Author: Saraya, Y.
Paper Title Page
TUM2C03 Commissioning of Heavy-Ion Treatment Facility i-Rock in Kanagawa 130
 
  • E. Takeshita, Y. Kusano, S. Minohara, S. Yamada
    Kanagawa Cancer Center, Ion-beam Radiation Oncology Center in Kanagawa, Kanagawa, Japan
  • T. Furukawa, Y. Hara, K. Mizushima, K. Noda, N. S. Saotome, R. Tansho
    NIRS, Chiba-shi, Japan
  • Y. Saraya
    National Institute of Radiological Sciences, Chiba, Japan
 
  As part of the Kanagawa "Challenge-10-year strategy to cancer" it was decided in March 2005 to establish a carbon-ion therapy system at the Kanagawa Cancer Center (KCC). From around 2009, the basic design and the foundational planning of the facility were considered and in January 2012 a contract was made with the Toshiba Corp. In December of the same year, construction of the main building for the acceleration and treatment devices has been started and completed in October 2014. Currently, the KCC is in a commissioning phase with the aim to start treatment in December this year. Various treatments for cancer, which include four present photon LINAC for the radiation therapy, will be provided to patients in cooperation with our cancer center hospital. In addition, we will combine a compact dissemination treatment system of carbon-ion therapy to the pencil beam 3D scanning technique designed by the National Institute of Radiological Sciences (NIRS). The treatment experience with the carbon-ion scanning technique is expected to be the second in the country following NIRS. In this presentation, we will report on the progress of the beam commissioning of the scanning system.  
slides icon Slides TUM2C03 [19.968 MB]  
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FRM1C01 Present Status of a Superconducting Rotating-Gantry for Carbon Therapy 288
 
  • Y. Iwata, T. Furukawa, Y. Hara, S. Matsuba, S. Mori, K. Noda, S. Sato, T. Shirai, K. Shoda, R. Tansho
    NIRS, Chiba-shi, Japan
  • N. Amemiya
    Kyoto University, Kyoto, Japan
  • H. Arai, T. Fujimoto
    AEC, Chiba, Japan
  • T.F. Fujita, K. Mizushima, Y. Saraya
    National Institute of Radiological Sciences, Chiba, Japan
  • Y. Nagamoto, T. Orikasa, S. Takayama
    Toshiba, Yokohama, Japan
  • T. Ogitsu
    KEK, Ibaraki, Japan
 
  A superconducting rotating-gantry for carbon therapy is being developed. This isocentric rotating gantry can transport carbon ions with the maximum energy of 430 MeV/u to an isocenter with irradiation angles of over 0-360 degrees, and is further capable of performing three-dimensional raster-scanning irradiation. The combined-function superconducting magnets were employed for the rotating gantry. The superconducting magnets with optimized beam optics allowed a compact gantry design with a large scan size at the isocenter; the length and the radius of the gantry are approximately 13 and 5.5 m, respectively, which are comparable to those for the existing proton gantries. Furthermore, the maximum scan size at the isocenter is calculated to be as large as approximately 200 mm square for heavy-ion beams at the maximum energy of 430 MeV/u. A construction and installation of the superconducting gantry is in progress, and beam commissioning will begin from this autumn. We will present a status of the superconducting rotating-gantry.  
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MOPA02 Beam Alignment Procedure for Scanned Ion-Beam Therapy 36
 
  • Y. Saraya, T. Furukawa, Y. Hara, K. Mizushima, K. Noda, N. S. Saotome, T. Shirai, R. Tansho
    NIRS, Chiba-shi, Japan
  • E. Takeshita
    Kanagawa Cancer Center, Ion-beam Radiation Oncology Center in Kanagawa, Kanagawa, Japan
 
  It's important to control the beam position for the 3D pencil-beam scanning because the position accuracy of the beam has a serious matter on the alignment of the irradiation field. In order to suppress this matter, we have been developed a simple procedure for the beam tuning. The fluctuation of the beam position is tuned with the steering magnets (ST) and the fluorescent screen monitors (SCN). At first, the beam positions are measured by two SCN and the kick angles of two ST are calculated using deviates from the center of the beam position measured by SCN and the transfer matrix. After the tuning, the beam position at the isocenter is checked on the verification system for the alignment of the beam consists of the SCN and the iron sphere phantom. If the beam position is deviated from the center, one of ST placed on most downstream of the beam transport line will be corrected. These adjustments are iterated until the deviation for all energies of the beam are within 0.5 mm. We have been performed the beam commissioning using our procedure in Kanagawa Cancer Center. In this presentation, we will report on the result of these measurements.  
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