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Lee, K.

Paper Title Page
MOPEA010 Beam Measurement Experiment of X-band Linac for Compton Scattering X-ray Generation 82
 
  • T. Natsui
    UTNL, Ibaraki
  • K. Lee, M. Uesaka
    The University of Tokyo, Nuclear Professional School, Ibaraki-ken
  • A. Mori
    University of Tokyo, Tokyo
  • F. Sakamoto
    Akita National College of Technology, Akita
 
 

We are developing an X-band linac system for monochromatic X-rays source. The monochromatic X-ray is obtained by Compton scattering. Our system has an X-band (11.424 GHz) 3.5-cell thermionic cathode RF gun, traversing wave accelerating tube and a Q-switch Nd:YAG laser with a wavelength of 532 nm. We adopt a laser pulse circulation system. The RF gun can generate multi-bunch electron beam. We aim to generate 1 μs maximum energy electron beam and collide it to circulated laser pulse. I will present a current status of beam measurement of this linac.

 
MOPEA030 Material Recognition System using 950 keV X-band Linac with Dual Energy X-ray Scintillator Array 130
 
  • K. Lee, S. Hirai, M. Uesaka, T. Yamamoto
    The University of Tokyo, Nuclear Professional School, Ibaraki-ken
  • E. Hashimoto
    JAEA, Ibaraki-ken
  • T. Natsui
    UTNL, Ibaraki
 
 

Dual energy X-ray system using high energy X-ray from linear accelerator (Linac) applies two times X-ray irradiation which have different energy spectrum each other in many cases. Two different X-rays yield two tomography images which is analyzed through numerical calculation with pixel values for material recognition of a object. However if the X-ray generation is not stable, the results of numerical calculation shows irregular tendency during the inspection. We propose the scintillator array in detection part, because two tomography images are obtained by just one irradiation. That leads to the time saving during inspection and the cost down for additional facilities. The optimal condition is researched to increase the ability of material recognition in interesting materials designing the detector with CsI and CdWO4 scintillators. We focus on the discrimination between heavy materials and light materials with the system in the research. X-ray source is 950 keV X-band Linac we developed for industrial application, which produce pulsed X-ray, 10 pps with around 400 mA beam current.

 
MOPE006 Feasibility Study of Radial EO-Sampling Monitor to Measure 3D Bunch Charge Distributions 963
 
  • H. Tomizawa, H. Dewa, H. Hanaki, S. Matsubara, A. Mizuno, T. Taniuchi, K. Yanagida
    JASRI/SPring-8, Hyogo-ken
  • T. Ishikawa, N. Kumagai
    RIKEN/SPring-8, Hyogo
  • K. Lee, A. Maekawa, M. Uesaka
    The University of Tokyo, Nuclear Professional School, Ibaraki-ken
 
 

We are developing a single-shot and non-destructive 3D bunch charge distribution (BCD) monitor based on Electro-Optical (EO) sampling with a manner of spectral decoding for XFEL/SPring-8. For fine beam tuning, 3D-BCD is often required to measure in real-time. The main function of this bunch monitor can be divided into longitudinal and transverse detection. For the transverse detection, eight EO-crystals surround the beam axis azimuthally, and a linear-chirped probe laser pulse with a hollow shape passes thorough the crystal. The polarization axis of the probe laser should be radially distributed as well as the Coulomb field of the electron bunches. Since the signal intensity encoded at each crystal depends on the strength of the Coulomb field at each point, we can detect the transverse BCD. In the longitudinal detection, we utilize a broadband square spectrum (> 400 nm at 800 nm of a central wavelength) so that the temporal resolution is < 30 fs if the pulse width of probe laser is 500 fs. In order to achieve 30-fs temporal resolution, we use an organic EO material, DAST crystal, which is transparent up to 30 THz. We report the first experimental results of this 3D-BCD monitor.