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Togawa, K.

Paper Title Page
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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Slides

 
MOPC02 Beam Optics and Parameter Design of the XFEL/SPring-8 Accelerator 111
 
  • T. Hara, H. Tanaka, K. Togawa
    RIKEN/SPring-8, Hyogo
 
 

The commissioning of the XFEL/SPring-8 facility is scheduled in the spring of 2011. Since the accelerator of XFEL/SPring-8 uses a thermionic gun with an 1 A initial beam current, the total bunch compression ratio reaches about 3000, which is one order higher than a photocathode system. For nonlinearity compensation in the bunch compression, two correction cavities are installed, which are operated at the same frequency as the linac and not at its higher-harmonic. A large compression ratio, particularly at the velocity bunching, results in larger projected parameters of the electron bunch compared to its slice values. The transverse optics of the accelerator is designed for the projected parameters using newly introduced linear formulation of the beam envelope including acceleration effects. The beam optics of the main linac and undulator sections are based on a FODO-like lattice and additional quadrupole magnets are installed at each chicane for dispersion correction. In this presentation, the XFEL/SPring-8 accelerator layout and its expected beam parameters are shown to achieve the 0.1 nm X-ray FEL.