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By solving the scalar wave equation, we obtain the dispersion relation for photonic crystal i (i.e. i = A, B or C) as (1).
The mixed crystal i.r.r
The electron diffraction (ED) pattern shows Bragg reflection spots attributed to anthracene crystal, i.e., anthracene molecules never broke during evaporation.
A byproduct of indexing is to determine the symmetry of the crystal, i.e., its space group.
TopBK was crystallized in presence of magnesium (crystal I) and calcium (crystal II) and the structures were solved at 2.1 Å and 1.95 Å resolution, respectively, with one monomer in the asymmetric unit in both cases.
Crystal thickness was estimated by measuring the intensity of the crystal (I) relative to the intensity of a hole in the carbon film (I0) from an image and using Beer's law: l n I I 0 = − ε c t where ε is the molar absorptivity, c is the molar concentration, and t is the crystal thickness.
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Even though the SEMs alone did not distinguish between Fe3C crystal, i-C, g-C, t-C, and graphite crystal, the carbon classification in Figure 1, enabled the degree of crystal to be ranked (high to low) as graphite crystal > t-C > g-C > i-C.
The semiconductor materials described here are single crystals; i.e., the atoms are arranged in a three-dimensional periodic fashion.
An interface is a meeting surface between two dissimilarly oriented perfect crystals or between two chemically different crystals, i.e., a crystallographic or chemical discontinuity.
In contrast, we have investigated the preparation and evaluated the properties of nano-sized organic crystals, i.e., organic nanocrystals [8 11].
The calcite crystals for both vein samples started to grow from the surface of the vein wall by using the crystals along it as seed crystals (i.e., syntaxial growth) as the extension fractures opened.
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