The local structure of CH3NH3I around the I- ion in Phase α' and δ was studied by iodine K-edge EXAFS. The crystal structure in Phase α' was redetermined by single crystal X-ray diffraction. The Debye-Waller factor σ(2) derived from EXAFS spectra shows an anomalous behavior around the order-disorder transition temperature from Phase δ to α'. The phase transition has been interpreted as the disordering process which involves not only the H atoms but also the C atoms in the cation.
Several methods have been tried to prepare clean surfaces of 4H–SiC(0001)Si and C, whose surface atomic, or electronic, structures have been studied by LEED (low energy electron diffraction) STM (scanning tunneling microscopy) and AES (Auger electron spectroscopy). Some sequential chemical treatments, for example, agitation in an organic solvent and dipping in HF solution, followed by the heating of a SiC wafer in UHV (ultrahigh vacuum, below 10-7 Pa) at 950°C, gave either a [Formula: see text] or 3×3 superstructure, observed by LEED (low energy electron diffraction), for the SiC(0001) Si or C surface, respectively. An elongated NH4F treatment followed by a heat treatment in UHV at ~950°C gave a rather flat region to be investigated by STM, where a [Formula: see text] superstructure for the SiC(0001) Si surface has been observed. In the case of metal (Ni) atom deposition on SiC(0001) [Formula: see text] and (0001)C(3×3) surfaces, AES and LEED analysis have clarified that deposited metal atoms form islands up to ~5 Å. However, Ni atoms dispersed uniformly at the very beginning of the deposition, which means that the Ni overlayer piles up in layer followed by island growth mode.
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