<p>Terbium-149g (<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(t_{1/2}\)</EquationSource> </InlineEquation> = 4.12 h) is of particular interest for targeted alpha therapy cancer treatment due to its ability to decay via both alpha and positron emission, making it a potential theranostic nuclide. Due to many challenges facing its production, there are limited facilities worldwide that have demonstrated the ability to produce this nuclide in quantities sufficient for medical research. Since the Cyclotron Institute at Texas A&amp;M University is a specialized accelerator facility capable of accelerating a wide variety of ions, we are investigating production pathway options. One of the major challenges facing its production is the known co-production of the excited isomeric state, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(^{149\textrm{m}}\)</EquationSource> </InlineEquation>Tb (<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(t_{1/2}\)</EquationSource> </InlineEquation> = 4.1 min). However, this state does not decay to the ground state of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(^{149\textrm{g}}\)</EquationSource> </InlineEquation>Tb, negating any potential contribution to its yield. Due to its short-half life, the cross section for the population of this state has never been measured. After calculating several potential reaction yields using predictive models, the reactions of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^{147-149}\)</EquationSource> </InlineEquation>Sm(<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(^{6}\)</EquationSource> </InlineEquation>Li,xn)<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(^{149}\)</EquationSource> </InlineEquation>Tb were identified as candidates. Lithium-6 beams of varied energies between 45-65 MeV were impinged on enriched <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(^{147}\)</EquationSource> </InlineEquation>Sm, <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{148}\)</EquationSource> </InlineEquation>Sm, and <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(^{149}\)</EquationSource> </InlineEquation>Sm targets at the Cyclotron Institute at Texas A&amp;M University, and the reaction products were measured immediately following irradiation using high-purity germanium detectors, enabling detection of both <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(^{149\textrm{m}}\)</EquationSource> </InlineEquation>Tb and <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(^{149\textrm{g}}\)</EquationSource> </InlineEquation>Tb. Cross sections for all nuclides produced in sufficient activity in these reactions were also measured and reported here. We conclude that the population of <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(^{149\textrm{m}}\)</EquationSource> </InlineEquation>Tb is much preferred over population of the ground state for these <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(^{6}\)</EquationSource> </InlineEquation>Li-induced reactions, and it is necessary to explore other options for <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(^{149\textrm{g}}\)</EquationSource> </InlineEquation>Tb production.</p>

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Cross sections of \(^{147-149}\)Sm(\(^{6}\)Li,x) reactions for the production of \(^{149}\)Tb for targeted alpha therapy

  • Laura A. Bills,
  • Alan B. McIntosh,
  • Jonathan T. Morrell,
  • Philip Adsley,
  • Austin D. Abbott,
  • Diana Carrasco Rojas,
  • Jeremias Garcia-Duarte,
  • Matthew D. Gott,
  • Kris Hagel,
  • Travis Hankins,
  • Jason T. Harke,
  • Bryan M. Harvey,
  • Richard O. Hughes,
  • Lauren A. McIntosh,
  • Yonatan Mishnayot,
  • Connor Mohs,
  • Gabriela A. Picayo,
  • Madison Reuter,
  • Robert Rider,
  • John Santucci,
  • Sophia Sauceda,
  • Maxwell Sorensen,
  • Alexandra Tabacaru,
  • Aaron S. Tamashiro,
  • Evgeny E. Tereshatov,
  • David Thomas,
  • Zachary Tobin,
  • C. Etienne Vermeulen,
  • Benjamin Wellons,
  • Sherry J. Yennello

摘要

Terbium-149g ( \(t_{1/2}\) = 4.12 h) is of particular interest for targeted alpha therapy cancer treatment due to its ability to decay via both alpha and positron emission, making it a potential theranostic nuclide. Due to many challenges facing its production, there are limited facilities worldwide that have demonstrated the ability to produce this nuclide in quantities sufficient for medical research. Since the Cyclotron Institute at Texas A&M University is a specialized accelerator facility capable of accelerating a wide variety of ions, we are investigating production pathway options. One of the major challenges facing its production is the known co-production of the excited isomeric state, \(^{149\textrm{m}}\) Tb ( \(t_{1/2}\) = 4.1 min). However, this state does not decay to the ground state of \(^{149\textrm{g}}\) Tb, negating any potential contribution to its yield. Due to its short-half life, the cross section for the population of this state has never been measured. After calculating several potential reaction yields using predictive models, the reactions of \(^{147-149}\) Sm( \(^{6}\) Li,xn) \(^{149}\) Tb were identified as candidates. Lithium-6 beams of varied energies between 45-65 MeV were impinged on enriched \(^{147}\) Sm, \(^{148}\) Sm, and \(^{149}\) Sm targets at the Cyclotron Institute at Texas A&M University, and the reaction products were measured immediately following irradiation using high-purity germanium detectors, enabling detection of both \(^{149\textrm{m}}\) Tb and \(^{149\textrm{g}}\) Tb. Cross sections for all nuclides produced in sufficient activity in these reactions were also measured and reported here. We conclude that the population of \(^{149\textrm{m}}\) Tb is much preferred over population of the ground state for these \(^{6}\) Li-induced reactions, and it is necessary to explore other options for \(^{149\textrm{g}}\) Tb production.