2 research outputs found
Effect of Subsurface Oxygen on Selective Catalytic Reduction of NO by H<sub>2</sub> on Pt(100): A First-Principles Study
The
mechanisms of NO reduction by H<sub>2</sub> on the Pt(100)
surface and the surface modified with subsurface oxygen atoms (Md-Pt(100))
are studied by first-principles calculations. Similar catalytic activity
toward NO dissociation is found on both surfaces with barriers of
0.86 and 0.96 eV, respectively. The pathway of N + N → N<sub>2</sub> rather than NO + N → N<sub>2</sub> + O is the N<sub>2</sub> formation pathway on the Pt(100) surface, while these two
pathways are competitive on the Md-Pt(100) surface. The NH<sub>3</sub> formation is almost negligible, and reductant hydrogen can effectively
remove the surface oxygen on both surfaces. The microkinetic analysis
further confirms that, compared to the high selectivity toward N<sub>2</sub>O (almost 100% at 300–500 K) on the clean surface,
higher N<sub>2</sub> low-temperature selectivity (larger than 90%)
is achieved on the Md-Pt(100) surface under lower pressure. The present
study shows that subsurface oxygen has an enhanced effect for improving
the N<sub>2</sub> selectivity of NO reduction on Pt catalysts
Honeycomb Boron Allotropes with Dirac Cones: A True Analogue to Graphene
We
propose a series of planar boron allotropes with honeycomb topology
and demonstrate that their band structures exhibit Dirac cones at
the K point, the same as graphene. In particular, the Dirac point
of one honeycomb boron sheet locates precisely on the Fermi level,
rendering it as a topologically equivalent material to graphene. Its
Fermi velocity (<i>v</i><sub>f</sub>) is 6.05 × 10<sup>5</sup> m/s, close to that of graphene. Although the freestanding
honeycomb B allotropes are higher in energy than α-sheet, our
calculations show that a metal substrate can greatly stabilize these
new allotropes. They are actually more stable than α-sheet sheet
on the Ag(111) surface. Furthermore, we find that the honeycomb borons
form low-energy nanoribbons that may open gaps or exhibit strong ferromagnetism
at the two edges in contrast to the antiferromagnetic coupling of
the graphene nanoribbon edges