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ON DYNAMIC EFFECTS IN COHERENT X-RADIATION OF RELATIVISTIC ELECTRON IN BRAGG SCATTERING GEOMETRY

机译:散射几何中相对论电子相干X射线的动力学效应

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Analytical expressions for spectral-angular distribution of parametric X-radiation (PXR) and diffracted transition radiation (DTR) of relativistic electron crossing a single crystal plate in Bragg geometry are derived on the basis of two-wave approximation of dynamic diffraction theory [1]. The expressions for the general case of asymmetrical reflection of relativistic electron Coulomb field on the plate are obtained. It was shown that in this geometry the essential increase of PXR angular density is possible due to a dynamic effect of PXR spectrum broadening just as in Laue geometry [2]. The considered Bragg geometry is interesting because of an interference effect of extinction, as the wave vector becomes complex even when an absorption is absent, and then the incident wave energy is transferred into reflected wave. A frequency region where the extinction effect manifests itself is named "region of total absorption". It is shown that decrease of the angle of electron incidence to the plate under fixed Bragg angle (asymmetric change) gives rise to a considerable increase of DTR angle density. The possibility of dynamical Borrmann effect manifestation in PXR and DTR for a thick single crystal is also considered in this work. It is shown that by the change of reflection asymmetry one can create such conditions in which the length of the electron path in the plate becomes small enough to neglect the electron multiply scattering, and the length of photon path exceeds the photo absorption length resulting in a bright manifestation of Borrmann effect in PXR.
机译:基于动态衍射理论的两波近似,推导了穿过布拉格晶体的相对论电子穿过单晶板的参数X射线(PXR)和衍射跃迁辐射(DTR)的光谱角分布的解析表达式[1] 。得到了相对论电子库仑场在板上不对称反射的一般情况下的表达式。结果表明,在这种几何形状中,由于Lax几何形状中PXR谱展宽的动态影响,PXR角密度的必要增大是可能的[2]。由于消光的干扰效应,考虑到的布拉格几何形状很有趣,因为即使没有吸收时波矢量也会变得复杂,然后入射波能量会转换为反射波。本身表现出消光效果的频率区域被称为“总吸收区域”。结果表明,在固定的布拉格角(不对称变化)下,电子向板的入射角的减小会引起DTR角密度的显着增加。在这项工作中,还考虑了在厚的单晶PXR和DTR中动态出现Borrmann效应的可能性。结果表明,通过改变反射不对称性,人们可以创造这样的条件:板中电子路径的长度变得足够小,可以忽略电子的多次散射,而光子路径的长度超过了光吸收长度,从而导致在PXR中表现出Borrmann效应。

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