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Shintake, T.

Paper Title Page
MOOBI2 XFEL/SPring-8 Construction and SCSS Operation Status 20
 
  • T. Shintake
    RIKEN/SPring-8, Hyogo
 
 

XFEL/SPring-8 construction was started in 2006, aiming at generating X-ray laser at 1 Angstrom. The building construction was completed in April 2009, followed by installation of accelerator components. In March 2010, we completed all accelerating structure installation. The klystron modulator and LLRF systems are under installation. We use 19 undulator of in-vacuum type (5 m each). At this moment 10 undulators have been installed and careful qualification of undulator field is carried out. We will start high power processing in this October, and we will send the first electron beam into beam dump before April 2011, followed by beam commissioning for X-ray lasing.

 

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MOOAI7 First Observation of the 61.5 nm Seeded FEL at the SCSS Test Accelerator 13
 
  • T. Togashi, K. Fukami, S. Matsubara, H. Ohashi, H. Tomizawa, T. Watanabe
    JASRI/SPring-8, Hyogo-ken
  • M. Aoyama, K. Yamakawa
    JAEA/Kansai, Kyoto
  • M.-E. Couprie
    SOLEIL, Gif-sur-Yvette
  • T. Hara, T. Hatsui, T. Ishikawa, T.K. Kameshima, H. Kitamura, N. Kumagai, M. Nagasono, Y. Otake, T. Shintake, H. Tanaka, T. Tanaka, K. Togawa, M. Yabashi
    RIKEN/SPring-8, Hyogo
  • A. Iwasaki, T. Okino, S. Owada, T. Sato, K. Yamanouchi
    The University of Tokyo, Tokyo
  • F. Kannari
    Keio University, Kanagawa-ken
  • K. Midorikawa, E. Takahashi
    RIKEN, Saitama
  • H. Nakano
    NTT Corp., Kanagawa-ken
  • A. Yagishita
    KEK, Tsukuba
 
 

A seeded FEL is the most promised way to generate fully coherent radiation in a short-wavelength region. After the improvement of the laser and HHG system at the SCSS test accelerator, we have succeeded the amplification of the seed, for the first time, in the plateau region. The wavelength of the seed is 61.5 nm, which is the 13th harmonic of a Ti:Sa laser, and clear intensity increase and spectral narrowing by the FEL was observed. Although there still remains room for optimization of the transverse matching and synchronization of the seed, this result leads to realization of a fully coherent light source to users in VUV and soft x-ray regions.

 

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WEOC3 Construction of 8-GeV C-band Accelerator for XFEL/SPring-8 525
 
  • T. Inagaki, T. Hasegawa, H. Maesaka, T. Ohshima, Y. Otake, T. Shintake
    RIKEN/SPring-8, Hyogo
  • C. Kondo, T. Sakurai, K. Shirasawa
    JASRI/SPring-8, Hyogo-ken
 
 

An 8-GeV C-band (5712 MHz) accelerator is employed as a main accelerator for XFEL/SPring-8. Since a C-band accelerating structure generates a high accelerating gradient of higher than 35 MV/m, the total length of the accelerator fits within 400 m, including the injector and three bunch compressors. We use 64 C-band rf units, which consist of 128 accelerating structures, 64 rf pulse compressors and waveguide components, 64 klystrons and modulators, etc. Mass-production of the C-band rf components has been done by several Japanese manufacturers. The components reliability has been improved during the production, and all the components finally have excellent quality. The production quality was also confirmed by a high power rf test. We achieved the accelerating gradient of 40 MV/m without any problem. Since XFEL realizes high bunch compression with precise control of the energy chirp, the rf should be quite stable. We developed a high precision high voltage charger combined with a low-noise klystron modulator. The pulse-to-pulse stability of the PFN voltage was less than 0.01%. Installation of the components started in August 2009 and was now almost completed on schedule.

 

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