<HashMap><database>biostudies-literature</database><scores/><additional><omics_type>Unknown</omics_type><volume>49(4)</volume><submitter>De Nardo L</submitter><funding>INFN CSN3 project COME - COpper MEasurement</funding><pubmed_abstract>&lt;h4>Purpose&lt;/h4>&lt;sup>64&lt;/sup> Cu and &lt;sup>67&lt;/sup> Cu radioisotopes have nuclear characteristics suitable for nuclear medicine applications. The production of &lt;sup>64&lt;/sup> Cu is already well established. However, the production of &lt;sup>67&lt;/sup> Cu in quantities suitable to conduct clinical trials is more challenging as it leads to the coproduction of other Cu isotopes, in particular &lt;sup>64&lt;/sup> Cu. The aim of this study is to investigate the possibility of using a CuCl&lt;sub>2&lt;/sub> solution with a mixture of &lt;sup>67/64&lt;/sup> Cu radioisotopes for therapeutic purposes, providing an alternative solution for the cyclotron production problem.&lt;h4>Methods&lt;/h4>Copper radioisotopes activities were calculated by considering proton beam irradiation of the following targets: (i) &lt;sup>70&lt;/sup> Zn in the energy range 70-45 MeV; (ii) &lt;sup>68&lt;/sup> Zn in the energy range 70-35 MeV; (iii) a combination of &lt;sup>70&lt;/sup> Zn (70-55 MeV) and &lt;sup>68&lt;/sup> Zn (55-35 MeV). The contribution of each copper radioisotope to the human-absorbed dose was estimated with OLINDA/EXM software using the biokinetic model for CuCl&lt;sub>2&lt;/sub> published by ICRP 53. The total absorbed dose generated by the &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture, obtained through different production routes, was calculated at different times after the end of the bombardment (EOB). A simple spherical model was used to simulate tumors of different sizes containing uniformly distributed &lt;sup>67/64&lt;/sup> Cu mixture and to calculate the absorbed dose of self-irradiation. The biological damage produced by &lt;sup>67&lt;/sup> Cu and &lt;sup>64&lt;/sup> Cu was also evaluated through cellular dosimetry and cell surviving fraction assessment using the MIRDcell code, considering two prostate cancer cell lines with different radiosensitivity.&lt;h4>Results&lt;/h4>The absorbed dose to healthy organs and the effective dose (ED) per unit of administered activity of &lt;sup>67&lt;/sup> CuCl&lt;sub>2&lt;/sub> are higher than those of &lt;sup>64&lt;/sup> CuCl&lt;sub>2&lt;/sub> . Absorbed dose values per unit of administered activity of &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture increase with time after the EOB because the amount of &lt;sup>67&lt;/sup> Cu in the mixture increases. Survival data showed that the biological damage caused per each decay of &lt;sup>67&lt;/sup> Cu is greater than that of &lt;sup>64&lt;/sup> Cu, assuming that radionuclides remain accumulated in the cell cytoplasm. Sphere model calculations demonstrated that &lt;sup>64&lt;/sup> Cu administered activity must be about five times higher than that of &lt;sup>67&lt;/sup> Cu to obtain the same absorbed dose for tumor mass between 0.01 and 10 g and about 10 times higher for very small spheres. Consequently, the &lt;sup>64&lt;/sup> CuCl&lt;sub>2&lt;/sub> -absorbed dose to healthy organs will reach higher values than those of &lt;sup>67&lt;/sup> CuCl&lt;sub>2&lt;/sub> . The supplemental activity of the &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture, required to get the same tumor-absorbed dose produced by &lt;sup>67&lt;/sup> CuCl&lt;sub>2&lt;/sub> , triggers a dose increment (DI) in healthy organs. The waiting time post-EOB necessary to keep this DI below 10% (t&lt;sub>10%&lt;/sub> ) depends on the irradiation methods employed for the production of the &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture.&lt;h4>Conclusions&lt;/h4>A mixture of cyclotron produced &lt;sup>67/64&lt;/sup> Cu radioisotopes proved to be an alternative solution for the therapeutic use of CuCl&lt;sub>2&lt;/sub> with minimal DI to healthy organs compared with pure &lt;sup>67&lt;/sup> Cu. Irradiation of a &lt;sup>70&lt;/sup> Zn+&lt;sup>68&lt;/sup> Zn target in the 70-35 MeV proton energy range for 185 h appears to be the best option from among all the production routes investigated, as it gives the maximum amount of activity, the shortest t&lt;sub>10%&lt;/sub> (10 h), and less than 1% of &lt;sup>61&lt;/sup> Cu and &lt;sup>60&lt;/sup> Cu impurities.</pubmed_abstract><journal>Medical physics</journal><pagination>2709-2724</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9305914</full_dataset_link><repository>biostudies-literature</repository><pubmed_title>A feasibility study of the therapeutic application of a mixture of &lt;sup>67/64&lt;/sup> Cu radioisotopes produced by cyclotrons with proton irradiation.