Figure 4
(a) A two-dimensional detector frame recorded close to the (113)pc reciprocal lattice vector accumulated at a selected position on the sample. The feature P0 corresponds to the crystal truncation rod of the sample, while P1 and P2 are caused by the lateral periodicity of the domains along . The dashed areas mark the regions of intensity integration. (b) The integrated intensity of P0 as a function of the vertical scattering vector component Qz. (c), (d) Integrated (113)pc intensity maps (5 × 5 µm) of (c) P1 and (d) P2 in real space. |