• Title of article

    Grid pulser for an electron gun with a thermionic cathode for the high-power operation of a terahertz free-electron laser

  • Author/Authors

    Suemine، نويسنده , , Shoji and Kawase، نويسنده , , Keigo and Sugimoto، نويسنده , , Naoya and Kashiwagi، نويسنده , , Shigeru and Furukawa، نويسنده , , Kazuya and Kato، نويسنده , , Ryukou and Irizawa، نويسنده , , Akinori and Fujimoto، نويسنده , , Masaki and Ohsumi، نويسنده , , Hiroki and Yaguchi، نويسنده , , Masaki and Funakoshi، نويسنده , , Sousuke and Tsutsumi، نويسنده , , Ryouta and Kubo، نويسنده , , Kumiko and Tokuchi، نويسنده , , Akira and Isoyama، نويسنده , , Goro، نويسنده ,

  • Issue Information
    روزنامه با شماره پیاپی سال 2015
  • Pages
    7
  • From page
    97
  • To page
    103
  • Abstract
    A grid pulser for a thermionic-cathode electron gun for an L-band electron linac with an RF frequency of 1.3 GHz was developed in an effort to increase the power of a terahertz (THz) free-electron laser (FEL) based on the linac. The grid pulser can generate a train of electron pulses with a 5-ns duration at intervals of 36.9 ns or at a repetition frequency of 27 MHz, which is the 48th sub-harmonic of the RF frequency, and with a peak current of up to 2.4 A or higher, which is four times higher than the current that can be obtained with the conventional grid pulser. In combination with the sub-harmonic buncher (SHB) system, whose fundamental frequency is 108 MHz (the 12th sub-harmonic of the RF frequency), an electron beam that comprises electron bunches separated by 36.9-ns intervals for a period of 8 μs can be successfully accelerated using the linac to an energy of 15 MeV under the condition that the average beam current or, correspondingly, the beam loading in the acceleration tube of the linac is the same as that obtained using the conventional grid pulser. The time-resolved energy spectrum indicates that the energy is constant over the latter 6 μs and that the energy spread is 1.2% (FWHM); this performance satisfies the requirements for the FEL. The bunch charge measured at the end of the FEL beamline is 4 nC, which is four times higher than that obtained using the conventional grid pulser.
  • Keywords
    Free-electron lasers , Thermionic cathode , Electron linear accelerator
  • Journal title
    Nuclear Instruments and Methods in Physics Research Section A
  • Serial Year
    2015
  • Journal title
    Nuclear Instruments and Methods in Physics Research Section A
  • Record number

    2197038