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Otake, Y.

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MOP079 Development of Modulating Permanent Magnet Sextupole Lens for Focusing of Pulsed Cold Neutrons 263
 
  • M. Yamada, H. Fujisawa, M. Ichikawa, Y. Iwashita, H. Tongu
    Kyoto ICR, Uji, Kyoto
  • P. Geltenbort
    ILL, Grenoble
  • K. Hirota, Y. Otake, H. Sato
    RIKEN, Wako, Saitama
  • T. Ino, K. Mishima, T. Morishima, S. Mutou, H.M. Shimizu, K. Taketani
    KEK, Tsukuba
  • Y. Kamiya, S. Kawasaki, S. Komamiya, H. Otono, S. Yamashita
    University of Tokyo, Tokyo
  • T. Oku, K. Sakai, T. Shinohara, J. Suzuki
    JAEA, Ibaraki-ken
  • Y. Seki
    Kyoto University, Kyoto
  • T. Yoshioka
    ICEPP, Tokyo
 
 

We are developing a modulating permanent magnet sextupole lens to focus pulsed cold neutrons. It is based on the extended Halbach configuration to generate stronger magnetic field. In order to adjust the strength, the magnet is divided into two nested co-axial rings, where the inner ring is fixed and the outer ring can be rotated. Synchronizing the modulation with neutron beam pulse suppresses the chromatic aberration. These devices largely improve the utilization efficiency of neutrons, which makes even small linac based neutron sources practical. We have fabricated a half-scale model and studied its strength, torque and temperature rise during the operation. The main causes of the temperature rise are eddy-current loss in the poles made of soft magnetic material in inner ring and hysteresis loss. A laminated structure reduced the eddy-current loss. The temperature rise was suppressed to about half of the former model. We now study their B-H curve to optimize the thickness of the sheet. Annealing of the material is supposed to reduce the hysteresis loss, which will be tested soon. The experimental results of very-cold neutrons focusing with the half-scale model are also described.

 

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TUP077 Development of Screen Monitor with a Spatial Resolution of Ten Micro-meters for XFEL/SPring-8 573
 
  • K. Yanagida, H. Tomizawa, A. Yamashita
    JASRI/SPring-8, Hyogo-ken
  • S.I. Inoue, Y. Otake
    RIKEN/SPring-8, Hyogo
 
 

At SPring-8, the 8 GeV linac for an X-ray free electron laser (XFEL) is now under construction. In order to realize the XFEL, highly qualified electron beams are required. A measurement of spatial structure of such beam is very important for the beam tuning of XFEL. The spatial structure is measured with a screen monitor, which we now develop. The resolution of the measurement is required within 10 um. The screen monitor comprises a vacuum chamber with a thin metal (100 um, SUS) foil to emit OTR, lenses for focusing and a CCD camera system. The main feature of the monitor is a bright and high-resolution optical system. In order to realize this system, the lenses are placed close to the foil, the distance between the lenses and the foil is 100 mm, and the lenses have a large diameter (2 in.). This optical-geometrical structure also contributes much to reduce the airy radius of a near field image. Although the range of an observation wavelength is wide as which is form 400 to 800 nm, the resolution of the measurement on the foil is calculated as 2.5 um. The experimental data of the developed screen monitor also suggested the same resolution.

 
THP104 Low Level RF and Timing System for XFEL/SPring-8 1036
 
  • T. Ohshima, N. Hosoda, H. Maesaka, Y. Otake
    RIKEN/SPring-8, Hyogo
  • M. Musha
    University of electro-communications, Tokyo
  • K. Tamasaku
    RIKEN Spring-8 Harima, Hyogo
 
 

Requirement on a Low Level rf (LLRF) system is very tight and allowable jitter is less than several tens femto seconds for the XFEL/SPring-8. To satisfy this requirement, we have developed special components; a low-noise master oscillator, a high precision IQ modulator/demodulator, a high speed DAC/ADC, and a delayed pulse generator with 700 fs jitter to a 5712 MHz reference clock. These components were installed in the SCSS test accelerator and their performance was checked. The standard deviations of the phase and amplitude were less than 0.02 degree and 0.03% for a 238 MHz SHB acceleration cavity. Measured rms jitter of the beam arrival time relative to the reference rf signal was 50 fs, which demonstrated the high performance of the total LLRF system. For the XFEL, the length of reference signal transmission line is long, about 1 km. Therefore an optical system is adopted because of low transmission loss and an ability to keep precise time accuracy using fiber length control, which has 0.2 um/sqrt(Hz) noise floor. Achieved performance of the LLRF and timing system, and development status on the optical transmission system will be presented in this paper.

 

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