Severity: Warning
Message: file_get_contents(https://...@pubfacts.com&api_key=b8daa3ad693db53b1410957c26c9a51b4908&a=1): Failed to open stream: HTTP request failed! HTTP/1.1 429 Too Many Requests
Filename: helpers/my_audit_helper.php
Line Number: 176
Backtrace:
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 176
Function: file_get_contents
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 250
Function: simplexml_load_file_from_url
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 1034
Function: getPubMedXML
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 3152
Function: GetPubMedArticleOutput_2016
File: /var/www/html/application/controllers/Detail.php
Line: 575
Function: pubMedSearch_Global
File: /var/www/html/application/controllers/Detail.php
Line: 489
Function: pubMedGetRelatedKeyword
File: /var/www/html/index.php
Line: 316
Function: require_once
Background: Radiotheragnostics makes use of the same molecular targeting vectors, labeled either with a diagnostic or therapeutic radionuclide, ideally of the same chemical element. The matched pair of scandium radionuclides, Sc and Sc, satisfies the desired physical aspects for PET imaging and radionuclide therapy, respectively. While the production and application of Sc was extensively studied, Sc is still in its infancy. The aim of the present study was, therefore, to investigate and compare two different methods of Sc production, based on the neutron irradiation of enriched Ca and Ti targets, respectively.
Methods: Sc was produced by thermal neutron irradiation of enriched Ca targets via the Ca(n,γ)Ca → Sc nuclear reaction and by fast neutron irradiation of Ti targets via the Ti(n,p)Sc nuclear reaction, respectively. The product was compared with regard to yield and radionuclidic purity. The chemical separation of Sc was optimized in order to obtain a product of sufficient quality determined by labeling experiments using DOTANOC. Finally, preclinical SPECT/CT experiments were performed in tumor-bearing mice and compared with the PET image of the Sc labeled counterpart.
Results: Up to 2 GBq Sc was produced by thermal neutron irradiation of enriched Ca targets. The optimized chemical isolation of Sc from the target material allowed formulation of up to 1.5 GBq Sc with high radionuclidic purity (>99.99%) in a small volume (~700 μL) useful for labeling purposes. Three consecutive separations were possible by isolating the in-grown Sc from the Ca-containing fraction. Sc produced by fast neutron irradiated Ti targets resulted in a reduced radionuclidic purity (99.95-88.5%). The chemical purity of the separated Sc was determined by radiolabeling experiments using DOTANOC achievable at specific activities of 10 MBq/nmol. In vivo the Sc-DOTANOC performed equal to Sc-DOTANOC as determined by nuclear imaging.
Conclusion: The production of Sc via the Ca(n,γ)Ca nuclear reaction demonstrated significant advantages over the Ti production route, as it provided higher quantities of a radionuclidically pure product. The subsequent decay of Ca enabled the repeated separation of the Sc daughter nuclide from the Ca parent nuclide. Based on the results obtained from this work, Sc shows potential to be produced in suitable quality for clinical application.
Download full-text PDF |
Source |
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC5824697 | PMC |
http://dx.doi.org/10.1186/s41181-017-0024-x | DOI Listing |
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