Is time-dependent density functional theory formally exact?
J. Schirmer, A. Dreuw

TL;DR
This paper critically reexamines the formal exactness of time-dependent density functional theory (TDDFT), revealing foundational flaws in its theoretical basis and analyzing simplified models to understand its limitations.
Contribution
It demonstrates the invalidity of the original Runge-Gross theorems due to phase issues and introduces a simplified Kohn-Sham model to analyze TDDFT's formal properties.
Findings
Runge-Gross theorems are invalid due to phase factors.
Simplified single-particle Kohn-Sham model clarifies TDDFT limitations.
Local operators do not lose information in linear response analysis.
Abstract
The general expectation that, in principle, time-dependent density functional theory (TDDFT) be an exact formulation of the time-evolution of an interacting N-electron system is critically reexamined. It is demonstrated that the previous TDDFT foundation, resting on three theorems by Runge and Gross (RG) [Phys.Rev.Lett.52, 997(1984)], is invalid because undefined phase factors corrupt the RG action integral functionals. Our finding confirms much of a previous analysis by van Leeuwen [Int. J. Mod. Phys. B15, 1969(2001)]. To analyze the RG theorems and other aspects of TDDFT, an utmost simplification of the KS theory is introduced, in which the density is obtained from a single KS equation for one spatial (spin-less) particle. This radical KS formulation allows us to analyze also the concept of KS-type equations derived without a variational principle. We argue that such an approach can…
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