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Generation of time-synchronized two-color X-ray free-electron laser pulses using phase shifters.
Cho, Myung-Hoon; Kang, Teyoun; Yang, Haeryong; Kim, Gyujin; Kwon, Seong-Hoon; Moon, Kook-Jin; Nam, Inhyuk; Min, Chang-Ki; Heo, Hoon; Kim, Changbum; Kang, Heung-Sik; Shim, Chi Hyun.
Affiliation
  • Cho MH; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea. mh0309@postech.ac.kr.
  • Kang T; Department of Physics and Earth Science, Korea Science Academy of KAIST, Busan, 47162, Korea.
  • Yang H; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Kim G; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Kwon SH; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Moon KJ; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Nam I; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Min CK; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Heo H; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Kim C; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Kang HS; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea.
  • Shim CH; Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang, 37673, Korea. sch0914@postech.ac.kr.
Sci Rep ; 13(1): 13786, 2023 Aug 23.
Article in En | MEDLINE | ID: mdl-37612325
ABSTRACT
To optimize the intensity of X-ray free-electron lasers (XFELs), phase shifters, oriented in phase with the phases of the XFEL pulse and electron beam, are typically installed at undulator lines. Although a π-offset between the phases (i.e., an "out-of-phase" configuration) can suppress the XFEL intensity at resonant frequencies, it can also generate a side-band spectrum, which results in a two-color XFEL pulse; the dynamics of such a pulse can be described using the spontaneous radiation or low gain theory. This attributes of this two-color XFEL pulse can be amplified (log-scale amplification) through an undulator line with out-of-phase phase shifters. In this study, the features of two-color XFEL pulses were evaluated through theory, simulations and experiments performed at Pohang Accelerator Laboratory X-ray Free Electron Laser. The XFEL gain slope and energy separation between the two-color spectral peaks were consistent through theoretical expectation, and the results of simulation and experiment. The experimentally determined two-color XFEL pulse energy was 250 µJ at a photon energy of 12.38 keV with a separation of 60 eV.