Author: Bundesmann, J.
Paper Title Page
MOE02 A Multi-leaf Faraday Cup Especially for Proton Therapy of Ocular Tumors 118
 
  • S. Seidel, J. Bundesmann, T. Damerow, A. Denker, C.S.G. Kunert
    HZB, Berlin, Germany
  • A. Weber
    Charite, Berlin, Germany
 
  In cooperation with the university hospital Charité – Universitätsmedizin Berlin the Helmholtz-Zentrum Berlin (HZB) provides a proton beam used for radiation therapy of intraocular tumors. The protons are accelerated to 68 MeV by an isochronous cyclotron as the main accelerator. The human eye is a very small and complex organ with several critical structures which must be spared from irradiation as much as possible. Hence radiation therapy with protons is especially convenient due to their well-defined Bragg peak. At the HZB the distal fall off (the distance between 90% and 10% of the dose level) is less than 1 mm in water. Therefore it is crucial to measure the energy and maximum range of the beam with the corresponding high accuracy. A Multi-Leaf Faraday Cup (MLFC) allows a quick and precise range-measurement of proton beams. We present a MLFC which meets those special requirements of the eye tumor therapy. Results of range-measurements in different energy regions revealing the achievable submillimeter precession are shown; and examples for applications in radiation hardness testing are given.  
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TUA03 New Time Structures Available at the HZB Cyclotron 130
 
  • A. Denker, J. Bundesmann, T. Damerow, T. Fanselow, D. Hildebrand, U. Hiller, C. Rethfeldt, J. Röhrich
    HZB, Berlin, Germany
 
  While most of the beam time of the cyclotron is used for proton therapy of ocular melanomas, an increasing amount of beam time is used for experiments. In response to a growing demand on time structures a new pulse suppressor was developed. This was necessary as our cyclotron was originally designed for heavy ions, thus limiting us to repetition rates of 75 kHz for light ions. The pulse suppression is now accomplished completely on the low-energy side, making the pulse suppressor on the high energy side, which was needed for single pulses, superfluous. With this new pulse suppressor the repetition rate of the pulse may be varied from 2 MHz down to 1 Hz or less. The pulse length can be freely chosen from a quasi-continuous beam to single pulses with a pulse width less than 1 ns. The pulses are measured either with a specially developed Faraday cup or non-destructively with a pick-up. The extraction of single pulses surveys very precisely if single turn extraction is achieved. The set-up of the pulse suppressor, measurements on the time structures for various beams and examples of their experimental use will be presented.  
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