Abstract:The basal (0001) surface plane of R-Al 2 O 3 has been extensively studied both by experimental techniques and applications of theory. Although this surface is not easily created upon cleavage, it grows in during aluminum oxidation and has been shown to be one of the lowest energy surfaces of alumina. Upon heating under vacuum, this (0001) surface of R-Al 2 O 3 undergoes a series of reconstructions. The final structure obtained at ∼1700 K is an air-stable termination known as the ( 31 × 31)R ( 9°reconstruction.… Show more
“…The periodic repetitions of the supercell geometry along the z-axis are separated by~12 Å of vacuum to eliminate interactions between periodic cells, and the Al 2 O 3 slab is cut to have an Al truncated surface since it was shown to be the most stable surface termination. [38,44,45] The calculated bulk NiAl lattice constant of 2.891 Å , which is in good agreement with the experimental value of 2.887 Å , yields a lattice misfit of 0.5 pct between NiAl and Al 2 O 3 surfaces, demonstrating a reasonable coherent interface model.…”
Section: Theoretical Methodssupporting
confidence: 80%
“…The recent ab initio DFT calculations, [44,45] however, demonstrated that the Al-terminated Al 2 O 3 (0001) surface is more stable than that with O as a termination layer. Therefore, it is essential to investigate the NiAl/Al 2 O 3 interface with Al-terminated layer, at which the highest work of separation can be achieved through examining various translations of NiAl (110) relative to the Al 2 O 3 .…”
“…The periodic repetitions of the supercell geometry along the z-axis are separated by~12 Å of vacuum to eliminate interactions between periodic cells, and the Al 2 O 3 slab is cut to have an Al truncated surface since it was shown to be the most stable surface termination. [38,44,45] The calculated bulk NiAl lattice constant of 2.891 Å , which is in good agreement with the experimental value of 2.887 Å , yields a lattice misfit of 0.5 pct between NiAl and Al 2 O 3 surfaces, demonstrating a reasonable coherent interface model.…”
Section: Theoretical Methodssupporting
confidence: 80%
“…The recent ab initio DFT calculations, [44,45] however, demonstrated that the Al-terminated Al 2 O 3 (0001) surface is more stable than that with O as a termination layer. Therefore, it is essential to investigate the NiAl/Al 2 O 3 interface with Al-terminated layer, at which the highest work of separation can be achieved through examining various translations of NiAl (110) relative to the Al 2 O 3 .…”
“…1a [25,26]; the Al termination yields non-polar surfaces. Experimentally, it is observed that ð0 0 0 1Þ surfaces prepared at temperatures below $1500 K show a stable ð1  1Þ surface, corresponding to the nonpolar Al-termination; this surface is also characterized by large inward relaxation of the Al atoms [27][28][29][30][31][32]. Annealing to higher temperatures produces a rotated ð ffiffiffiffiffiffi 31 p  ffiffiffiffiffiffi 31 p Þ surface reconstruction, associated with the Al-rich (Al-Al) surface [30,[33][34][35][36][37][38][39][40][41].…”
a b s t r a c tThe growth and characterization of epitaxial Co 3 O 4 ð1 1 1Þ films grown by oxygen plasma-assisted molecular beam epitaxy on single crystal a-Al 2 O 3 ð0 0 0 1Þ is reported. The Co 3 O 4 ð1 1 1Þ grows single crystalline with the epitaxial relation Co 3 O 4 ð1 1 1Þ½1 21ka-Al 2 O 3 ð0 0 0 1Þ½1010, as determined from in situ electron diffraction. Film stoichiometry is confirmed by X-ray photoelectron spectroscopy, while ex situ X-ray diffraction measurements show that the Co 3 O 4 films are fully relaxed. Post-growth annealing induces significant modifications in the film morphology, including a sharper Co 3 O 4 =a-Al 2 O 3 interface and improved surface crystallinity, as shown by X-ray reflectometry, atomic force microscopy and electron diffraction measurements. Despite being polar, the surface of both as-grown and annealed Co 3 O 4 ð1 1 1Þ films are ð1 Â 1Þ, which can be explained in terms of a surface inversion in the spinel structure.
“…Fig 2͑b͔͒. The metallic-like character of the Al-rich surface of corundum has been reported previously. 33,34 For the reconstructed ͱ31ϫͱ31 surface we would expect the metallization to strongly influence the surface reactivity. For the oxygen terminated surface, on the other hand, the 2p shell could be unfilled.…”
We report density functional theory calculations of the interaction of Cu and Pd with the ͑0001͒ surface of ␣-Al 2 O 3 . The interaction of those metals with the oxide surface varies from covalent-like for the aluminum rich surface to ionic-like for the oxygen terminated surface. Stoichiometric hydroxylation of the surface does not increase the metal-oxide interaction significantly. We suggest that defects created upon hydroxylation are the main mechanism to explain the observed metal wetting of the oxide.
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