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Simulated X-ray Diffraction and Machine Learning for Interpretation of Dynamic Compression Experiments.
Abstract not provided.
X-ray diffraction of material under ramp compression on the Thor pulsed-power generator.
Abstract not provided.
Temperature-dependent x-ray diffraction of thermographic phosphors.
Abstract not provided.
Electron Backscatter Diffraction Analysis of Additively Manufactured Steel Grains.
Abstract not provided.
Structures and equation of state of gadolinium using in-situ x-ray diffraction.
Abstract not provided.
Electron Backscatter Diffraction of Low Symmetry Metals and Alloys
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CHARACTERIZATION OF MOS2 FILMS VIA SIMULTANEOUS GRAZING INCIDENCE X-RAY DIFFRACTION AND GRAZING INCIDENCE X-RAY FLUORESCENCE (GIXRD/GIXRF)
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Dynamic x-ray diffraction of shock compressed carbon phase transformations on Sandia’s Z Pulsed Power Facility
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Dynamic x-ray diffraction of materials under ramp compression on the Thor pulsed-power generator
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Temperature-dependent x-ray diffraction of thermographic phosphors
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Alpha-Quartz Plastic Strength Investigation Via Diffraction Experiments on Novaculite Using A D-Dia and Elastic Plastic Self- Consistent Interpretation [Thesis}
X-Ray Tomography. Porosity is commonly measured using mercury injection (MI) or water immersion porosimeter (WIP). Both MI and WIP utilize pressure to fill open voids with mercury or water respectively. A measure of the volume change of the sample is then used to estimate the percentage of open voids. However, for the purpose of rheological study it is important to get an accurate measure of open and closed voids. X-ray tomography has been selected as it offers a three-dimensional view into the sample that can quantify all pores limited only by the voxel size which is in the micron range for this study. Radiographs for tomography were collected at the Material Science and Technology Division at Los Alamos National Lab using the Carl Zeiss Xradio 520 instrument and Scout-and-Scan version 16.1 operating software. Two samples were imaged, the starting material and the deformed sample SiO2_65. 3001 radiographs were taken of the starting material with a 6 second exposure time using a 4x objective lens. The x-ray beam was set to 60 kilovoltage peak (kVp) and 5 watts. 1901 radiographs were taken of SiO2_65 with a 25 second exposure time using a 10x objective lens. The x-ray beam was set to 80 kVp and 7 watts. Radiograph files were analyzed by Brian Patterson using Avizo. Void and inclusion volumes were output by voxel sized (1.03 μm) slices, used to calculate a total percentage volume for the starting material.
CsPbBr3 phase transition using neutron diffraction data
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Update of X-ray Diffraction on Z and Thor
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Diffraction at the LHCb Experiment
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Effect of Dry Electropolishing on the Electron Backscatter Diffraction Mapping of Dissimilar Titanium Welds
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Laser-irradiated X-ray sources for X-ray diffraction of dynamically compressed matter on Sandia's Z-Machine
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