{"title":"Selection of key parameters for the high yield production of 99mTc via 100Mo (p, 2n) 99mTc reaction in a cyclotron","authors":"Yue Yu, Zhi Chen","doi":"10.1016/j.radphyschem.2025.112695","DOIUrl":null,"url":null,"abstract":"<div><div>The most common radioisotope in nuclear medicine imaging is <sup>99m</sup>Tc. One of the efficient ways to alleviate the instability of the <sup>99m</sup>Tc supply chain in recent years is to produce <sup>99m</sup>Tc by <sup>100</sup>Mo (p,2n) in a cyclotron. The selection of key parameters in production is crucial for enhancing resource utilization and productivity. The purpose of this study is to examine how specific factors, such as the target parameters (material type, size) and irradiation parameters (proton energy, beam spot size, beam intensity, irradiation time, and cooling time) impact the yield of <sup>99m</sup>Tc, to obtain the appropriate technological parameters for producing <sup>99m</sup>Tc via <sup>100</sup>Mo (p,2n) <sup>99m</sup>Tc in a cyclotron. The <sup>99m</sup>Tc yields of enriched targets (<sup>100</sup>Mo-1, <sup>100</sup>Mo-2, <sup>100</sup>MoO<sub>3</sub>, <sup>100</sup>Mo<sub>2</sub>C) and natural targets (Mo-nat, MoO<sub>3</sub>-nat) under various irradiation conditions are simulated by using the Monte Carlo software FLUKA, and the obtained results are analyzed and compared. The findings indicate that for enriched targets, the optimal beam energies for maximizing <sup>99m</sup>Tc yield is approximately 17.3 MeV, while for natural targets, it is around 13 MeV for a high RNP of <sup>99m</sup>Tc. Enriched <sup>100</sup>Mo metal demonstrated superior production capacity, followed by molybdenum carbide to molybdenum oxide, natural molybdenum is not recommended for production but can be used as a test material. Shorter irradiation and cooling periods are preferable. A beam radius that is marginally smaller than the target radius is ideal. The target thickness should be maintained to reduce the incident energy to the reaction threshold. The optimal production parameters corresponding to the specified targets are obtained in this work, which provides valuable guidance for selecting key parameters in the preparation of <sup>99m</sup>Tc using a proton accelerator.</div></div>","PeriodicalId":20861,"journal":{"name":"Radiation Physics and Chemistry","volume":"232 ","pages":"Article 112695"},"PeriodicalIF":2.8000,"publicationDate":"2025-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Radiation Physics and Chemistry","FirstCategoryId":"92","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0969806X25001872","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The most common radioisotope in nuclear medicine imaging is 99mTc. One of the efficient ways to alleviate the instability of the 99mTc supply chain in recent years is to produce 99mTc by 100Mo (p,2n) in a cyclotron. The selection of key parameters in production is crucial for enhancing resource utilization and productivity. The purpose of this study is to examine how specific factors, such as the target parameters (material type, size) and irradiation parameters (proton energy, beam spot size, beam intensity, irradiation time, and cooling time) impact the yield of 99mTc, to obtain the appropriate technological parameters for producing 99mTc via 100Mo (p,2n) 99mTc in a cyclotron. The 99mTc yields of enriched targets (100Mo-1, 100Mo-2, 100MoO3, 100Mo2C) and natural targets (Mo-nat, MoO3-nat) under various irradiation conditions are simulated by using the Monte Carlo software FLUKA, and the obtained results are analyzed and compared. The findings indicate that for enriched targets, the optimal beam energies for maximizing 99mTc yield is approximately 17.3 MeV, while for natural targets, it is around 13 MeV for a high RNP of 99mTc. Enriched 100Mo metal demonstrated superior production capacity, followed by molybdenum carbide to molybdenum oxide, natural molybdenum is not recommended for production but can be used as a test material. Shorter irradiation and cooling periods are preferable. A beam radius that is marginally smaller than the target radius is ideal. The target thickness should be maintained to reduce the incident energy to the reaction threshold. The optimal production parameters corresponding to the specified targets are obtained in this work, which provides valuable guidance for selecting key parameters in the preparation of 99mTc using a proton accelerator.
期刊介绍:
Radiation Physics and Chemistry is a multidisciplinary journal that provides a medium for publication of substantial and original papers, reviews, and short communications which focus on research and developments involving ionizing radiation in radiation physics, radiation chemistry and radiation processing.
The journal aims to publish papers with significance to an international audience, containing substantial novelty and scientific impact. The Editors reserve the rights to reject, with or without external review, papers that do not meet these criteria. This could include papers that are very similar to previous publications, only with changed target substrates, employed materials, analyzed sites and experimental methods, report results without presenting new insights and/or hypothesis testing, or do not focus on the radiation effects.