“…One often tries to find a good compromise between detection efficiency, which is dictated by the geometry employed, and overall energy resolution, that is a convolution of several contributions . The latter depends mainly on the intrinsic width of the analyzer Bragg diffraction (given by dynamical diffraction theory), the source size, and how close to backscattering the analyzer is positioned, with other contributions coming from crystal imperfections, broadening due to the stress induced by bending, and errors in the spherical/cylindrical bending radius ,,. In certain cases, the energy bandwidth of the incoming radiation also plays a role in the total resolution, as in the case of resonant XES and HERFD XAS experiments.…”