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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. B, Beam Interactions with Materials and Atoms >Measurements of the line resolved M-shell X-ray production cross sections for_(79)Au,_(82)Pb and _(83)Bi by 100 keV/u proton, C, N, O ions
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Measurements of the line resolved M-shell X-ray production cross sections for_(79)Au,_(82)Pb and _(83)Bi by 100 keV/u proton, C, N, O ions

机译:通过100 keV / u质子,C,N,O离子测量_(79)Au,_(82)Pb和_(83)Bi的线分辨M壳X射线产生截面

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摘要

The cross sections for production of the M_k (k = ξ, αβ, γ, m_1) X-rays of _(79)Au, _(82)Pb and _(83)Bi induced by the 100 keV/u proton, C~(4+), N~(5+) and O~(6+) ions have been measured in the present work. The experimental cross sections have been compared with the earlier reported values and those calculated using the ionization cross sections based on the ECPSSR model, the X-ray emission rates based on the Dirac-Fock model, the fluorescence and Coster-Kronig yields based on the Dirac-Hartree-Slater model. In addition, the present measured proton induced X-ray production cross sections have also been compared with those calculated using the Dirac-Hartree-Slater model based ionization cross sections. The intensity ratios among the M_k X-rays have been deduced and compared with the theoretical values. The present measured M_k (k = ξ, αβ, γ, m_1) X-ray production cross sections are found to be very high as compared to the theoretical values. The total M X-ray production cross sections for the targets under investigation exhibited Z_p~2 dependence; Z_p denotes the projectile atomic number.
机译:100 keV / u质子C诱发_(79)Au,_(82)Pb和_(83)Bi的M_k(k =ξ,αβ,γ,m_1)X射线的截面图在本工作中已测量了〜(4 +),N〜(5+)和O〜(6+)离子。已将实验横截面与先前报告的值进行了比较,并使用基于ECPSSR模型的电离横截面,基于Dirac-Fock模型的X射线发射速率,基于EPC的荧光和Coster-Kronig产率进行了计算。 Dirac-Hartree-Slater模型。此外,目前测得的质子诱导的X射线产生截面也已与使用Dirac-Hartree-Slater模型基于电离截面计算得出的截面进行了比较。推导了M_k X射线之间的强度比,并将其与理论值进行了比较。与理论值相比,发现当前测量的M_k(k =ξ,αβ,γ,m_1)X射线产生截面非常高。所研究目标的总M射线产生截面显示Z_p〜2依赖性; Z_p表示射弹的原子序数。

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