REGAE

| Time resolved diffraction with relativistic electrons

REGAE accelerator

Time resolved diffraction with relativistic electrons

REGAE accelerator

REAGE provides electron beams of outstanding quality and stability to perform 3D structural analysis and pump-probe type experiments on quantum materials and biological samples.

Figure 1: Overview of the REGAE accelerator.

Figure 1: Overview of the REGAE accelerator.

REGAE employs an S-band photocathode RF gun to produce electron bunches of typically 100 fC charge with a normalized emittance of about 20 nm {DOI: 10.1016/j.nima.2016.01.065} at an energy of 3 – 5 MeV. Focusing solenoids, beam steering and diagnostics elements are distributed along the beam line and give a high flexibly of the transverse beam optics to adjust the beam parameters according to experimental demands. Figure 1 displays a schematic overview of the electron accelerator. By means of a buncher cavity the initial bunch length can be compressed to below 20 fs at the sample position. The bunch length is presently limited by the available S-band Transverse Deflecting Structure (TDS) for bunch length measurements {DOI:10.1088/1742-596/1238/1/012069|, while in simulations bunch lengths to below 1 fs have been reached {DOI: 10.1103/PhysRevSTAB.18.120102}. In the so-called stretcher mode, the buncher cavity can be tuned in a way to reduce the relative energy spread of bunches down to about 10-5 for comparatively long bunches.

Figure 2: The S-band TDS with optimized geometry is powered by a 5 kW RF amplifier and achieves a resolution of ~20 fs.

Figure 2: The S-band TDS with optimized geometry is powered by a 5 kW RF amplifier and achieves a resolution of ~20 fs.

Efforts to develop a bunch length measurement system with higher resolution are ongoing {https://accelconf.web.cern.ch/ipac2017/papers/mopab052.pdf}. The bunch repetition rate of REGAE is presently limited to 12.5 Hz due to an interference with magnetic fields from the nearby operating DESY synchrotron.