% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Botti:56493,
      author       = {Botti, S. and Schindlmayr, A. and Del Sole, R. and Reining,
                      L.},
      title        = {{T}ime-dependent density-functional theory for extended
                      systems},
      journal      = {Reports on progress in physics},
      volume       = {70},
      issn         = {0034-4885},
      address      = {Bristol},
      publisher    = {IOP Publ.},
      reportid     = {PreJuSER-56493},
      pages        = {357},
      year         = {2007},
      note         = {Record converted from VDB: 12.11.2012},
      abstract     = {For the calculation of neutral excitations, time-dependent
                      density functional theory (TDDFT) is an exact reformulation
                      of the many-body time-dependent Schrodinger equation, based
                      on knowledge of the density instead of the many-body
                      wavefunction. The density can be determined in an efficient
                      scheme by solving one-particle non-interacting Schrodinger
                      equations -the Kohn-Sham equations. The complication of the
                      problem is hidden in the unknown -time-dependent exchange
                      and correlation potential that appears in the Kohn-Sham
                      equations and for which it is essential to find good
                      approximations. Many approximations have been suggested and
                      tested for finite systems, where even the very simple
                      adiabatic local-density approximation (ALDA) has often
                      proved to be successful. In the case of solids, ALDA fails
                      to reproduce optical absorption spectra, which are instead
                      well described by solving the Bethe Salpeter equation of
                      many-body perturbation theory (MBPT). On the other hand,
                      ALDA can lead to excellent results for loss functions (at
                      vanishing and finite momentum transfer). In view of this and
                      thanks to recent successful developments of improved
                      linear-response kernels derived from MBPT, TDDFT is today
                      considered a promising alternative to MBPT for the
                      calculation of electronic spectra, even for solids. After
                      reviewing the fundamentals of TDDFT within linear response,
                      we discuss different approaches and a variety of
                      applications to extended systems.},
      keywords     = {J (WoSType)},
      cin          = {IFF-1},
      ddc          = {530},
      cid          = {I:(DE-Juel1)VDB781},
      pnm          = {Kondensierte Materie},
      pid          = {G:(DE-Juel1)FUEK414},
      shelfmark    = {Physics, Multidisciplinary},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000244875800003},
      doi          = {10.1088/0034-4885/70/3/R02},
      url          = {https://juser.fz-juelich.de/record/56493},
}