Kulage Zachary, Cantrell Tyler, Griswold Justin, Denton David, Garland Marc, Copping Roy, Mirzadeh Saed
Isotope and Fuel Cycle Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN, 37831-6226, USA; Department of Nuclear Engineering, Texas A&M University, College Station, TX, 77843-3133, USA.
Isotope and Fuel Cycle Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN, 37831-6226, USA.
Appl Radiat Isot. 2021 Jun;172:109645. doi: 10.1016/j.apradiso.2021.109645. Epub 2021 Feb 24.
The newest radioisotope for brachytherapy treatment of prostate cancer is Cs (t = 9.69 d, 100% EC). Generated via electron capture decay of Ba (t = 11.6 d, 100% EC), Cs has been used in brachytherapy for prostate cancer since 2004. The Ba parent is produced through neutron capture of enriched Ba in a nuclear reactor. For large-scale production of Ba, an accurate knowledge of production and burnup cross sections of Ba are essential. In this paper, we report two group cross sections (thermal and resonance integrals) for Ba and Ba and a new measure of the half-life of Ba. Targets consisting of milligram quantities of enriched Ba (∼35%) were irradiated in Oak Ridge National Laboratory's High Flux Isotope Reactor at thermal and resonance neutron fluxes of (1.9-2.1) × 10 and (5.8-7.0) × 10 neutrons·cm s, respectively, for durations ranging from 3 to 26 days. In addition, cadmium covered samples of Ba were irradiated for 1 hour at 12.6% full reactor power (10.7 MW). The yield of Ba approaches a saturation value of ∼60 GBq (∼1.6 Ci) per mg of Ba for 20 days irradiation at a thermal neutron flux of 1.8 × 10 n·s·cm, with a thermal/epithermal ratio of ∼30. Under the above experimental conditions, the two group cross sections of Ba are 6.9 ± 0.5 b (thermal, σ) and 173 ± 7 b (resonance, I). These values represent the sum of cross sections to metastable and ground states of Ba. For Ba, the empirically measured thermal cross section is 200 ± 50 b assuming an I/σ of 10. This cross section is reported for the first time. Further, the half-life of Ba was remeasured to be 11.657 ± 0.008 d. Lastly, this study also resulted in the co-production of Ba (t = 10.52 y, 100% EC). The experimental yield of Ba is ∼370 MBq (∼10 mCi) per mg of Ba (thin target) for one cycle irradiation in the High Flux Isotope Reactor, and measured two-group Ba cross sections are 7.2 ± 0.2 b and 39.9 ± 1.3 b. These values also represent the sum of cross sections to metastable and ground states of Ba.
用于前列腺癌近距离治疗的最新放射性同位素是铯 - 131(t₁/₂ = 9.69天,100%电子俘获)。铯 - 131通过钡 - 131(t₁/₂ = 11.6天,100%电子俘获)的电子俘获衰变产生,自2004年以来一直用于前列腺癌的近距离治疗。钡母体是通过在核反应堆中对富集的钡 - 130进行中子俘获产生的。对于大规模生产钡 - 131,准确了解钡 - 130的生产和燃耗截面至关重要。在本文中,我们报告了钡 - 130和钡 - 131的两组截面(热中子截面和共振积分)以及钡 - 131半衰期的新测量值。由毫克量的富集钡 - 130(约35%)组成的靶材分别在橡树岭国家实验室的高通量同位素反应堆中,以(1.9 - 2.1)×10¹³和(5.8 - 7.0)×10¹³中子·cm⁻²·s⁻¹的热中子通量和共振中子通量照射3至26天。此外,用镉覆盖的钡 - 130样品在反应堆满功率的12.6%(10.7兆瓦)下照射1小时。在热中子通量为1.8×10¹³ n·s⁻¹·cm⁻²的条件下照射20天,钡 - 131的产率接近每毫克钡 - 130约60吉贝可(约1.6居里)的饱和值,热中子/超热中子比约为30。在上述实验条件下,钡 - 130的两组截面为6.9±0.5靶恩(热中子截面,σ)和173±7靶恩(共振积分,I)。这些值代表了钡 - 130亚稳态和基态截面的总和。对于钡 - 131,假设I/σ为10,经验测量的热中子截面为200±50靶恩。该截面首次被报道。此外,钡 - 131的半衰期重新测量为11.657±0.008天。最后,本研究还导致了钡 - 133(t₁/₂ = 10.52年,100%电子俘获)的联产。在高通量同位素反应堆中进行一个循环照射,钡 - 133的实验产率约为每毫克钡 - 130(薄靶)370兆贝可(约10毫居里),测量得到的钡 - 133两组截面为7.2±0.2靶恩和39.9±1.3靶恩。这些值也代表了钡 - 133亚稳态和基态截面的总和。