Graduate → Theoretical and Computational Chemistry → Quantum chemical methods ↓
Density functional theory
Density functional theory (DFT) is a powerful computational quantum mechanical modeling method used in physics, chemistry, and materials science to investigate the electronic structure of many-body systems, especially atoms, molecules, and condensed phases. Its importance lies in its ability to explain all kinds of chemical properties using electron densities rather than wave functions.
Basic concepts of DFT
The basic idea behind DFT is contained in its name itself: the density functional approach. In DFT, the properties of a many-electron system are uniquely determined by its electron density, which is a much simpler quantity than the many-body wave function. The electron density, ρ(r)
, describes the probability of finding an electron at a point, r
, in space.
This equation defines the electron density ρ(r)
in terms of the molecular orbitals ψ i (r)
.
Historical development
DFT was developed from the Thomas–Fermi model, which was based on a semiclassical approximation of electron gases. A leap forward came in 1964 with two important theorems by Hohenberg and Kohn, which laid the mathematical foundation for modern DFT.
Hohenberg–Cohn theorem
1. Existence theorem: It states that the ground state properties of a many-electron system are uniquely determined by the electron density ρ(r)
.
2. The variational principle: for any density ρ(r)
that can be physically realized, the energy functional, E[ρ]
, attains its minimum value at the true ground state density. In other words, if you can guess the true density, you can calculate the ground state energy.
Where, E[ρ]
is the energy as a functional of the density ρ(r)
, T[ρ]
denotes the kinetic energy part, V[ρ]
denotes the electron-electron interaction, V ne [ρ]
is the electron-nuclear interaction, and E xc [ρ]
is the exchange-correlation functional.
Kohn–Sham approach
Practical implementations of DFT are primarily based on the Kohn–Sham (KS) formalism, introduced in 1965. Kohn and Sham provided a way to treat interacting systems as non-interacting systems of particles with the same density.
Kohn–Sham DFT reduces the problem of interacting electrons to solving a set of self-consistent field equations for non-interacting electrons:
in which V eff (r)
is the effective potential, ε i
are the orbital energies, and ψ i (r)
are the Kohn–Sham orbitals. The electron density is expressed in terms of these orbitals.
Exchange-correlation functional
An important element of the DFT is the exchange-correlation energy, E xc [ρ]
. This is where the tricky part of the DFT lies: finding an exact expression for the exchange-correlation functional. All terms except E xc [ρ]
can be derived directly.
Several approximations to the exchange–correlation functional exist, including:
- Local density approximation (LDA): This assumes that the exchange-correlation at each point in space depends only on the electron density at that point.
- Generalized gradient approximation (GGA): This includes not only the density but also its gradient, providing greater flexibility and accuracy.
- Hybrid functionals: combine a part of the exact exchange from Hartree–Fock theory, aiming to further improve accuracy.
The choice of functional significantly affects the reliability of DFT calculations, and choosing the right functional often depends on the trade-off between accuracy and computational cost.
Applications of DFT
DFT is used extensively in various fields of chemistry and materials science due to its computational efficiency and reliability. It helps in predicting molecular structures, vibrational spectra, thermochemical properties, reaction mechanisms, and much more.
- Atoms and Molecules: DFT is widely used to calculate electron distribution and energy states in atoms and molecules. It plays an important role in quantum chemistry to understand chemical bonding and reactivity.
- Solid State Physics: In solids, DFT helps calculate band structures, lattice dynamics, and mechanical properties, which proves essential in materials science for new materials design.
- Catalysis: DFT enables the study of catalytic surfaces and reaction mechanisms at the atomic level, helping in the design of more efficient catalysts.
Limitations of DFT
Despite its wide application and popularity, DFT has its limitations, mainly due to the approximations in the exchange-correlation functional.
- Exchange-correlation: choosing inappropriate functionals can lead to erroneous results, especially for systems with significant electron correlation.
- Van der Waals interactions: DFT usually underestimates these weak, long-range interactions unless specifically corrected for.
- Open systems: Modeling open systems with non-conserved particle number can be challenging within the DFT framework.
Researchers are continually developing new functionalities and approaches to overcome these limitations and further extend the applicability of DFT.
Main advantages of DFT
The main strength of the DFT lies in its computational efficiency and accuracy for a wide range of systems compared to traditional wave function methods.
- Efficiency: The computational cost of DFT is typically lower than that of wave function-based methods such as Hartree–Fock or post-Hartree–Fock methods, making it possible to study larger systems.
- Scalability: DFT scales more favorably with the size of the system, making it suitable for systems containing hundreds of atoms.
- Versatility: It is applicable to a wide variety of systems - from isolated atoms to large molecular complexes and solids.
Conclusion
Density functional theory is a cornerstone of computational chemistry and physics. With its balance of computational efficiency and accuracy, DFT has been widely adopted to tackle complex electronic structure problems in chemistry and physics. Despite inherent challenges and limitations, advances in the methodology continue to advance its capabilities, strengthening its role in future discoveries and technological innovations.