-
1
-
-
10644250257
-
-
10.1103/PhysRev.136.B864
-
P. Hohenberg and W. Kohn, Phys. Rev. 136, B864 (1964). 10.1103/PhysRev.136.B864
-
(1964)
Phys. Rev.
, vol.136
, pp. 864
-
-
Hohenberg, P.1
Kohn, W.2
-
4
-
-
0042113153
-
-
10.1103/PhysRev.140.A1133
-
W. Kohn and L. J. Sham, Phys. Rev. 140, A1133 (1965). 10.1103/PhysRev.140.A1133
-
(1965)
Phys. Rev.
, vol.140
, pp. 1133
-
-
Kohn, W.1
Sham, L.J.2
-
5
-
-
5444237332
-
-
10.1088/0022-3719/5/13/012
-
U. von Barth and L. Hedin, J. Phys. C 5, 1629 (1972). 10.1088/0022-3719/5/13/012
-
(1972)
J. Phys. C
, vol.5
, pp. 1629
-
-
Von Barth, U.1
Hedin, L.2
-
6
-
-
33744596259
-
-
10.1103/PhysRevB.28.1809;
-
D. C. Langreth and M. J. Mehl, Phys. Rev. B 28, 1809 (1983) 10.1103/PhysRevB.28.1809
-
(1983)
Phys. Rev. B
, vol.28
, pp. 1809
-
-
Langreth, D.C.1
Mehl, M.J.2
-
7
-
-
4243553426
-
-
10.1103/PhysRevA.38.3098;
-
A. D. Becke, Phys. Rev. A 38, 3098 (1988) 10.1103/PhysRevA.38.3098
-
(1988)
Phys. Rev. A
, vol.38
, pp. 3098
-
-
Becke, A.D.1
-
8
-
-
4243943295
-
-
10.1103/PhysRevLett.77.3865
-
J. P. Perdew, K. Burke, and M. Ernzerhof, Phys. Rev. Lett. 77, 3865 (1996), and references therein. 10.1103/PhysRevLett.77.3865
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 3865
-
-
Perdew, J.P.1
Burke, K.2
Ernzerhof, M.3
-
12
-
-
12044251032
-
-
10.1103/RevModPhys.66.763;
-
E. Dagotto, Rev. Mod. Phys. 66, 763 (1994) 10.1103/RevModPhys.66.763
-
(1994)
Rev. Mod. Phys.
, vol.66
, pp. 763
-
-
Dagotto, E.1
-
13
-
-
0030528685
-
-
10.1103/RevModPhys.68.13;
-
A. Georges, G. Kotliar, W. Krauth, and M. J. Rozenberg, Rev. Mod. Phys. 68, 13 (1996) 10.1103/RevModPhys.68.13
-
(1996)
Rev. Mod. Phys.
, vol.68
, pp. 13
-
-
Georges, A.1
Kotliar, G.2
Krauth, W.3
Rozenberg, M.J.4
-
15
-
-
2842617037
-
-
10.1103/PhysRev.124.41
-
P. W. Anderson, Phys. Rev. 124, 41 (1961). 10.1103/PhysRev.124.41
-
(1961)
Phys. Rev.
, vol.124
, pp. 41
-
-
Anderson, P.W.1
-
17
-
-
0000541030
-
-
10.1143/PTP.30.275;
-
J. Kanamori, Prog. Theor. Phys. 30, 275 (1963) 10.1143/PTP.30.275
-
(1963)
Prog. Theor. Phys.
, vol.30
, pp. 275
-
-
Kanamori, J.1
-
18
-
-
33744619385
-
-
10.1103/PhysRevLett.10.159
-
M. C. Gutzwiller, Phys. Rev. Lett. 10, 159 (1963). 10.1103/PhysRevLett. 10.159
-
(1963)
Phys. Rev. Lett.
, vol.10
, pp. 159
-
-
Gutzwiller, M.C.1
-
21
-
-
34748873709
-
-
10.1039/tf9534901375
-
J. A. Pople, Trans. Faraday Soc. 49, 1375 (1953). 10.1039/tf9534901375
-
(1953)
Trans. Faraday Soc.
