2010/06/03 by N. F. Shul'ga, N.F. Shul’ga, Shul'ga, N. F. +4
Physics and Astronomy · #Accelerator Physics (physics.acc-ph) #Computational Physics (physics.comp-ph) #Crystallography and Radiation Phenomena #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #hep-ph #physics.acc-ph #physics.comp-ph
paper · pdf · doi:10.48550/arxiv.1006.0635
5 pages, 5 .eps figures, based on the report presented at XL International Conference on the Physics of Interaction of Charged Particles with Crystals, Moscow, 2010, May 25-27
arxiv created 2010/06/03 · openalex publication_date 2010/06/03 · arxiv updated 2010/06/04 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
The bremsstrahlung cross section for relativistic electrons in a crystal is split into the sum of coherent and incoherent parts (the last is due to a thermal motion of atoms in the crystal). Although the spectrum of incoherent radiation in crystal is similar to one in amorphous medium, the incoherent radiation intensity could demonstrate substantial dependence on the crystal orientation due to the electrons' flux redistribution in the crystal. In the present paper we apply our method of the incoherent bremsstrahlung simulation developed earlier to interpretation of some recent experimental results obtained at the Mainz Microtron MAMI.