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It could be seen from the XRD patterns of samples with high MoO3 doping content (≥0.05 mol) that X-ray intensities of a particular set of planes, i.e., (004), (006), (008), (0012), (0014), and (0016), were relatively higher than those in the samples with lower MoO3 content.
Using this observation, we group points of maximum curvature to find a set of planes for decomposing the colony into individual nuclei.
θB is the Bragg angle, specific to the set of planes calculated, and θm is the Bragg angle for the monochromator.
The diffraction profile from a set of planes from a perfect crystal is predicted to reveal two peaks, one associated with a mirror reflection and the other associated with the spacing between the planes (Fewster, 2014 ▸).
The AID Ihkl of the diffraction ring for a certain set of planes {hkl} were obtained by radial integration of the 2D-pattern and a localized background subtraction (see SI).
Radial integrations were performed to obtain the azimuthal intensity variations (AID, or pole figures) I hkl (where γ is azimuthal angle on the detector starting in the horizontal plane (see Supporting Information Figure S2)) along the diffraction ring of a specific set of planes.
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They constructed such an isotropic field with a uniform, set of plane waves coming from all directions with the same energy.
The appearance of rings is attributed to set of diffraction planes (1 1 1), (2 0 0), (2 2 0), and (3 1 1) of fcc gold (Figure 2d).
A set of plane mirrors, aligned at right angles to the eye surface, change the direction of rays (in much the same way as len cylinders), thereby producing a single erect image by superposition.
The motion of the plate is assumed composed of a set of plane propagating waves of unknown wavenumber and amplitude.
A set of plane diffuse reflectors is used to direct the radiation onto the lower side of the absorber plate.
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