High-Resolution Phase-Contrast Imaging at XFELs

We built an x-ray microscope for the Matter in Extreme Conditions (MEC) endstation of the LCLS, which is especially adapted to the XFEL environment, and used the setup to carry out different experiments based on magnified x-ray phase-contrast imaging. The method allows one to image a sample with high spatial resolution and high sensitivity to small density changes within a sample. The xray microscope is based on a set of Beryllium compound refractive lenses (Be-CRLs) creating a secondary x-ray source closely in front of a sample. The sample is positioned in the divergent x-ray beam and a CCD detector records a magnified image of the illuminated area at a larger distance further downstream [cf. Fig. 1 a)]. In a pump-probe scheme an optical laser hits the sample from the side, which initiates a shock wave propagating into the material, and the XFEL pulse probes the state of the material shortly after. In Figs. 1 b) – 1 e) a series of measured phase-contrast images recorded on Kapton at diff t delay times between the optical and XFEL pulse is shown. Larger features such as the position of the shock front and structures behind it can be observed directly in the image. However, due to diffraction effects it is necessary to evaluate the phase-contrast images numerically using phase retrieval methods in order to obtain high-resolution images of the sample. In addition, a quantitative analysis requires a precise knowledge of the illumination wave fi to disentangle features already present in the incoming x-ray beam from the actual object. Beam characterization was carried out using scanning coherent x-ray microscopy (ptychography). The method yields the wave fi distribution of the nano-focused XFEL beam with high spatial resolution (cf. Fig. 2) [3, 4]. In this contribution we report on current activities to implement high-resolution x-ray imaging at the Linac Coherent Light Source (LCLS) [5]. We demonstrate these new capabilities at the example of imaging of shock waves in different materials, outline the analysis procedure and discuss limitations related to fluctuations in beam intensity and position, bandwidth of the XFEL beam [6] and dispersive properties of the x-ray optics.