Progress in Time-Dependent Density-Functional Theory
M. E. Casida, M. Huix-Rotllant

TL;DR
This paper reviews the development, applications, and limitations of time-dependent density-functional theory (TD-DFT), emphasizing the challenges in describing excited states and recent advances in overcoming these issues.
Contribution
It provides an updated overview of TD-DFT, discussing its strengths, weaknesses, and recent solutions for accurately modeling excited states beyond the adiabatic approximation.
Findings
TD-DFT is widely used for molecular spectra calculations.
Limitations exist in describing doubly-excited states.
Recent methods aim to go beyond the adiabatic approximation.
Abstract
The classic density-functional theory (DFT) formalism introduced by Hohenberg, Kohn, and Sham in the mid-1960s, is based upon the idea that the complicated N-electron wavefunction can be replaced with the mathematically simpler 1-electron charge density in electronic struc- ture calculations of the ground stationary state. As such, ordinary DFT is neither able to treat time-dependent (TD) problems nor describe excited electronic states. In 1984, Runge and Gross proved a theorem making TD-DFT formally exact. Information about electronic excited states may be obtained from this theory through the linear response (LR) theory formalism. Begin- ning in the mid-1990s, LR-TD-DFT became increasingly popular for calculating absorption and other spectra of medium- and large-sized molecules. Its ease of use and relatively good accuracy has now brought LR-TD-DFT to the forefront for this type of…
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