Abstract

To achieve the lowest emittance electron bunches from photoemission electron guns, it is essential to limit the uncorrelated emittance growth due to space charge forces acting on the bunch in the vicinity of the photocathode through appropriate temporal shaping of the optical pulses illuminating the photocathode. We present measurements of the temporal profile of electron bunches from a bulk crystal GaAs photocathode illuminated with 520 nm wavelength pulses from a frequency-doubled Yb-fiber laser. A transverse deflecting rf cavity was used to make these measurements. The measured laser pulse temporal profile and the corresponding electron beam temporal profile have about 30 ps FWHM duration, with rise and fall times of a few ps. GaAs illuminated by 520 nm optical pulses is a prompt emitter within our measurement uncertainty of $\ensuremath{\sim}1\text{ }\text{ }\mathrm{ps}\text{ }\mathrm{rms}$. Combined with the low thermal emittance of negative electron affinity photocathodes, GaAs is a very suitable photocathode for high-brightness photoinjectors. We also report measurements of the photoemission response time for GaAsP, which show a strong dependence on the quantum efficiency of the photocathode.

Highlights

  • Novel accelerator applications based on the energy recovery linac (ERL) concept [1,2,3,4] require an electron source delivering both high average current and low beam emittance

  • Photoemission electron guns with high quantum efficiency (QE) cathode materials provide a natural route to meeting the requirements of an ERL injector

  • The negative electron affinity (NEA) class of photocathodes is of particular interest given their low thermal emittance [5] and high QE

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Summary

INTRODUCTION

Novel accelerator applications based on the energy recovery linac (ERL) concept [1,2,3,4] require an electron source delivering both high average current and low beam emittance. Photoemission electron guns with high quantum efficiency (QE) cathode materials provide a natural route to meeting the requirements of an ERL injector. The negative electron affinity (NEA) class of photocathodes is of particular interest given their low thermal emittance [5] and high QE. For illumination by a short duration laser pulse with a top-hat transverse profile, this is given by s. Equation (1) represents the lowest possible normalized emittance in the case of space charge limited extraction from the cathode.

EXPERIMENTAL SETUP
TEMPORAL PULSE SHAPING
PHOTOCATHODE RESPONSE TIME
DISCUSSION AND SUMMARY
Findings
Methods
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