</pubmed_title><pmcid>PMC9305914</pmcid><pubmed_authors>Esposito J</pubmed_authors><pubmed_authors>Rosato A</pubmed_authors><pubmed_authors>De Nardo L</pubmed_authors><pubmed_authors>Mou L</pubmed_authors><pubmed_authors>Pupillo G</pubmed_authors><pubmed_authors>Melendez-Alafort L</pubmed_authors></additional><is_claimable>false</is_claimable><name>A feasibility study of the therapeutic application of a mixture of &lt;sup>67/64&lt;/sup> Cu radioisotopes produced by cyclotrons with proton irradiation.</name><description>&lt;h4>Purpose&lt;/h4>&lt;sup>64&lt;/sup> Cu and &lt;sup>67&lt;/sup> Cu radioisotopes have nuclear characteristics suitable for nuclear medicine applications. The production of &lt;sup>64&lt;/sup> Cu is already well established. However, the production of &lt;sup>67&lt;/sup> Cu in quantities suitable to conduct clinical trials is more challenging as it leads to the coproduction of other Cu isotopes, in particular &lt;sup>64&lt;/sup> Cu. The aim of this study is to investigate the possibility of using a CuCl&lt;sub>2&lt;/sub> solution with a mixture of &lt;sup>67/64&lt;/sup> Cu radioisotopes for therapeutic purposes, providing an alternative solution for the cyclotron production problem.&lt;h4>Methods&lt;/h4>Copper radioisotopes activities were calculated by considering proton beam irradiation of the following targets: (i) &lt;sup>70&lt;/sup> Zn in the energy range 70-45 MeV; (ii) &lt;sup>68&lt;/sup> Zn in the energy range 70-35 MeV; (iii) a combination of &lt;sup>70&lt;/sup> Zn (70-55 MeV) and &lt;sup>68&lt;/sup> Zn (55-35 MeV). The contribution of each copper radioisotope to the human-absorbed dose was estimated with OLINDA/EXM software using the biokinetic model for CuCl&lt;sub>2&lt;/sub> published by ICRP 53. The total absorbed dose generated by the &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture, obtained through different production routes, was calculated at different times after the end of the bombardment (EOB). A simple spherical model was used to simulate tumors of different sizes containing uniformly distributed &lt;sup>67/64&lt;/sup> Cu mixture and to calculate the absorbed dose of self-irradiation. The biological damage produced by &lt;sup>67&lt;/sup> Cu and &lt;sup>64&lt;/sup> Cu was also evaluated through cellular dosimetry and cell surviving fraction assessment using the MIRDcell code, considering two prostate cancer cell lines with different radiosensitivity.&lt;h4>Results&lt;/h4>The absorbed dose to healthy organs and the effective dose (ED) per unit of administered activity of &lt;sup>67&lt;/sup> CuCl&lt;sub>2&lt;/sub> are higher than those of &lt;sup>64&lt;/sup> CuCl&lt;sub>2&lt;/sub> . Absorbed dose values per unit of administered activity of &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture increase with time after the EOB because the amount of &lt;sup>67&lt;/sup> Cu in the mixture increases. Survival data showed that the biological damage caused per each decay of &lt;sup>67&lt;/sup> Cu is greater than that of &lt;sup>64&lt;/sup> Cu, assuming that radionuclides remain accumulated in the cell cytoplasm. Sphere model calculations demonstrated that &lt;sup>64&lt;/sup> Cu administered activity must be about five times higher than that of &lt;sup>67&lt;/sup> Cu to obtain the same absorbed dose for tumor mass between 0.01 and 10 g and about 10 times higher for very small spheres. Consequently, the &lt;sup>64&lt;/sup> CuCl&lt;sub>2&lt;/sub> -absorbed dose to healthy organs will reach higher values than those of &lt;sup>67&lt;/sup> CuCl&lt;sub>2&lt;/sub> . The supplemental activity of the &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture, required to get the same tumor-absorbed dose produced by &lt;sup>67&lt;/sup> CuCl&lt;sub>2&lt;/sub> , triggers a dose increment (DI) in healthy organs. The waiting time post-EOB necessary to keep this DI below 10% (t&lt;sub>10%&lt;/sub> ) depends on the irradiation methods employed for the production of the &lt;sup>67/64&lt;/sup> CuCl&lt;sub>2&lt;/sub> mixture.&lt;h4>Conclusions&lt;/h4>A mixture of cyclotron produced &lt;sup>67/64&lt;/sup> Cu radioisotopes proved to be an alternative solution for the therapeutic use of CuCl&lt;sub>2&lt;/sub> with minimal DI to healthy organs compared with pure &lt;sup>67&lt;/sup> Cu. Irradiation of a &lt;sup>70&lt;/sup> Zn+&lt;sup>68&lt;/sup> Zn target in the 70-35 MeV proton energy range for 185 h appears to be the best option from among all the production routes investigated, as it gives the maximum amount of activity, the shortest t&lt;sub>10%&lt;/sub> (10 h), and less than 1% of &lt;sup>61&lt;/sup> Cu and &lt;sup>60&lt;/sup> Cu impurities.</description><dates><release>2022-01-01T00:00:00Z</release><publication>2022 Apr</publication><modification>2025-04-04T12:26:47.916Z</modification><creation>2022-08-03T07:07:14.795Z</creation></dates><accession>S-EPMC9305914</accession><cross_references><pubmed>35134261</pubmed><doi>10.1002/mp.15524</doi></cross_references></HashMap>