Viraj Sawant, Sneha Mithun, Ashish K Jha, Venkatesh Rangarajan
{"title":"Discovery NM/ ct670 Pro SPECT常规放射性核素诊断和治疗系统特性的蒙特卡罗模拟。","authors":"Viraj Sawant, Sneha Mithun, Ashish K Jha, Venkatesh Rangarajan","doi":"10.2967/jnmt.124.268696","DOIUrl":null,"url":null,"abstract":"<p><p>The collimator in the SPECT imaging system is a critical component that uniquely influences image quality. Collimator selection for the imaging of the specific isotope is of the utmost importance. This study used Monte Carlo simulations to evaluate the response of different collimators for commonly used radionuclides in SPECT imaging. <b>Methods:</b> The Simulating Medical Imaging Nuclear Detectors Monte Carlo program was used to simulate the Discovery NM/CT 670 Pro SPECT system equipped for a collimator-radionuclide pair to optimize the selection of the collimator for SPECT imaging. Low-energy high-resolution (LEHR), medium-energy general-purpose (MEGP), and high-energy general-purpose (HEGP) collimators were simulated with <sup>99m</sup>Tc, <sup>177</sup>Lu, and <sup>131</sup>I point sources (1 MBq) to evaluate spatial resolution, sensitivity, scatter fraction, and septal penetration. The results were analyzed for the optimization of the collimator-radionuclide pair. <b>Results:</b> For <sup>99m</sup>Tc (γ-energy, 140 keV), the resolution (full width at half maximum), sensitivity, scatter fraction, and septal penetration for LEHR, MEGP, and HEGP were 7.03 mm, 189 counts per minute (cpm)/μCi, 3.50%, and 2.65%; 9.3 mm, 184 cpm/μCi, 2.32%, and 1.35%; and 11.3 mm, 224 cpm/μCi, 2.05%, and 1.27%, respectively. For <sup>177</sup>Lu (γ-energy, 113 and 208 keV), the respective values were 7.5 mm, 62.52 cpm/μCi, 22.22%, and 18.56%; 9.6 mm, 20 cpm/μCi, 3.36%, and 2.19%; and 12.03 mm, 25 cpm/μCi, 2.88%, and 1.89%. For <sup>131</sup>I (γ-energy, 364 keV), the respective values were 11.5 mm, 6,027 cpm/μCi, 28.80%, and 49.78%; 11.3 mm, 152 cpm/μCi, 43.49%, and 32.89%; and 14.08 mm, 86 cpm/μCi, 23.85%, and 17.96%. <b>Conclusion:</b> The study highlighted the need to understand collimator characteristics as a function of photon energy, where quantitative evaluation is the main aspect. The study suggests that the collimators that had optimal characteristics for imaging with <sup>99m</sup>Tc, <sup>177</sup>Lu, and <sup>131</sup>I were the LEHR, MEGP, and HEGP collimators, respectively.</p>","PeriodicalId":16548,"journal":{"name":"Journal of nuclear medicine technology","volume":" ","pages":"30-35"},"PeriodicalIF":1.0000,"publicationDate":"2025-03-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Monte Carlo Simulation of Characteristics of Discovery NM/CT 670 Pro SPECT System for Routinely Used Diagnostic and Therapeutic Radionuclides.\",\"authors\":\"Viraj Sawant, Sneha Mithun, Ashish K Jha, Venkatesh Rangarajan\",\"doi\":\"10.2967/jnmt.124.268696\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The collimator in the SPECT imaging system is a critical component that uniquely influences image quality. Collimator selection for the imaging of the specific isotope is of the utmost importance. This study used Monte Carlo simulations to evaluate the response of different collimators for commonly used radionuclides in SPECT imaging. <b>Methods:</b> The Simulating Medical Imaging Nuclear Detectors Monte Carlo program was used to simulate the Discovery NM/CT 670 Pro SPECT system equipped for a collimator-radionuclide pair to optimize the selection of the collimator for SPECT imaging. Low-energy high-resolution (LEHR), medium-energy general-purpose (MEGP), and high-energy general-purpose (HEGP) collimators were simulated with <sup>99m</sup>Tc, <sup>177</sup>Lu, and <sup>131</sup>I point sources (1 MBq) to evaluate spatial resolution, sensitivity, scatter fraction, and septal penetration. The results were analyzed for the optimization of the collimator-radionuclide pair. <b>Results:</b> For <sup>99m</sup>Tc (γ-energy, 140 keV), the resolution (full width at half maximum), sensitivity, scatter fraction, and septal penetration for LEHR, MEGP, and HEGP were 7.03 mm, 189 counts per minute (cpm)/μCi, 3.50%, and 2.65%; 9.3 mm, 184 cpm/μCi, 2.32%, and 1.35%; and 11.3 mm, 224 cpm/μCi, 2.05%, and 1.27%, respectively. For <sup>177</sup>Lu (γ-energy, 113 and 208 keV), the respective values were 7.5 mm, 62.52 cpm/μCi, 22.22%, and 18.56%; 9.6 mm, 20 cpm/μCi, 3.36%, and 2.19%; and 12.03 mm, 25 cpm/μCi, 2.88%, and 1.89%. For <sup>131</sup>I (γ-energy, 364 keV), the respective values were 11.5 mm, 6,027 cpm/μCi, 28.80%, and 49.78%; 11.3 mm, 152 cpm/μCi, 43.49%, and 32.89%; and 14.08 mm, 86 cpm/μCi, 23.85%, and 17.96%. <b>Conclusion:</b> The study highlighted the need to understand collimator characteristics as a function of photon energy, where quantitative evaluation is the main aspect. 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引用次数: 0
摘要
在SPECT成像系统中,准直器是影响成像质量的关键部件。对特定同位素成像的准直器选择是至关重要的。本研究使用蒙特卡罗模拟来评估不同准直器对SPECT成像中常用放射性核素的响应。方法:采用模拟医学成像核探测器蒙特卡罗程序,模拟配备准直器-放射性核素对的Discovery NM/CT 670 Pro SPECT系统,优化SPECT成像准直器的选择。采用99mTc、177Lu和131I点源(1 MBq)模拟低能量高分辨率(LEHR)、中能量通用(MEGP)和高能通用(HEGP)准直器,评估空间分辨率、灵敏度、散射分数和间隔穿透度。对结果进行了分析,以优化准直器-放射性核素对。结果:在99mTc (γ-能量,140 keV)条件下,LEHR、MEGP和HEGP的分辨率(最大半宽)、灵敏度、散射分数和间隔穿透率分别为7.03 mm、189次/ min (cpm)/μCi、3.50%和2.65%;9.3 mm, 184 cpm/μCi, 2.32%, 1.35%;11.3 mm, 224 cpm/μCi, 2.05%, 1.27%。177Lu (γ-能,113和208 keV),分别为7.5 mm、62.52 cpm/μCi、22.22%和18.56%;9.6 mm, 20 cpm/μCi, 3.36%, 2.19%;12.03 mm, 25 cpm/μCi, 2.88%, 1.89%。131I (γ-能,364 keV)分别为11.5 mm、6027 cpm/μCi、28.80%和49.78%;11.3 mm, 152 cpm/μCi, 43.49%, 32.89%;14.08 mm, 86 cpm/μCi, 23.85%, 17.96%。结论:该研究强调需要理解准直器特性作为光子能量的函数,其中定量评价是主要方面。研究表明,99mTc、177Lu和131I成像特性最佳的准直器分别是LEHR、MEGP和HEGP准直器。
Monte Carlo Simulation of Characteristics of Discovery NM/CT 670 Pro SPECT System for Routinely Used Diagnostic and Therapeutic Radionuclides.
The collimator in the SPECT imaging system is a critical component that uniquely influences image quality. Collimator selection for the imaging of the specific isotope is of the utmost importance. This study used Monte Carlo simulations to evaluate the response of different collimators for commonly used radionuclides in SPECT imaging. Methods: The Simulating Medical Imaging Nuclear Detectors Monte Carlo program was used to simulate the Discovery NM/CT 670 Pro SPECT system equipped for a collimator-radionuclide pair to optimize the selection of the collimator for SPECT imaging. Low-energy high-resolution (LEHR), medium-energy general-purpose (MEGP), and high-energy general-purpose (HEGP) collimators were simulated with 99mTc, 177Lu, and 131I point sources (1 MBq) to evaluate spatial resolution, sensitivity, scatter fraction, and septal penetration. The results were analyzed for the optimization of the collimator-radionuclide pair. Results: For 99mTc (γ-energy, 140 keV), the resolution (full width at half maximum), sensitivity, scatter fraction, and septal penetration for LEHR, MEGP, and HEGP were 7.03 mm, 189 counts per minute (cpm)/μCi, 3.50%, and 2.65%; 9.3 mm, 184 cpm/μCi, 2.32%, and 1.35%; and 11.3 mm, 224 cpm/μCi, 2.05%, and 1.27%, respectively. For 177Lu (γ-energy, 113 and 208 keV), the respective values were 7.5 mm, 62.52 cpm/μCi, 22.22%, and 18.56%; 9.6 mm, 20 cpm/μCi, 3.36%, and 2.19%; and 12.03 mm, 25 cpm/μCi, 2.88%, and 1.89%. For 131I (γ-energy, 364 keV), the respective values were 11.5 mm, 6,027 cpm/μCi, 28.80%, and 49.78%; 11.3 mm, 152 cpm/μCi, 43.49%, and 32.89%; and 14.08 mm, 86 cpm/μCi, 23.85%, and 17.96%. Conclusion: The study highlighted the need to understand collimator characteristics as a function of photon energy, where quantitative evaluation is the main aspect. The study suggests that the collimators that had optimal characteristics for imaging with 99mTc, 177Lu, and 131I were the LEHR, MEGP, and HEGP collimators, respectively.