• High Power Laser Science and Engineering
  • Vol. 4, Issue 1, 010000e1 (2016)
Zhuoran Ma1、2, Zhe Wang1、2, Feichao Fu1、2, Rui Wang1、2, and Dao Xiang1、2、*
Author Affiliations
  • 1Key Laboratory for Laser Plasmas (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 2IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
  • show less
    DOI: 10.1017/hpl.2015.35 Cite this Article Set citation alerts
    Zhuoran Ma, Zhe Wang, Feichao Fu, Rui Wang, Dao Xiang. Generating quasi-single-cycle THz pulse from frequency-chirped electron bunch train and a tapered undulator[J]. High Power Laser Science and Engineering, 2016, 4(1): 010000e1 Copy Citation Text show less
    (a) Radiation field of a single bunch; (b) superposition of radiation fields from the whole electron beam (eight bunches). (c) Total radiation field from the eight bunches. The horizontal axis is the longitudinal position normalized to the radiation wavelength (bunch head to the left) and the vertical axis is the amplitude of the radiation field normalized to that of a single bunch.
    Fig. 1. (a) Radiation field of a single bunch; (b) superposition of radiation fields from the whole electron beam (eight bunches). (c) Total radiation field from the eight bunches. The horizontal axis is the longitudinal position normalized to the radiation wavelength (bunch head to the left) and the vertical axis is the amplitude of the radiation field normalized to that of a single bunch.
    (a) Frequency-chirped radiation from a single bunch; (b) superposition of radiation fields from the whole electron beam (eight bunches). (c) Total radiation field from the eight bunches.
    Fig. 2. (a) Frequency-chirped radiation from a single bunch; (b) superposition of radiation fields from the whole electron beam (eight bunches). (c) Total radiation field from the eight bunches.
    (a) Frequency-chirped radiation from a single bunch; (b) superposition of radiation fields from the whole electron beam (chirped bunches). (c) Total radiation field from the chirped bunches when the bunch chirp matches the undulator tapering.
    Fig. 3. (a) Frequency-chirped radiation from a single bunch; (b) superposition of radiation fields from the whole electron beam (chirped bunches). (c) Total radiation field from the chirped bunches when the bunch chirp matches the undulator tapering.
    (a) Difference in time-of-flight for electrons launching at various rf phases in a photocathode rf gun; (b) compression ratio of the electron bunch launching at various rf phases.
    Fig. 4. (a) Difference in time-of-flight for electrons launching at various rf phases in a photocathode rf gun; (b) compression ratio of the electron bunch launching at various rf phases.
    (a) Measured frequency-chirped electron bunch train (bunch head to the left); (b) separation of the bunch train.
    Fig. 5. (a) Measured frequency-chirped electron bunch train (bunch head to the left); (b) separation of the bunch train.
    Zhuoran Ma, Zhe Wang, Feichao Fu, Rui Wang, Dao Xiang. Generating quasi-single-cycle THz pulse from frequency-chirped electron bunch train and a tapered undulator[J]. High Power Laser Science and Engineering, 2016, 4(1): 010000e1
    Download Citation