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Crystal to detector distance varied according to the resolution limits of the crystal.
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In particular: 1) The diffraction image shows spots well past 2.8 A, but the structure was refined only to 3.2 A. Why was it not processed and refined to the diffraction limit of the crystal?
The corresponding solvent content of 67%[25] and the glycosylation content may explain the 2.70 Å diffraction limit of the crystals.
3) Figure 2A: Is the diffraction limit of the crystals related to size?
Inspection of the packing and the resulting map verified the solution; this determines a Matthews coefficient of 6.3 (80.5% solvent content), possibly explaining the observed intrinsic resolution limit of the crystals.
In the limit-ordered regions of the crystal every chain is surrounded by four enantiomorphous and isoclined chains.
Further comparison of inhibitor interactions is limited since the crystal structures of the PRP51-D25N mutare are in the open conformation without inhibitor bound in the standard active site location.
To understand the limits of crystal plasticity models in predicting the microstructural evolution process, simulation data were compared to experimentally observed crystal orientation evolution and strain analyses.
The highest single pulse energy of 1.4 mJ near 2.02 μm was realized in an actively Q-switched solid-state laser, and further power scaling was just limited by the damage of the crystal coating.
The characterization of the mixing process allows for a better understanding of rubrene nanocrystal synthesis: a fast supersaturation induces the generation of numerous nuclei, which limits the crystal growth.
Figure 2 A reveals that the catalytic activity of nondealuminated SP-MOR is limited to the outer surface of the crystal.
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