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Study of coherent bremsstrahlung and comparison with channeling radiation.

机译:相干致辐射的研究以及与通道辐射的比较。

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摘要

Theoretical calculations of channeling radiation and coherent bremsstrahlung and experimental measurements of channeling radiation are presented in this work.; The many-beam formalism and the standard Hartree-Fock potentials were used to calculate the channeling radiation transition energies. The widths of the spectral lines were determined by the use of the complex potential which describes the incoherent scattering from vibrating atoms of the crystal. A series of channeling radiation experiments were performed at the Darmstadt superconducting linear accelerator S-DALINAC using incident electron beam energies of 6.00, 9.00 and 10.18 MeV on a germanium crystal. The results of the theoretical calculations (planar case) were compared with experimental data and are in reasonable agreement with the observed results. The observed linewidths are somewhat larger than the calculated values and this disagreement is thought to be due to crystal heating and lattice defects. The channeling radiation energies scale as {dollar}gammasp{lcub}5/3{rcub}{dollar} ({dollar}gamma{dollar} is the ratio of the electron total energy and its rest mass) for the deeply bound states (states localized in the vicinity of the atomic plane) and {dollar}gammasp2{dollar} for states localized between the channeling planes. Multiple scattering and x-ray absorption in the crystal are found to modify the shapes of the channeling peaks and shift their centers. The dependence of the channeling states relative to the crystal thickness is determined and theoretical values of the occupation length are calculated for the 1-0 transition.; Theoretical calculations of coherent bremsstrahlung are also presented, and compared with channeling radiation.
机译:这项工作介绍了信道辐射和相干致辐射的理论计算以及信道辐射的实验测量。使用多光束形式主义和标准的Hartree-Fock势来计算沟道辐射跃迁能。光谱线的宽度通过使用复电位来确定,该复电位描述了晶体振动原子的非相干散射。使用锗晶体上的6.00、9.00和10.18 MeV的入射电子束能量,在达姆施塔特超导线性加速器S-DALINAC上进行了一系列通道辐射实验。理论计算的结果(平面情况)与实验数据进行了比较,并与观察到的结果合理吻合。观察到的线宽比计算值大一些,并且该差异被认为是由于晶体加热和晶格缺陷引起的。对于深束缚态(态),沟道辐射能的标度为{dollar} gammasp {lcub} 5/3 {rcub} {dollar}({dollar} gamma {dollar}是电子总能量与它的静止质量之比) (位于原子平面附近)和{dollar} gammasp2 {dollar}用于位于通道平面之间的状态。发现晶体中的多次散射和X射线吸收会改变通道峰的形状并改变其中心。确定沟道状态相对于晶体厚度的依赖性,并计算出1-0跃迁的占据长度的理论值。还介绍了相干致辐射的理论计算,并将其与通道辐射进行了比较。

著录项

  • 作者

    Chouffani El Fassi, Khalid.;

  • 作者单位

    The Catholic University of America.;

  • 授予单位 The Catholic University of America.;
  • 学科 Physics Nuclear.; Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 1995
  • 页码 152 p.
  • 总页数 152
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 原子核物理学、高能物理学;
  • 关键词

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