A quantum mechanical method using electron density to compute properties of many-body systems.Density functional theory (DFT) is a quantum mechanical modeling method used to investigate the electronic structure of many-body systems, such as molecules, solids, and liquids. Instead of tracking every individual electron, it uses the electron density as the central variable, making calculations feasible for systems with thousands of atoms. DFT has become the standard tool in materials science, chemistry, and condensed matter physics for predicting properties like binding energies, band gaps, and reaction pathways.
The foundations were laid by Pierre Hohenberg and Walter Kohn in 1964, with the practical Kohn-Sham formulation introduced the following year. Walter Kohn received the Nobel Prize in Chemistry in 1998 for this work.
The theory rests on the Hohenberg-Kohn theorems, which state that the ground-state energy of a system is a unique functional of the electron density. In practice, the Kohn-Sham equations map the interacting electron problem onto a set of non-interacting particles moving in an effective potential. This potential includes the external potential, the classical Coulomb repulsion, and an exchange-correlation term that approximates quantum many-body effects. The equations are solved iteratively until the density converges to a self-consistent solution.
DFT is used to design new battery materials, predict the properties of catalysts, simulate drug interactions with proteins, and study the electronic structure of novel superconductors.
DFT calculations are so widespread that they account for a significant fraction of all supercomputer time used in materials science worldwide.











