TY - GEN
T1 - FEL gain measurement with a Novel Method
AU - Fujimoto, Masaki
AU - Kato, Ryukou
AU - Kawase, Keigo
AU - Irizawa, Akinori
AU - Kamitsukasa, Fumiyoshi
AU - Ohsumi, Hiroki
AU - Yaguchi, Masaki
AU - Isoyama, Goro
AU - Kashiwagi, Shigeru
AU - Yamamoto, Shigeru
PY - 2012
Y1 - 2012
N2 - A novel method to measure temporal development of the FEL power has been developed using a silicon bolometer, which response linearly to input over a wide range[1]. The Si bolometer has the time resolution of ∼1 ms, which is much longer than the FEL macropulse of a few μs, so that it measures energy in the macropulse. The number of amplifications is changed by varying the pulse length of electrons from the gun of the linac and energy in the FEL macropulse is measured at a wavelength ∼100 μm with the detector and appropriate Teflon absorbers. The energy development of the FEL macropulse is measured over eight orders of magnitude from a very low power level close to the incoherent radiation up to the FEL power saturation. The temporal development of the FEL power is derived from the energy development as a function of the number of amplifications. Then the FEL gain is derived from the power development. We measured energy development in the macropulse and derived the FEL gain at some cavity lengths. The maximum FEL gain thus evaluated is about 56 percent, which agrees with calculation by the Super-Mode theory.
AB - A novel method to measure temporal development of the FEL power has been developed using a silicon bolometer, which response linearly to input over a wide range[1]. The Si bolometer has the time resolution of ∼1 ms, which is much longer than the FEL macropulse of a few μs, so that it measures energy in the macropulse. The number of amplifications is changed by varying the pulse length of electrons from the gun of the linac and energy in the FEL macropulse is measured at a wavelength ∼100 μm with the detector and appropriate Teflon absorbers. The energy development of the FEL macropulse is measured over eight orders of magnitude from a very low power level close to the incoherent radiation up to the FEL power saturation. The temporal development of the FEL power is derived from the energy development as a function of the number of amplifications. Then the FEL gain is derived from the power development. We measured energy development in the macropulse and derived the FEL gain at some cavity lengths. The maximum FEL gain thus evaluated is about 56 percent, which agrees with calculation by the Super-Mode theory.
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M3 - Conference contribution
AN - SCOPUS:84884369133
SN - 9783954501236
T3 - FEL 2012 - 34th International Free Electron Laser Conference
SP - 515
EP - 518
BT - FEL 2012 - 34th International Free Electron Laser Conference
T2 - 34th International Free Electron Laser Conference, FEL 2012
Y2 - 26 August 2012 through 31 August 2012
ER -