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Hiraga et al. ( 2002) reported the presence of nanoscale melt films using high-resolution electron microscopy and energy dispersive X-ray profiling in scanning transmission electron microscopy.
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The LH deposition profiles used in the JETTO code are consistent with the measured hard X-ray profiles.
The phases were determined by X-ray profile as well as microstructure observation.
Two candidates emerged that had the expected red color, seen by Hubble and Spitzer, as well as the X-ray profile predicted from Chandra.
In the years 1959 1991, this scheme of examinations included X-ray profiles of the singers' vocal tracts.
In addition to the "self-seeding" for LCLS, he guided research efforts for two-color X-ray generation and femtosecond X-ray profile measurements using an X-band radio-frequency deflector.
The radial profiles of the LH-driven current density are expected to have the same shape as the hard X-ray profile, as routinely assumed in tokamak experiment modelling.
X-ray profiles, recorded for all samples, both unpyrolysed and pyrolysed, support the interpretation of the conductivity results.
The origin of the asymmetry of observed X-ray profiles was discussed in detail and the procedure to derive a precise (sub-eV) X-ray transition energy for such asymmetric profiles was proposed.
Both of the deposits showed amorphous X-ray profile, however, as it was expected, the presence of small (about 10 nm in size) nanocrystallites was observed in both kinds of plating under transmission electron microscope (TEM).
Single crystal structure investigations as well as powder X-ray profile refinements employing the Rietveld method and pair distribution function technique revealed, that with increasing δ the distortions lessen and finally disappear, as was predicted based on the Kleinke–Harbrecht structure map.
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