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inception413

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[求助] 有关吸附氧化的一篇英文文献 帮我分析一下

大概意思是将金刚石薄膜模型搭建一个6层的表面slab模型(这一步我还懂)但是接下来说让这个模型暴露在温度为298k左右,能量为5ev的氧原子中,氧原子的概率是随机的,这些都是如何做到的?
Theoretical investigations of 5 eV hyperthermal AO collisions
with diamond (100) and (111) surfaces were conducted. Direct
dynamics calculations were performed with forces and energies
derived from self-consistent charge density-functional-based tightbinding
(SCC-DFTB) calculations.33,34 The Γ point was used for
Brillouin zone sampling. The (100) and (111) surface models each
contained 72 carbon atoms, forming six atomic layers.
Three-dimensional periodic boundary conditions were used.
The two unit-cell vectors within the basal planes were optimized
so that the pristine diamond was under zero strain. The lattice
vector in the direction normal to the surfaces was set to 30 Å,
a value large enough to prevent unrealistic interactions between
neighboring unit cells in this direction. These unit-cell vectors
were fixed at these values for all of the simulations. In the (100)
case, the back sides (the surfaces opposite the sides with which
the incoming AO collides) were (2 × 1) reconstructed, with
the remaining dangling bonds terminated by using hydrogen
atoms. In the (111) case, they were also hydrogen-terminated.

Intramolecular trajectories were run at 298 K for the atoms in
the slabs, and these trajectories were sampled to determine initial
velocities and positions for all but the incoming AO.
Slabs were exposed to oxygen atoms traveling with 5 eV of
translational energy. Normal incidence was considered, with
impact locations chosen randomly. Trajectories were propagated
for 1 ps by using a 10.0 au (0.24 fs) time step on the lowest
triplet potential-energy surface. Initial AO-to-diamond-surface
separations of ∼10 au (5.3 Å were used.
Different oxygen-, hydrogen-, and deuterium-containing
surface coverages were systematically investigated. A subset
of these simulations is described below.
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  • 附件 1 : oxidationandetchingofcvddiamondbythermalandhyperthermalatomicoxygen.pdf
  • 2012-11-16 20:47:07, 5.72 M

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