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Time-dependent density-functional theory beyond the adiabatic approximation: insights from a two-electron model system

Authors
  • Ullrich, C. A.
Type
Preprint
Publication Date
Oct 12, 2006
Submission Date
Oct 12, 2006
Identifiers
DOI: 10.1063/1.2406069
arXiv ID: cond-mat/0610341
Source
arXiv
License
Unknown
External links

Abstract

Most applications of time-dependent density-functional theory (TDDFT) use the adiabatic local-density approximation (ALDA) for the dynamical exchange-correlation potential Vxc(r,t). An exact (i.e., nonadiabatic) extension of the ground-state LDA into the dynamical regime leads to a Vxc(r,t) with a memory, which causes the electron dynamics to become dissipative. To illustrate and explain this nonadiabatic behavior, this paper studies the dynamics of two interacting electrons on a two-dimensional quantum strip of finite size, comparing TDDFT within and beyond the ALDA with numerical solutions of the two-electron time-dependent Schroedinger equation. It is shown explicitly how dissipation arises through multiple particle-hole excitations, and how the nonadiabatic extension of the ALDA fails for finite systems, but becomes correct in the thermodynamic limit.

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