1994
DOI: 10.1103/physrevlett.73.2599
|View full text |Cite
|
Sign up to set email alerts
|

Ab InitioMolecular Dynamics with Excited Electrons

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
180
0

Year Published

1997
1997
2020
2020

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 239 publications
(180 citation statements)
references
References 21 publications
0
180
0
Order By: Relevance
“…A detailed analysis of the electronic structure for selected geometries ͑snapshots͒ has been carried out with the Lanczos diagonalization scheme and the free energy functional of Alavi et al ͑T = 1000 K͒. 26 Memory of the crystalline starting structure was erased by starting the simulations at 3000 K ͑liquid͒, followed by gradual cooling over 42 ps to the melting point ͑900 K͒. The first data collection was performed for 21 ps at 900 K, followed by cooling to 300 K over 139 ps.…”
Section: A Density Functional Calculationsmentioning
confidence: 99%
“…A detailed analysis of the electronic structure for selected geometries ͑snapshots͒ has been carried out with the Lanczos diagonalization scheme and the free energy functional of Alavi et al ͑T = 1000 K͒. 26 Memory of the crystalline starting structure was erased by starting the simulations at 3000 K ͑liquid͒, followed by gradual cooling over 42 ps to the melting point ͑900 K͒. The first data collection was performed for 21 ps at 900 K, followed by cooling to 300 K over 139 ps.…”
Section: A Density Functional Calculationsmentioning
confidence: 99%
“…The most elegant solution would be to treat electrons in the grand canonical ensemble, that is, to allow the number of electrons to change during the electronic structure self-consistency loop, which is equivalent to connecting the system to a fictitious potentiostat. 5,6 Unfortunately, convergence of the grand canonical Kohn-Sham equations is significantly slower than with a fixed number of electrons, limiting the method to small system sizes. Other suggested methods rely on extrapolating calculated energies from canonical, constant charge DFT simulations to constant electrode potential.…”
Section: Introductionmentioning
confidence: 99%
“…Several methods [5][6][7][8][9][10][11][12][13] have been proposed for correcting quantum chemical calculations to constant electrode potential. The most elegant solution would be to treat electrons in the grand canonical ensemble, that is, to allow the number of electrons to change during the electronic structure self-consistency loop, which is equivalent to connecting the system to a fictitious potentiostat.…”
Section: Introductionmentioning
confidence: 99%
“…Contemporary computations on WDM [5][6][7][8][9][10][11][12][13][14][15][16][17][18] are dominated by use of the Kohn-Sham (KS) realization of thermal density functional theory (DFT) [19][20][21][22][23][24][25] to generate a potential surface for ionic motion (treated classically). The majority of such calculations use approximate ground-state exchange-correlation (XC) functionals, E xc , with the temperature dependence of the XC free energy picked up implicitly from the T-dependence of the density n(r, T).…”
Section: Introductionmentioning
confidence: 99%