“…Although the energy spread of an electron beam has to be narrow in order to oscillate a free-electron laser (FEL) with an optical klystron, the optical klystron can achieve a high FEL gain given its length. Thus, optical klystrons have been used as an insertion device for the whole storage-ring FEL system (Deacon et al, 1984;Litvinenko, 1988;Couprie et al, 1991;Takano et al, 1993;Yamazaki et al, 1993;Litvinenko et al, 1999;Walker et al, 2001) and have contributed to shorten the FEL wavelength down to the vacuum-ultraviolet region (Litvinenko et al, 2001;Marsi et al, 2002). The characteristics of the optical klystron's spontaneous emission were analyzed by the Novossibirsk group and by the ACO group (Elleaume, 1984a;Vinokurov & Skrinskii, 1977), and these groups reported the results of detailed measurements of the fundamental harmonic spontaneous emission.…”