Abstract
Time-dependent density functional theory (TDDFT) in its current adiabatic implementations exhibits three remarkable failures: (a) completely wrong behavior of the excited state surface along a bond-breaking coordinate; (b) lack of doubly excited configurations; (c) much too low charge transfer excitation energies. These TDDFT failure cases are all strikingly exhibited by prototype two-electron systems such as dissociating H2 and HeH+. We find for these systems with time-dependent density matrix functional theory that: (a) Within previously formulated simple adiabatic approximations, the bonding-to- antibonding excited state surface as well as charge transfer excitations are described without problems, but not the double excitations; (b) An adiabatic approximation is formulated in which also the double excitations are fully accounted for. © 2008 The American Physical Society.
| Original language | English |
|---|---|
| Pages (from-to) | 033004 |
| Journal | Physical Review Letters |
| Volume | 101 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 2008 |
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SDG 7 Affordable and Clean Energy
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