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ERL-FELからのチャープパルス計測

Measurement of a chirped pulse generation from the ERL-FEL

飯島 北斗; 羽島 良一; 永井 良治; 峰原 英介; 山内 俊彦

Iijima, Hokuto; Hajima, Ryoichi; Nagai, Ryoji; Minehara, Eisuke; Yamauchi, Toshihiko

原研・光量子科学研究センター・FELグループはエネルギー回収型超伝導加速器(ERL)を用いた遠赤外超短パルス高出力FELの開発を進めてきた。この加速器から発振される波長約20$$mu$$mのチャープされたFELは、例えば多原子分子の解離などに応用した場合、現状の技術よりも飛躍的に高い解離効率が期待される。これまでの研究で、波長23.3$$mu$$m,パルス幅319fs(FWHM),チャープ量$$Deltaomega/omega_0$$=14.3%のFEL発振に成功し、これを自己相関により測定した。現在はこのチャープされたFELの時間と周波数の相関を直接観測するために、frequency-resolved optical grating (FROG)による計測の準備を進めている。加えて、FEL光輸送系の構築も行った。

We report the construction of FEL transport line and the measurement method of chirped FEL pulse. An infrared-chirped pulse is an effective way of dissociating molecules. The chirped FEL pulse oscillator is operated by the JAERI-FEL superconducting accelerator, in which a long pulse of electron beam is produced. Until now, the chirped pulse was measured to be $$Deltaomega/omega_0$$ = 14.3% with the wavelength of 23.3 $$mu$$m and the pulse width of 319 fs at FWHM by an autocorrelation. In order to measure the correlation between time and frequency in the chirped pulse directly, the frequency-resolved optical grating (FROG) is developing. Since the measurement is performed in new experimental room, the vacuum transport line guiding the FEL to the room has been constructed.

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