Abstract

rf photoinjectors produce incredibly bright electron beams enabling advanced photon science applications such as the current generation of free electron lasers and high energy x-rays and gamma-rays via laser-Compton scattering. A second generation 5.59 cell $X$-band rf gun has been developed, installed, conditioned, commissioned, tuned, and used to produce laser-Compton x-rays and multiple electron bunches. A charge per bunch from a few pC to 500 pC has been measured, consistent with a quantum efficiency of $5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}$ using a 263 nm 10 Hz photocathode drive laser. The rf gun has operated close to design performance at high gradient, and more reliably at lower gradient achieving a root mean square normalized emittance of 0.3 mm mrad at both 80 pC at $185\text{ }\text{ }\mathrm{MV}/\mathrm{m}$, and 40 pC at $165\text{ }\text{ }\mathrm{MV}/\mathrm{m}$. Thermal emittance is estimated at $0.55\text{ }\text{ }\mathrm{mm}\text{ }\mathrm{mrad}/\mathrm{mm}$. Energy spread of 0.03% has been achieved. These results agree very well with modeling predictions for the operating conditions under which the measurements were made. Unusually disruptive breakdowns were observed with an applied magnetic field of $0.5T$ used for emittance compensation.

Highlights

  • The latest generation of light sources has been made possible by the advances in peak electron brightness due to modern rf photoinjectors [1,2]. rf guns offer low emittance beams that can be accelerated to the necessary operating energy to lower the geometric emittance, and temporally compressed to the required peak current for free-electron laser (FEL) operation [3,4,5]

  • At Lawrence Livermore National Laboratory (LLNL), X-band accelerator technology has been developed to enable laser-Compton light sources spanning a wide range of x-ray and gamma-ray energies in a system that fits in a small laboratory space

  • An emittance of 0.3 mm mrad and an energy spread of 0.03% are expected at 30 MeV for a 100 pC bunch, which requires the use of the Mark 1 rf gun and a single T53 accelerator structure operating at 45 MV=m [35]

Read more

Summary

INTRODUCTION

The latest generation of light sources has been made possible by the advances in peak electron brightness due to modern rf photoinjectors [1,2]. rf guns offer low emittance beams that can be accelerated to the necessary operating energy to lower the geometric emittance, and temporally compressed to the required peak current for free-electron laser (FEL) operation [3,4,5]. The photons that are produced can be collimated to produce narrow bandwidth x-rays and gamma-rays with a source size and bandwidth limited by the electron beam quality Examples of such facilities are the high intensity gammaray source (HIGS) [11], and the under construction Extreme Light Infrastructure Nuclear Physics GammaBeam System in Romania (ELI-NP GBS) [12]. The X-band photoinjector [22] discussed here was originally designed to serve as the electron source for the VELOCIRAPTOR, and LLNL commissioned the MEGa-ray (Mono-Energetic Gammaray) Test Station (MTS) to leverage hardware in hand into a platform for developing the critical technologies. Conclusions include an outline of major improvements and design considerations for the generation X-band photoinjector, i.e. a Mark 2 rf gun

Source
Testing
Distribution
25 MHz OFHC Copper
ACCELERATOR
PHOTOCATHODE LASER
MEASUREMENTS
Quantum efficiency
Emittance
Energy
CONCLUSION
Outlook
Findings
Facility
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call