Nanoradian angular stabilization of x-ray optical components

Stanislav Stoupin; Frank Lenkszus; Robert Laird; Kurt Goetze; Kwang-Je Kim; Yuri Shvyd'ko

doi:10.1063/1.3428722

Nanoradian angular stabilization of x-ray optical components

Rev Sci Instrum. 2010 May;81(5):055108. doi: 10.1063/1.3428722.

Authors

Stanislav Stoupin¹, Frank Lenkszus, Robert Laird, Kurt Goetze, Kwang-Je Kim, Yuri Shvyd'ko

Affiliation

¹ Advanced Photon Source, Argonne National Laboratory, Illinois 60439, USA. sstoupin@aps.anl.gov

PMID: 20515173
DOI: 10.1063/1.3428722

Abstract

An x-ray free-electron laser oscillator (XFELO) has been recently proposed [K. Kim et al., Phys. Rev. Lett. 100, 244802 (2008)]. Angular orientation and position in space of Bragg mirrors of the XFELO optical cavity must be continuously adjusted to compensate for the instabilities and maximize the output intensity. An angular stability of about 10 nrad (rms) is required [K. Kim and Y. Shvyd'ko, Phys. Rev. ST Accel. Beams 12, 030703 (2009)]. To approach this goal, a feedback loop based on a null-detection principle was designed and used for stabilization of a high-energy-resolution x-ray monochromator (DeltaE/E approximately 4 x 10(-8), E=23.7 keV) and a high-heat-load monochromator. Angular stability of about 13 nrad (rms) has been demonstrated for x-ray optical elements of the monochromators.