A formalism for the vacancy formation energies in random alloys within the single-site meanfiled approximation, where vacancy-vacancy interaction is neglected, is outlined. It is shown that the alloy configurational entropy can substantially reduce the concentration of vacancies at high temperatures. The energetics of vacancies in random Cu0.5Ni0.5 alloy is considered as a numerical example illustrating the developed formalism. It is shown that the effective formation energy is increases with temperature, however, in this particular system it is still below the mean value of the vacancy formation energy which would correspond to the vacancy formation energy in a homogeneous model of a random alloy, such as given by the coherent potential approximation. 62.20.de, 75.30.Ds, 75.20.En Concentration of vacancies is one of the key parameters, which determines the kinetic of phase transformation and diffusion in solids. In spite of the structural simplicity of vacancies, their energetics has proven to be one of the least reliable physical properties determined in the first principles calculations (see, for instance, Ref.1-6). The situation becomes even more complicated at high temperatures, where anharmonic effects play an important role.
6In this paper, we will not however deal with those problems related to different approximations in first-principles calculations and subsequent modelling of the vacancy thermodynamics, but rather consider another important aspect, namely, the statistical description of vacancies in concentrated alloys at finite temperature connected with their first-principles modelling. This topic has recently been recently attracted attention of several groups doing first-principles simulations.7-11 In contrast to those investigations, in this work a simplified model for the energetics of vacancies will be presented for completely random alloys with the purpose to get a qualitative picture of the configurational effects.It is based on the single-site mean-field approximation, and thus all the effects related to the vacancyvacancy interactions will be ignored, while vacancy-alloycomponent interactions will be indirectly taken into consideration through the account of the local environment effects next to the vacancy. Although this is a simplified model, it anyway yields a quite accurate description of the phenomenon in real systems. To demonstrate the formalism, we will consider the energetics of vacancies in Cu 0.5 Ni 0.5 random alloy.The vacancy formation energy at 0 K in a binary random A c B 1−c alloy can be formally defined aswhere E 0 is the total energy per atom of a random A c(1−cv) B (1−c)(1−cv) Va cv alloy consisting c v concentration of vacancies (Va). This definition takes into consideration the fact that the derivative in (1) is not well defined since in real random alloys there exist substantial fluctuations of local compositions, which affect this derivative leading to a wide spectrum of the local vacancy formation energies connected to the specific space arrangements of the alloy...