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Title: Measurement of the 230Th(p,2n)Pa229 and 230Th(p,3n)Pa228 reaction cross sections from 14.1 to 16.9 MeV

Abstract

Actinium-225 is of interest for medical isotope production and there is on-going research into methods of producing Ac 225 , either directly or via the decay of its parent isotopes ( Th 229 , Pa 229 , and Ra 225 ). One method that has been suggested is the Th 230 ( p , 2 n ) Pa 229 reaction. However, there is no available cross-section data for this reaction in the literature. Purpose: Measure the Th 230 ( p , 2 n ) and Th 230 ( p , 3 n ) reaction cross sections in the energy range where the ( p , 2 n ) reaction is predicted to peak to determine the feasibility of Ac 225 production via the Th 230 ( p , 2 n ) reaction. Methods: Targets naturally enriched in Th 230 were irradiated at the Center for Accelerator Mass Spectrometry at Lawrence Livermore National Laboratory with energies ranging from 14.1 to 16.9 MeV. Furthermore, chemical processing was used to separate the protactinium activation products, followed by γ -ray spectroscopy to measure the activities of Pa 228 , 229 , 230 , 232 produced in the irradiation. Results: We find that excitation functions are reported for the first time in the literature for the Th 230 ( p , 2 n ) and Th 230 ( p , 3 n ) reactions in this energy range. The peak measured value of the Th 230 ( p , 2 n ) reaction was found to be 182 ± 12 mb at 14.4 ± 0.1 MeV. The Th 232 ( p , n ) Pa 232 reaction was used to verify the experimental conditions, the measured values are reported and are comparable to the existing literature values. From the γ -ray spectrometry data, the half-life of Pa 229 was measured as 1.5 ± 0.1 days, which is within the error of the half-life reported in the evaluated nuclear data as well as in the recent measurements, and the half-life of Pa 228 was measured as 19.5 ± 0.4 hours. Conclusions: Overall, the Th 230 ( p , 2 n ) Pa 229 reaction could reasonably be used for Ac 225 isotope production, although significant amounts of relatively isotopically pure Th 230 would be needed for significant production because the low alpha-decay branching ratio of Pa 229 and long half-life of Th 229 inhibit the in-growth of significant amounts of Ac 225 .

Authors:
ORCiD logo [1];  [2]; ORCiD logo [3]
  1. Univ. of California, Berkeley, CA (United States); Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  2. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  3. Univ. of California, Berkeley, CA (United States)
Publication Date:
Research Org.:
Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)
Sponsoring Org.:
USDOE National Nuclear Security Administration (NNSA)
OSTI Identifier:
1779588
Report Number(s):
LLNL-JRNL-818313
Journal ID: ISSN 2469-9985; 1028002; TRN: US2209666
Grant/Contract Number:  
AC52-07NA27344; NA0003180
Resource Type:
Accepted Manuscript
Journal Name:
Physical Review C
Additional Journal Information:
Journal Volume: 103; Journal Issue: 3; Journal ID: ISSN 2469-9985
Publisher:
American Physical Society (APS)
Country of Publication:
United States
Language:
English
Subject:
38 RADIATION CHEMISTRY, RADIOCHEMISTRY, AND NUCLEAR CHEMISTRY; Lifetimes & widths; nuclear reactions; nucleon induced nuclear reactions; rare & new isotopes; transfer reactions; particle sources & targets

Citation Formats

Kmak, Kelly N., Shaughnessy, Dawn A., and Vujic, Jasmina. Measurement of the 230Th(p,2n)Pa229 and 230Th(p,3n)Pa228 reaction cross sections from 14.1 to 16.9 MeV. United States: N. p., 2021. Web. doi:10.1103/physrevc.103.034610.
Kmak, Kelly N., Shaughnessy, Dawn A., & Vujic, Jasmina. Measurement of the 230Th(p,2n)Pa229 and 230Th(p,3n)Pa228 reaction cross sections from 14.1 to 16.9 MeV. United States. https://doi.org/10.1103/physrevc.103.034610
Kmak, Kelly N., Shaughnessy, Dawn A., and Vujic, Jasmina. Mon . "Measurement of the 230Th(p,2n)Pa229 and 230Th(p,3n)Pa228 reaction cross sections from 14.1 to 16.9 MeV". United States. https://doi.org/10.1103/physrevc.103.034610. https://www.osti.gov/servlets/purl/1779588.
@article{osti_1779588,
title = {Measurement of the 230Th(p,2n)Pa229 and 230Th(p,3n)Pa228 reaction cross sections from 14.1 to 16.9 MeV},
author = {Kmak, Kelly N. and Shaughnessy, Dawn A. and Vujic, Jasmina},
abstractNote = {Actinium-225 is of interest for medical isotope production and there is on-going research into methods of producing Ac225, either directly or via the decay of its parent isotopes (Th229, Pa229, and Ra225). One method that has been suggested is the Th230(p,2n)Pa229 reaction. However, there is no available cross-section data for this reaction in the literature. Purpose: Measure the Th230(p,2n) and Th230(p,3n) reaction cross sections in the energy range where the (p,2n) reaction is predicted to peak to determine the feasibility of Ac225 production via the Th230(p,2n) reaction. Methods: Targets naturally enriched in Th230 were irradiated at the Center for Accelerator Mass Spectrometry at Lawrence Livermore National Laboratory with energies ranging from 14.1 to 16.9 MeV. Furthermore, chemical processing was used to separate the protactinium activation products, followed by γ-ray spectroscopy to measure the activities of Pa228,229,230,232 produced in the irradiation. Results: We find that excitation functions are reported for the first time in the literature for the Th230(p,2n) and Th230(p,3n) reactions in this energy range. The peak measured value of the Th230(p,2n) reaction was found to be 182±12 mb at 14.4±0.1 MeV. The Th232(p,n)Pa232 reaction was used to verify the experimental conditions, the measured values are reported and are comparable to the existing literature values. From the γ-ray spectrometry data, the half-life of Pa229 was measured as 1.5±0.1 days, which is within the error of the half-life reported in the evaluated nuclear data as well as in the recent measurements, and the half-life of Pa228 was measured as 19.5±0.4 hours. Conclusions: Overall, the Th230(p,2n)Pa229 reaction could reasonably be used for Ac225 isotope production, although significant amounts of relatively isotopically pure Th230 would be needed for significant production because the low alpha-decay branching ratio of Pa229 and long half-life of Th229 inhibit the in-growth of significant amounts of Ac225.},
doi = {10.1103/physrevc.103.034610},
journal = {Physical Review C},
number = 3,
volume = 103,
place = {United States},
year = {Mon Mar 15 00:00:00 EDT 2021},
month = {Mon Mar 15 00:00:00 EDT 2021}
}

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