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note
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Before carrying out computer simulation, we first determine the coordinates of the center of each elongated diffraction spot in the experimental diffraction pattern. The orientation of a crystallite is characterized by Euler angles θ, φ, and ψ. In calculation the wavelength of X-ray is set between 0.7 and 2.2 Å. θ, φ and ψ are changed with a step of 2 mRod. This step size corresponds to a linear separation of about 50 microns in the diffraction spectrum in our experiment. At each step the diffraction pattern is calculated and compared with the experimental data. Once a bestfit combination of θ, φ, and ψ is found, we continue to determine the axis of the orientation rotation and the degree that the crystallite has been rotated in a similar way. If the computed direction of the spot elongation is in agreement with the experimental observation, we conclude that the correct axis of rotation has been found. It is noteworthy that the noise-to-signal ratio in our experiments is not high, so many high-indexed diffraction spots cannot be identified. As a matter of fact, the analysis of the diffraction spots on the image plate shows that the diffraction coming from hkl > 2 is so weak that those spots are virtually not seen. For this reason we only consider hkl ≤ 2in the computer calculation.
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23
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0012738733
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note
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→, respectively.
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25
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0003905979
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0012678692
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When the supersaturation is higher than 0.2, it has been found 〈111〉 is the fast growth direction. See ref 26 for details
-
When the supersaturation is higher than 0.2, it has been found 〈111〉 is the fast growth direction. See ref 26 for details.
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31
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23544444002
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