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Photoneutron cross-sections for the reactions $$^{181}\mathrm{Ta}(\gamma ,\textit{x}n; \textit{x} = 1$$ 181 Ta ( γ , x n ; x = 1 – $$8)^{181-\textit{x}}\mathrm{Ta}$$ 8 ) 181 - x Ta AT $$\hbox { {E}}_\gamma {_\mathrm{max}}=$$ E γ max = 80–95 MeV
The European Physical Journal A ( IF 2.7 ) Pub Date : 2021-06-28 , DOI: 10.1140/epja/s10050-021-00484-x
A. N. Vodin , O. S. Deiev , I. S. Timchenko , S. N. Olejnik , M. I. Ayzatskiy , V. A. Kushnir , V. V. Mytrochenko , S. A. Perezhogin

The flux-averaged cross-sections \(\langle {\sigma (E_{\gamma \mathrm{max}})}\rangle \) for the \(^{181}\mathrm{Ta}(\gamma ,\textit{x}n; \textit{x} = 1\)\(8)^{181-\textit{x}}\mathrm{Ta}\) reactions have been measured at the end-point bremsstrahlung energies of 80–95 MeV. The experiments were performed by using the beam from the NSC KIPT electron linear accelerator LUE-40 and measuring the residual \(\gamma \)-ray activities of the reaction products. The theoretical \(\langle {\sigma (E_{\gamma \mathrm{max}})}\rangle \) values were computed using the mono-energetic cross-sections \(\sigma (E)\) from TALYS1.9 code. A comparison between the measured average cross-sections and the theoretical values show good agreement for the \((\gamma ,1\)\(6\mathrm{n})\) reactions but substantial differences for the \((\gamma ,7\mathrm{n})\) and \((\gamma ,8\mathrm{n})\) reactions. Isomeric average cross-section ratios \(d(E_{\gamma \mathrm{max}})\) of a product \(^{178g,m}\mathrm{Ta}\) produced from the \(^{181}\mathrm{Ta}(\gamma ,3\mathrm{n})\) reaction have been obtained. The results have been compared with the literature data and the theoretical values based on TALYS1.9 code.



中文翻译:

反应的光中子截面 $$^{181}\mathrm{Ta}(\gamma ,\textit{x}n; \textit{x} = 1$$ 181 Ta ( γ , xn ; x = 1 – $ $8)^{181-\textit{x}}\mathrm{Ta}$$ 8 ) 181 - x Ta $$\hbox { {E}}_\gamma {_\mathrm{max}}=$$ E γ 最大值 = 80–95 MeV

通量平均横截面\(\ langle {\西格玛(E _ {\伽马\ mathrm {MAX}})} \ rangle \)\(^ {181} \ mathrm {的Ta}(\γ,\ textit {x}n; \textit{x} = 1\)\(8)^{181-\textit{x}}\mathrm{Ta}\)反应在端点轫致辐射能量为 80– 95 兆电子伏。实验是通过使用来自 NSC KIPT 电子直线加速器 LUE-40 的光束并测量反应产物的残余\(\gamma \)射线活度来进行的。理论\(\langle {\sigma (E_{\gamma \mathrm{max}})}\rangle \)值是使用单能截面\(\sigma (E)\)来自 TALYS1.9 代码。测量的平均横截面与理论值之间的比较表明\((\gamma ,1\)\(6\mathrm{n})\)反应非常一致,但\((\gamma ,7\mathrm{n})\)\((\gamma ,8\mathrm{n})\)反应。由\(^{181}产生的产物\(^{178g,m}\mathrm{Ta}\) 的异构平均横截面比\(d(E_{\gamma \mathrm{max}})\) \mathrm{Ta}(\gamma ,3\mathrm{n})\)反应已经得到。结果与文献数据和基于TALYS1.9代码的理论值进行了对比。

更新日期:2021-06-28
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