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首页> 外文期刊>Radiochimica Acta: International Journal for Chemical Aspects of Nuclear Science and Technology >Measurement of photo-neutron cross sections and isomeric yield ratios in the 89Y(γ,xn)89?x Y reactions at the bremsstrahlung end-point energies of 65, 70 and 75 MeV
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Measurement of photo-neutron cross sections and isomeric yield ratios in the 89Y(γ,xn)89?x Y reactions at the bremsstrahlung end-point energies of 65, 70 and 75 MeV

机译:在89Y(γ,Xn)89Ω·x y反应的光学中子横截面和异构屈服比的测量在65,70和75 mev的Bremsstrahlung终点能量下的反应

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摘要

The flux-weighted average cross sections of the 89Y(γ,xn; x=1–4)89?x Y reactions and the isomeric yield ratios of the 87m,gY, 86m,gY, and 85m,gY radionuclides produced in these reactions with the bremsstrahlung end-point energies of 65, 70 and 75 MeV have been determined by an activation and off-line γ-ray spectrometric technique using the 100 MeV electron linac in Pohang Accelerator Laboratory, Korea. The theoretical 89Y(γ,xn; x=1–4)89?x Y reactioncross sections for mono-energetic photonshave been calculated using the computer code TALYS 1.6. Then the flux-weighted theoretical values were obtaind to compare with the present data. The flux-weighted experimental and theoretical 89Y(γ,xn; x=1–4)89?x Y reaction cross sections increase very fast from the threshold values to a certain bremsstrahlung energy, wherethe other reaction channels open up. Thereafter it remains constant a while and then slowly decreases with the increase of cross sections for other reactions. Similarly, the isomeric yield ratios of 87m,gY,86m,gY and 85m,gY in the 89Y(γ,xn; x=2–4)89?x Y reactions from the present work and literature data show an increasing trend from their respective threshold values to a certain bremsstrahlung energy. After a certain point ofenergy, the isomeric yield ratios increase slowly with the bremsstrahlung energy. These observations indicate the role of excitation energy and its partitioning in different reaction channels.
机译:89Y(γ,xN; x = 1-4)的助焊剂加权平均横截面89?x Y反应和87m,Gy,86m,Gy和85米,Gy放射性核素的异构产率比在这些反应中产生利用韩国浦项加速器实验室的100 MeV电子LINAC,通过激活和离线γ射线光谱技术确定了65,70和75MeV的Bremsstrahlung终点能量。理论89Y(γ,xn; x = 1-4)89?x Y yryctcross部分用于单能量光电子,使用计算机代码TALYS 1.6计算。然后获得磁通量加权理论值,以与当前数据进行比较。助焊剂加权实验和理论89Y(γ,xn; x = 1-4)89?x Y反应横截面从阈值增加到某个Bremsstrahlung能量,而其他反应通道打开。此后,它保持恒定的一段时间,然后随着其他反应的横截面的增加而缓慢降低。类似地,87m,Gy,86m,Gy和85m,Gy在89Y(γ,xn; x = 2-4)中的异构率比,GY为89°(γ,xn; x = 2-4)89?x y从本作的工作和文献数据的反应显示出越来越大的趋势对某个Bremsstrahlung能量的相应阈值。在某种程度上,通过Bremsstrahlung能量缓慢增加异构率比。这些观察结果表明激发能量的作用及其在不同反应通道中的分配。

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