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Signatures of the differential Klein-Nishina electronic cross section in Compton's quantum theory of scattering of radiation

机译:康普顿量子散射散射散射理论中差动Klein-Nishina电子横截面的签名

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Here, we consider the problem of separating the relative contributions of kinematics and dynamics to the differential Klein‐Nishina electronic cross section using graphical and numerical analysis. We show that the values of the energy of scattered photons, and hence the kineticenergy of recoiled electrons calculated from Compton's quantum theory of scattering of radiation, show a degree of matching that increases with the increase in incident photon energy as quantified by chi-square goodness of fit test, with the calculated differential Klein‐Nishina electroniccross section per electron per unit solid angle for the scattering of an unpolarized photon by a stationary free electron, when appropriate normalization procedures are invoked. There is a high degree of matching in a regime where the total electronic Klein‐Nishina cross section forthe Compton scattering on a free stationary electron scales as the inverse of the incident photon energy and the contribution of the electro-magnetic interaction to differential electronic cross section diminishes. Hence the third level explanation of Compton effect by quantum electrodynamicshas a degree of matching with the first level of Compton's quantum theory. The degree of mismatch is an indicator of the relative contribution of dynamics to differential Klein‐Nishina electronic cross section compared to kinematics. For incident photon energies less than 1?MeV,we obtain the values of the scattering angles at which calculated differential cross section is nonzero but is kinematically limited which may lead to broadening of Compton profile. At the scattering angle where the differential cross section value is minimum for a given incident photon energy,we obtain the relative contribution of dynamics to the differential cross section compared to kinematics. Therefore, these predictions which need to be confirmed experimentally have significance to the understanding of the mechanisms of photon‐electron interactions in the Compton scattering.
机译:在这里,我们考虑使用图形和数值分析将运动学和动力学的相对贡献分离到差分Klein-Nishina电子横截面的问题。我们表明散射光子能量的值,因此从康普顿量子散射散射辐射计算的蓄水电子的动力学,显示了随着Chi-Square良好量化的情况而增加的匹配程度。适合测试,随着调用适当的归一化程序时,每单位电子每单位单位固体角度的差分差分Klein-Nishina Electroniccross部分,用于通过固定式自由电子散射未经谐波的光子。在一个政权中,在自由固定电子秤上的康普顿散射的总电子克莱因 - 南那横截面作为事件光子能量的倒数和电磁相互作用与差分电子横截面的贡献,有很高的匹配减少。因此,量子电动动力学对康普顿效应的第三级解释与康普顿量子理论的第一级匹配程度。与运动学相比,不匹配程度是动态对差动Klein-Nishina电子横截面的相对贡献的指标。对于小于1Ω的光子能量,我们获得计算的差分横截面是非零的散射角度的值,但是在运动学上限制,这可能导致康普顿轮廓的扩大。在给定的入射光子能量的差分横截面值最小的散射角度,与运动学相比,我们获得了动力学对差分横截面的相对贡献。因此,需要确认的这些预测实验对康普顿散射中的光子 - 电子相互作用的机制来具有重要意义。

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