GENERAL POTENTIAL-ENERGY FUNCTION FOR H NI AND DYNAMICS CALCULATIONS OF SURFACE-DIFFUSION, BULK DIFFUSION, SUBSURFACE-TO-SURFACE TRANSPORT,AND ABSORPTION/
Se. Wonchoba et Dg. Truhlar, GENERAL POTENTIAL-ENERGY FUNCTION FOR H NI AND DYNAMICS CALCULATIONS OF SURFACE-DIFFUSION, BULK DIFFUSION, SUBSURFACE-TO-SURFACE TRANSPORT,AND ABSORPTION/, Physical review. B, Condensed matter, 53(16), 1996, pp. 11222-11241
We present a potential-energy function for H interacting with bulk met
allic Ni. The potential is parametrized to be accurate both for H adso
rbed on Ni surfaces and for H absorbed at interior sites. The function
introduces a nonlocal density dependence into the embedded-atom metho
d formalism. We show that the function provides dramatic improvement o
ver the best previous embedded-atom potential function for this system
, and that it gives good agreement with all available structural and e
nergetic data characterizing stationary points on the few-index surfac
e planes [(100), (111), and (110)] and in the interior. It also yields
good agreement with experiment for most diffusion coefficients and ac
tivation energies for surface and interior diffusion. We examine the d
ynamics of three diffusion processes: H diffusing on the (100) and (11
1) crystal faces, and H migrating in the interior, for the latter of w
hich we analyze the reaction path and predict coefficients for H diffu
sion between adjacent interior octahedral vacancies. We also examine t
wo other processes: H hopping from the threefold (111) surface binding
site to an octahedral vacancy immediately beneath the (111) surface p
lane to (absorption), and the reverse process (deabsorption). We also
calculate the binding energy and frequencies for H adsorbed on the pse
udothreefold site of the Ni(110) surface, and we find them to be in go
od agreement with experiment and a considerable improvement over previ
ous versions of the potential function. Our potential-energy function
should be useful for simulations of a variety of processes that are di
fficult to study experimentally, such as surface diffusion in the pres
ence of steps and kinks, site-to-site movement of H immediately beneat
h a surface plane of Ni, or bulk transport across a grain boundary.