Figure 8
Rocking curves of (a) the diamond splitter via one of the beamlets diffracted by the (113) Laue planes with 17.5° asymmetry, (b) the germanium recombiner via diffraction on the (660) Bragg planes with 10° asymmetry. (a) is normalized by the intensity of the direct beam before the splitter, while (b) is normalized by the intensity of the beamlet emerging from the splitter. The error bars are calculated by combining the noise of the detector and the quantum noise for the direct beam, the beamlet after the splitter, or after the recombiner. |