Development of Density Functional Theory

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Ab initio (aka First Principle) calculations are based on the basic laws of physics without any empirical parameters or fitting models. Simulations originating from the First Principles have played a more important role in studies in condensed matter physics and chemistry.
A solid system comprises electrons and nuclei, and interactions among them determine the total energy of the system. Also, the outer shell electrons have great influences on the electronic and optic properties of solids. As there are many particles inside a real solid system, “single-electron” approximation is essential to make simulation possible.
The Density Functional Theory is a promising approach to compute the electronic structure of matter. It determines the properties of a system at the ground state by using functionals (i.e. functions of another function) of electron density.
The construction of the theory starts with elementary quantum mechanics and the theory is later generalized to fit different situations.

A Schrodinger equation describes how the quantum state of a system varies with time. However, it would be really complex for solid system consisting of many nuclei and electrons. It would be much better if a time-independent, non-relativistic Schrodinger equation can be acquired.
H ̂Ψ_i (x ⃑_1,x ⃑_2,…,x ⃑_N,R ⃑_1,R ⃑_2,…,R ⃑_M )=E_i Ψ_i (x ⃑_1,x ⃑_2,…,x ⃑_N,R ⃑_1,R ⃑_2,…,R ⃑_M )

Ĥ is the Hamiltonian for a system consisting M nuclei and N electrons, and it governs the dynamics of the quantum system.
H ̂=-1/2 ∑_(i=1)^N▒∇_i^2 -1/2 ∑_(A=1)^M▒〖1/M_A ∇_i^2 〗-∑_(i=1)^N▒∑_(A=1)^M▒Z_A/r_iA +∑_(i=1)^N▒∑_(j>1)^N▒1/r_ij +∑_(A=1)^M▒∑_(B>A)^M▒(Z_A Z_B)/R_AB where the first two terms are describing the kinetic energy of electrons and nuclei, th...

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...ctron gas. This is a system in which electrons move on a positive background charge distribution such that the total ensemble is neutral. The central idea of LDA is the assumption that we can write EXC in the following form [eq43]
Here, εXC(ρ(⃗r)) is the exchange-correlation energy per particle of an uniform electron gas of density ρ(⃗r). This energy per particle is weighted with the probability ρ(⃗r) that there is an electron at this position. The quantity εXC(ρ(⃗r)) can be further split into exchange and correlation contributions, εXC(ρ(⃗r)) = εX(ρ(⃗r)) + εC(ρ(⃗r)). (44)
The exchange part, εX , which represents the exchange energy of an electron in a uniform electron gas of a particular density, was originally derived by Bloch and Dirac in the late 1920’s
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Works Cited

J. C. Cuevas, “Introduction to Density Functional Theory,” Universitat Karlsruhe(Germany).

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