Abstract

Coherent X-ray photons with energies higher than 50 keV offer new possibilities for imaging nanoscale lattice distortions in bulk crystalline materials using Bragg peak phase retrieval methods. However, the compression of reciprocal space at high energies typically results in poorly resolved fringes on an area detector, rendering the diffraction data unsuitable for the three-dimensional reconstruction of compact crystals. To address this problem, we propose a method by which to recover fine fringe detail in the scattered intensity. This recovery is achieved in two steps: multiple undersampled measurements are made by in-plane sub-pixel motion of the area detector, then this data set is passed to a sparsity-based numerical solver that recovers fringe detail suitable for standard Bragg coherent diffraction imaging (BCDI) reconstruction methods of compact single crystals. The key insight of this paper is that sparsity in a BCDI data set can be enforced by recognising that the signal in the detector, though poorly resolved, is band-limited. This requires fewer in-plane detector translations for complete signal recovery, while adhering to information theory limits. We use simulated BCDI data sets to demonstrate the approach, outline our sparse recovery strategy, and comment on future opportunities.

Highlights

  • The fidelity is quantified by the sparse recovery transfer function (SRTF), which we define for a single recovered image as SRTF(i, j) = Irecovered(i, j)

  • We have described a signal recovery technique for single-crystal Bragg coherent diffraction imaging (BCDI) data sets acquired at X-ray energies typically suited to high-energy diffraction microscopy (HEDM) applications (>50 keV)

  • Our methodology relies on a modification of the conventional BCDI setup in which additional data is acquired by translating the detector perpendicular to the diffracted beam

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Summary

Objectives

We aimed to recover the ground truth within a 120 × 120 pixel region, such that N = 120

Results
Discussion
Conclusion
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