The intermetallic compound Ni3Al, one of the well-known high-temperature L1
(2) (gamma (t)) superalloys is an excellent model system for the studies of
long-range order (LRO) relaxation run by atomic jumps to nn vacancies in a
homogeneous superstructure. Experimental studies of "order-order" kinetics
in Ni3Al carried out by means of resistometry revealed that the relaxation
isotherms of the Bragg-Williams LRO parameter eta were composed of two sin
gle exponentials substantially differing in relaxation times. Later investi
gations suggested that this effect may show up in systems with different ty
pes of superlattices.
The origin of the phenomenon was studied by means of Monte Carlo (MC) simul
ations. Original studies were performed with a model system described by an
Ising Hamiltonian with phenomenological pair-interaction energy parameters
. Atomic jumps were simulated using the Glauber algorithm, in which their p
robabilities depend on differences of system energies before and after the
jumps. It was concluded that the fast component of the eta (t) relaxation c
onsists of the efficient elimination/creation of nn antisite pairs resultin
g from highly correlated ordering/disordering jumps of Al- and Ni-atoms. Th
e process permanently competes with Al-antisite migration within Ni-sublatt
ice, which is a mechanism of a slower elimination/creation of anti sites sh
owing up as the slow eta -relaxation component.
An important drawback of the kinetic model based on the Glauber algorithm i
s the negligence of saddle-point energies, which in any case must be overco
me by real atoms when jumping from lattice sites to nn vacancies. In the pr
esent paper it is proposed to go beyond the Ising model and to approach the
problem by directly implementing the "embedded-atom-method" (EAM) formalis
m for lattice energy with the "activated-state-rate approximation" and MC s
imulation.
Assuming that atoms jump only to mi vacancies, "order-order" kinetics (and
any other process controlled by atomic migration) is simulated by calculati
ng on line changes of the system energy DeltaE caused by each atomic jump.
It is important that, using EAM, it is possible to evaluate DeltaE being th
e difference not only between the system energies before and after the jump
, but also between the energy of a system with an atom on the saddle-point
and its energy before the jump. Consequently, EAM may be implemented with a
ny algorithm applied in MC simulation of atomic migration and postulating p
articular formula for the jump probability.
A systematic comparative study of "order-order" kinetics in Ni3Al is carrie
d out by means of MC simulations involving Glauber and "residence-time" alg
orithms implemented with EAM formalism. The results yield additional criter
ia for the evaluation of EAM potentials for Ni3Al.