Author: Campbell, K.
Paper Title Page
THB3CO03 Thermoacoustic Range Verification for Ion Therapy 1265
 
  • S.K. Patch, Y.M. Qadadha
    UWM, Milwaukee, Wisconsin, USA
  • R. Albright, P. Bloemhard, K. Campbell, A.P. Donoghue, T.L. Gimpel, A. Jackson, M.B. Johnson, M. Kireeff Covo, B. Ninemire, L. Phair, C.R. Siero, S.M. Small
    LBNL, Berkeley, California, USA
 
  Funding: We acknowledge support from a UWM Intramural Instrumentation Grant and by the Director, Office of Science, Office of Nuclear Physics, of the U.S. Dept. of Energy under Contract No. DE-AC02-05CH11231.
The potential of particle therapy due to focused dose deposition in the Bragg peak has not yet been fully realized due to inaccuracies in range verification. We report correlation of the Bragg peak location with target structure, by overlaying thermoacoustic localization of the Bragg peak onto a standard ultrasound image. Pulsed delivery of 50 MeV protons was accomplished by a fast chopper installed between the ion source and the inflector of the 88" cyclotron at Lawrence Berkeley National Lab. 2 Gy were delivered in 2 μs by a beam with peak current of 2 μA. Thermoacoustic emissions were detected by a clinical ultrasound array, which also generated a grayscale ultrasound image. Data was collected in a room temperature water bath and gelatin phantom with a cavity designed to mimic the intestine, where gas pockets can displace the Bragg peak. Experiments were performed with the cavity both empty and filled with olive oil. In the waterbath overlays of the Bragg peak agreed with Monte Carlo simulations to within 800±170 μm. Agreement within 1.3 ± 0.2 mm was achieved in the gelatin phantom, for which stopping power was estimated to first order from CT scans.
 
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DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-THB3CO03  
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FRA2IO02 High Precision RF Control for the LCLS-II 1292
 
  • G. Huang, K. Campbell, L.R. Doolittle, J.A. Jones, C. Serrano, V.K. Vytla
    LBNL, Berkeley, California, USA
  • S. Babel, M. Boyes, G.W. Brown, D. Cha, B. Hong, A. Ratti, C.H. Rivetta
    SLAC, Menlo Park, California, USA
  • R. Bachimanchi, C. Hovater, D.J. Seidman
    JLab, Newport News, Virginia, USA
  • B.E. Chase, E. Cullerton, Q. Du, J. Einstein, D.W. Klepec
    Fermilab, Batavia, Illinois, USA
 
  Funding: Work supported by the LCLS-II Project and the U.S. Department of Energy, Contract DE-AC02-76SF00515
The LCLS-II is a CW superconducting linac under construction to drive an X-ray FEL. The energy and timing stability requirements of the FEL drive the need for very high precision RF control. This paper summarize the design considerations and early demonstration of the performance of the components and system we developed.
 
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-FRA2IO02  
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