doi:10.1016/S0168-9002(01)01639-4
Copyright © 2001 Elsevier Science B.V. All rights reserved.
First measurements of subpicosecond electron beam structure by autocorrelation of coherent diffraction radiation*1
A. H. Lumpkin
,
, a, N. S. Serenoa and D. W. Ruleb
a Advanced Photon Source, Bldg. 32, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, IL 60439, USA
b Carderock Division, Naval Surface Warfare Center, West Bethesda, MD, USA
Available online 17 December 2001.
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Abstract
We report the initial measurements of subpicosecond electron beam structure using a nonintercepting technique based on the autocorrelation of coherent diffraction radiation (CDR). A far infrared (FIR) Michelson interferometer with a Golay detector was used to obtain the autocorrelation. The radiation was generated by a thermionic rf gun beam at 40 MeV as it passed through a 5-mm-tall slit/aperture in a metal screen whose surface was at 45° to the beam direction. For the observed bunch lengths of about 450 fs (FWHM) with a shorter time spike on the leading edge, peak currents of about 100 A are indicated. Also a model was developed and used to calculate the CDR from the back of two metal strips separated by a 5-mm vertical gap. The demonstrated nonintercepting aspect of this method could allow on-line bunch length characterizations to be done during free-electron laser experiments.
Author Keywords: Bunchlength; Subpicosecond; Coherent diffraction radiation
Fig. 1. A schematic of the initial portion of the injection linac for the APS. In these experiments the beam from thermionic RF gun #2 was accelerated to 40 MeV by the L2-AS1 accelerating structure after which the diagnostics station was located (courtesy of J. Lewellen, ANL).
Fig. 2. Schematic of geometry for diffraction radiation production by two finite width, infinitely long, reflecting strips. Here the y-axis is in the plane containing the velocity vector v and the normal to the plane of the aperture. Radiation is emitted in the direction of k.
Fig. 3. Calculated spectra of CDR from a slit for a 50-MeV electron beam with 8 nC total charge and bunch lengths of σt=0.2, 0.5, 1.0, 3.0 and 6.0 ps.
Fig. 4. The CDR autocorrelation from the FIR interferometer. Note the horizontal scale of mirror position in μm would be doubled for optical path difference.
Fig. 5. The amplitude spectrum derived from the autocorrelation and corrected spectrum at long wavelength (low wavenumber).
Fig. 6. Longitudinal bunch profiles derived from the corrected autocorrelation amplitude spectrum using CTR (upper) and using CDR (lower). The bunch distribution is sub-0.5 ps (FWHM) for the 40-MeV beam.
Table 1. APS linac beam properties at Station-1 in the low-emittance mode (RF Thermionic Gun)
