Abstract

A density-functional formalism comparable to the Hohenberg-Kohn-Sham theory of the ground state is developed for arbitrary time-dependent systems. It is proven that the single-particle potential $v(\stackrel{\ensuremath{\rightarrow}}{\mathrm{r}}t)$ leading to a given $v$-representable density $n(\stackrel{\ensuremath{\rightarrow}}{\mathrm{r}}t)$ is uniquely determined so that the corresponding map $v\ensuremath{\rightarrow}n$ is invertible. On the basis of this theorem, three schemes are derived to calculate the density: a set of hydrodynamical equations, a stationary action principle, and an effective single-particle Schr\"odinger equation.

Keywords

Invertible matrixFormalism (music)PhysicsMathematical physicsDensity functional theoryGround stateQuantum mechanics

Affiliated Institutions

Related Publications

Electron densities in search of Hamiltonians

By utilizing the knowledge that a Hamiltonian is a unique functional of its ground-state density, the following fundamental connections between densities and Hamiltonians are re...

1982 Physical review. A, General physics 670 citations

Crystalline Order in Two Dimensions

If $N$ classical particles in two dimensions interacting through a pair potential $\ensuremath{\Phi}(\stackrel{\ensuremath{\rightarrow}}{\mathrm{r}})$ are in equilibrium in a pa...

1968 Physical Review 1286 citations

Publication Info

Year
1984
Type
article
Volume
52
Issue
12
Pages
997-1000
Citations
8420
Access
Closed

External Links

Social Impact

Social media, news, blog, policy document mentions

Citation Metrics

8420
OpenAlex

Cite This

Erich Runge, E. K. U. Gross (1984). Density-Functional Theory for Time-Dependent Systems. Physical Review Letters , 52 (12) , 997-1000. https://doi.org/10.1103/physrevlett.52.997

Identifiers

DOI
10.1103/physrevlett.52.997