and cold rods.</p>","PeriodicalId":16548,"journal":{"name":"Journal of nuclear medicine technology","volume":" ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2026-06-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Development of a Phantom for Evaluating Image Quality and Partial-Volume Effects in Hot and Cold Regions in Small-Animal SPECT and PET.\",\"authors\":\"Takayuki Shibutani, Masahisa Onoguchi\",\"doi\":\"10.2967/jnmt.125.271314\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The partial-volume effect (PVE) is a major factor affecting quantitative accuracy in small-animal SPECT and PET imaging, leading to underestimation of activity in hot-rod images and overestimation in cold-rod images. However, a phantom capable of assessing image quality, including the PVE in both hot and cold regions, has not been available. This study aimed to determine whether a newly developed phantom can accurately evaluate image quality, including the PVE of hot- and cold-rod images, in small-animal SPECT and PET systems. <b>Methods:</b> The phantom consisted of a cylindric pool and rod sections. The rod section included 6 hot rods and 6 cold rods with diameters of 1-6 mm. The rod and pool sections were filled with solutions containing <sup>99m</sup>Tc and <sup>18</sup>F, respectively. In the hot-rod section, the radioactive concentration ratio between rods and background was set to 4:1. Images were acquired for 30 min and reconstructed with a voxel size of 0.8 mm using a pixel-based ordered-subset expectation maximization algorithm. Image contrast, absolute and inverse recovery coefficients (RCs) (indicators of the PVE), and percent coefficient of variation (%CV) and signal-to-noise ratio (indicators of uniformity) were evaluated for both hot and cold rods. <b>Results:</b> The contrast of the hot rod for <sup>99m</sup>Tc and <sup>18</sup>F showed lower values with decreasing rod diameters. Furthermore, the <sup>99m</sup>Tc image demonstrated a higher contrast than the <sup>18</sup>F image and approached the true contrast. The cold-rod contrasts with <sup>99m</sup>Tc and <sup>18</sup>F followed a similar trend. The RCs of <sup>99m</sup>Tc and <sup>18</sup>F were lower as rod diameters decreased. The radioactive concentration in the 40-mm pool section was similar to that of the 6-mm hot rod for both radionuclides. The inverse RC was lower with a decreasing cold-rod diameter. Moreover, cold-rod images with <sup>18</sup>F demonstrated lower inverse RCs than with <sup>99m</sup>Tc. The %CVs for the <sup>99m</sup>Tc and <sup>18</sup>F images were 3.49% ± 0.03% and 6.29% ± 0.07%, respectively, with the <sup>99m</sup>Tc image displaying a lower %CV compared with the <sup>18</sup>F image. <b>Conclusion:</b> We developed a phantom that allows the evaluation of physical phenomena in small-animal SPECT and PET images, providing reliable assessment of image contrast, PVE, and uniformity in both hot and cold rods.</p>\",\"PeriodicalId\":16548,\"journal\":{\"name\":\"Journal of nuclear medicine technology\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2026-06-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of nuclear medicine technology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.2967/jnmt.125.271314\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of nuclear medicine technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2967/jnmt.125.271314","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING","Score":null,"Total":0}
Development of a Phantom for Evaluating Image Quality and Partial-Volume Effects in Hot and Cold Regions in Small-Animal SPECT and PET.
The partial-volume effect (PVE) is a major factor affecting quantitative accuracy in small-animal SPECT and PET imaging, leading to underestimation of activity in hot-rod images and overestimation in cold-rod images. However, a phantom capable of assessing image quality, including the PVE in both hot and cold regions, has not been available. This study aimed to determine whether a newly developed phantom can accurately evaluate image quality, including the PVE of hot- and cold-rod images, in small-animal SPECT and PET systems. Methods: The phantom consisted of a cylindric pool and rod sections. The rod section included 6 hot rods and 6 cold rods with diameters of 1-6 mm. The rod and pool sections were filled with solutions containing 99mTc and 18F, respectively. In the hot-rod section, the radioactive concentration ratio between rods and background was set to 4:1. Images were acquired for 30 min and reconstructed with a voxel size of 0.8 mm using a pixel-based ordered-subset expectation maximization algorithm. Image contrast, absolute and inverse recovery coefficients (RCs) (indicators of the PVE), and percent coefficient of variation (%CV) and signal-to-noise ratio (indicators of uniformity) were evaluated for both hot and cold rods. Results: The contrast of the hot rod for 99mTc and 18F showed lower values with decreasing rod diameters. Furthermore, the 99mTc image demonstrated a higher contrast than the 18F image and approached the true contrast. The cold-rod contrasts with 99mTc and 18F followed a similar trend. The RCs of 99mTc and 18F were lower as rod diameters decreased. The radioactive concentration in the 40-mm pool section was similar to that of the 6-mm hot rod for both radionuclides. The inverse RC was lower with a decreasing cold-rod diameter. Moreover, cold-rod images with 18F demonstrated lower inverse RCs than with 99mTc. The %CVs for the 99mTc and 18F images were 3.49% ± 0.03% and 6.29% ± 0.07%, respectively, with the 99mTc image displaying a lower %CV compared with the 18F image. Conclusion: We developed a phantom that allows the evaluation of physical phenomena in small-animal SPECT and PET images, providing reliable assessment of image contrast, PVE, and uniformity in both hot and cold rods.