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The X-ray diffraction patterns of pure Qu, void PMs, physical mixture of void PMs and Qu, and Qu-PMs were obtained by using an X-ray powder diffractometer (Bruker AXS, Madison, WI, USA) at a voltage of 40 kV and 25 mA with a scanned angle from 5° ≤ 2θ ≤ 50° at a scan rate of 0.9 · min-1.
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In fact, with the introduction of frequency increment, the FDA apparent angle will be different from its nominal beam scanning angle.
The microscope images in a raster-scanning pattern with a ±6 degrees (mechanical) scan angle at ~3 kHz in the X-axis (fast) and up to 10 Hz (0 400 μm) in the Z-axis (slow).
For a total scan of 51,200 steps, a scan angle of about 23.3° is acheived.
But underestimation of Pgap from LiDAR amplifies at large off-nadir scan angle.
The corresponding vertical error is quadratic with respect to the scan angle.
High frequency scanning of 55.01 kHz with an optical scan angle of 5.2° is achievable even when operated in air.
The fitted line to the experimental results shows that scan angle changes linearly with the scan length.
Statistical results demonstrate that the scan angle impact is more severe for plots with discontinuous or sparse canopies.
X-ray diffraction patterns were collected on a Rigaku D/MAX-PC 2500 powder X-ray diffractometer, using Cu Kα radiation with scanning angle (2Ѳ) from 20o to 70o.
A polynomial interpolation of the square root of the backscattered signal energy versus scan angle is first plotted.
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