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W. Ulmer, “On the Creation of High Energy Bremsstrahlung and Intensity by a Multi-Target and Repeated Focusing of the Scattered Electrons by Small-Angle Backscatter at the Wall of a Cone and Magnetic Fields—A Possible Way to Improve Linear Accelerators in Radiotherapy and to Verify Heisenberg-Euler Scatter,” Radiation Physics and Chemistry, Vol. 81, No. 4, 2012, pp. 387-402. http://dx.doi.org/10.1016/j.radphyschem.2011.12.033

has been cited by the following article:

• TITLE: Creation of High Energy/Intensity Bremsstrahlung by a Multi-Target and Focusing of the Scattered Electrons by Small-Angle Backscatter at a Cone Wall and a Magnetic Field—Enhancement of the Outcome of Linear Accelerators in Radiotherapy

  AUTHORS: W. Ulmer

  KEYWORDS: Multitarget; Bremsstrahlung; Wall Scatter; Focusing by Magnetic Field

  JOURNAL NAME: International Journal of Medical Physics, Clinical Engineering and Radiation Oncology, Vol.2 No.4, November 5, 2013

  ABSTRACT: The yield of bremsstrahlung (BS) from collisions of fast electrons (energy at least 6 MeV) with a Tungsten target can be significantly improved by exploitation of Tungsten wall scatter in a multi-layered target. A simplified version of a previously developed principle is also able to focus on small angle scattered electrons by a Tungsten wall. It is necessary that the thickness of each Tungsten layer does not exceed 0.04 mm—a thickness of 0.03 mm is suitable for accelerators in medical physics. Further focusing of electrons results from suitable magnetic fields with field strength between 0.5 Tesla and 1.2 Tesla (if the cone with multi-layered targets is rather narrow). Linear accelerators in radiation therapy only need to be focused by wall scatter without further magnetic fields (a standard case: 31 plates with 0.03 mm thickness and 1 mm distance between the plates). We considered three cases with importance in medical physics: A very small cone with an additional magnetic field for focusing (the field diameter at 90 cm depth: 6 cm), a medium cone with an optional magnetic field (field diameter at 90 cm depth: 13 cm) and a broad cone without a magnetic field (the field diameter at 90 cm depth: 30 cm). All these cases can be positioned in a carousel. Measurements have been performed in the existing carousel positioned in the plane of the flattening filter and scatter foils for electrons.