, vol.49
, pp. 1375
-
-
Pople, J.A.1
-
23
-
-
33751231898
-
-
10.1103/PhysRevB.37.9919;
-
A. Svane and O. Gunnarsson, Phys. Rev. B 37, 9919 (1988) 10.1103/PhysRevB.37.9919
-
(1988)
Phys. Rev. B
, vol.37
, pp. 9919
-
-
Svane, A.1
Gunnarsson, O.2
-
26
-
-
0001096812
-
-
10.1103/PhysRevB.56.12058;
-
A. E. Carlsson, Phys. Rev. B 56, 12058 (1997) 10.1103/PhysRevB.56.12058
-
(1997)
Phys. Rev. B
, vol.56
, pp. 12058
-
-
Carlsson, A.E.1
-
27
-
-
0034905805
-
-
10.1103/PhysRevB.63.115116
-
R. G. Hennig and A. E. Carlsson, Phys. Rev. B 63, 115116 (2001). 10.1103/PhysRevB.63.115116
-
(2001)
Phys. Rev. B
, vol.63
, pp. 115116
-
-
Hennig, R.G.1
Carlsson, A.E.2
-
28
-
-
0037865512
-
-
10.1103/PhysRevLett.90.146402
-
N. A. Lima, M. F. Silva, L. N. Oliveira, and K. Capelle, Phys. Rev. Lett. 90, 146402 (2003). 10.1103/PhysRevLett.90.146402
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 146402
-
-
Lima, N.A.1
Silva, M.F.2
Oliveira, L.N.3
Capelle, K.4
-
29
-
-
54849420974
-
-
10.1103/PhysRevLett.101.166401
-
C. Verdozzi, Phys. Rev. Lett. 101, 166401 (2008). 10.1103/PhysRevLett. 101.166401
-
(2008)
Phys. Rev. Lett.
, vol.101
, pp. 166401
-
-
Verdozzi, C.1
-
37
-
-
0000630643
-
-
10.1103/PhysRevB.12.2111;
-
T. L. Gilbert, Phys. Rev. B 12, 2111 (1975) 10.1103/PhysRevB.12.2111
-
(1975)
Phys. Rev. B
, vol.12
, pp. 2111
-
-
Gilbert, T.L.1
-
38
-
-
0000588905
-
-
For more recent studies see, for example, 10.1103/PhysRevLett.81.866
-
For more recent studies see, for example, S. Goedecker and C. J. Umrigar, Phys. Rev. Lett. 81, 866 (1998), and references therein. 10.1103/PhysRevLett. 81.866
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 866
-
-
Goedecker, S.1
Umrigar, C.J.2
-
39
-
-
0000317461
-
-
10.1063/1.440249;
-
S. M. Valone, J. Chem. Phys. 73, 1344 (1980) 10.1063/1.440249
-
(1980)
J. Chem. Phys.
, vol.73
, pp. 1344
-
-
Valone, S.M.1
-
40
-
-
0000329098
-
-
10.1063/1.440656
-
S. M. Valone, J. Chem. Phys. 73, 4653 (1980). 10.1063/1.440656
-
(1980)
J. Chem. Phys.
, vol.73
, pp. 4653
-
-
Valone, S.M.1
-
41
-
-
67650027415
-
-
The LDFT formalism can be easily extended to arbitrary interactions HI = (1/2) Vijkl c iσ † c k σ′ † c l σ′ c jσ by replacing U i n i n i by HI in the expressions for the interaction-energy functional W [γ]. However, note that the functional dependence of W on γ depends crucially on the form of Vijkl (see also Refs.)
-
The LDFT formalism can be easily extended to arbitrary interactions HI = (1/2) Vijkl c iσ † c k σ′ † c l σ′ c jσ by replacing U i n i n i by HI in the expressions for the interaction-energy functional W [γ]. However, note that the functional dependence of W on γ depends crucially on the form of Vijkl (see also Refs.).
-
-
-
-
43
-
-
67650061668
-
-
In the presence of degeneracies in the single-particle spectrum one may find that Levy's minimum W does not derive from a single Slater determinant and that W0 < EHF. However, this is a finite-size effect whose importance decreases with increasing Na.
-
In the presence of degeneracies in the single-particle spectrum one may find that Levy's minimum W does not derive from a single Slater determinant and that W0 < EHF. However, this is a finite-size effect whose importance decreases with increasing Na.
-
-
-
|