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Abstract
The multi-scale characterization of building materials is necessary to understand complex mechanical processes, with the goal of developing new more sustainable materials. To that end, imaging methods are often used in materials science to characterize the microscale. However, these methods compromise the volume of interest to achieve a higher resolution. Dark-field (DF) contrast imaging is being investigated to characterize building materials in length scales smaller than the resolution of the imaging system, allowing a direct comparison of features in the nano-scale range and overcoming the scale limitations of the established characterization methods. This work extends the implementation of a dual-phase X-ray grating interferometer (DP-XGI) for DF imaging in a lab-based setup. The interferometer was developed to operate at two different design energies of 22.0 keV and 40.8 keV and was designed to characterize nanoscale-size features in millimeter-sized material samples. The good performance of the interferometer in the low energy range (LER) is demonstrated by the DF retrieval of natural wood samples. In addition, a high energy range (HER) configuration is proposed, resulting in higher mean visibility and good sensitivity over a wider range of correlation lengths in the nanoscale range. Its potential for the characterization of mineral building materials is illustrated by the DF imaging of a Ketton limestone. Additionally, the capability of the DP-XGI to differentiate features in the nanoscale range is proven with the dark-field of Silica nanoparticles at different correlation lengths of calibrated sizes of 106 nm, 261 nm, and 507 nm.
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1 Ghent University, Radiation Physics Research group, Department Physics and Astronomy, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); Ghent University, Centre for X-ray Tomography, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); Ghent University, UGent‑Woodlab, Department of Environment, Faculty of Bioscience Engineering, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); Ghent University, Pore-Scale Processes in Geomaterials Research Group (PProGRess), Department of Geology, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); ETH Zurich, Institute for Biomedical Engineering, Zurich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780)
2 Ghent University, Radiation Physics Research group, Department Physics and Astronomy, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); Ghent University, Centre for X-ray Tomography, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798)
3 ETH Zurich, Institute for Biomedical Engineering, Zurich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780); Paul Scherrer Institute, Swiss Light Source, Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
4 Paul Scherrer Institute, Swiss Light Source, Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
5 National Institute of Standards and Technology, Materials Science and Engineering Division, Gaithersburg, USA (GRID:grid.94225.38) (ISNI:0000 0001 2158 463X)
6 Ghent University, Centre for X-ray Tomography, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); Ghent University, UGent‑Woodlab, Department of Environment, Faculty of Bioscience Engineering, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798)
7 Ghent University, Centre for X-ray Tomography, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798); Ghent University, Pore-Scale Processes in Geomaterials Research Group (PProGRess), Department of Geology, Ghent, Belgium (GRID:grid.5342.0) (ISNI:0000 0001 2069 7798)