-
2
-
-
11944256577
-
-
M C. Payne, M P. Teter, D C. Allen, T A. Arias, and J D. Joannopoulos, Rev. Mod. Phys.64, 1045 (1992).
-
(1992)
Rev. Mod. Phys.
, vol.64
, pp. 1045
-
-
Payne, M.C.1
Teter, M.P.2
Allen, D.C.3
Arias, T.A.4
Joannopoulos, J.D.5
-
3
-
-
0000917236
-
-
N. Chetty, M. Weinert, T. Rahman, and J. Davenport, Phys. Rev. B52, 6313 (1995).
-
(1995)
Phys. Rev. B
, vol.52
, pp. 6313
-
-
Chetty, N.1
Weinert, M.2
Rahman, T.3
Davenport, J.4
-
4
-
-
0033554907
-
-
I. Lubomirsky, E. Gurovich, S A. Safran, and D. Cahen, Europhys. Lett.45, 201 (1999).
-
(1999)
Europhys. Lett.
, vol.45
, pp. 201
-
-
Lubomirsky, I.1
Gurovich, E.2
Safran, S.A.3
Cahen, D.4
-
7
-
-
0037087975
-
-
N. Knorr, H. Brume, M. Epple, A. Hirstein, M A. Schneider, and K. Kern, Phys. Rev. B65, 115420 (2002).
-
(2002)
Phys. Rev. B
, vol.65
, pp. 115420
-
-
Knorr, N.1
Brume, H.2
Epple, M.3
Hirstein, A.4
Schneider, M.A.5
Kern, K.6
-
10
-
-
0029753418
-
-
H X. Liu, H L. Zhang, H L. Ren, S X. Ouyang, and R Z. Yuan, Ceram. Int.22, 79 (1996).
-
(1996)
Ceram. Int.
, vol.22
, pp. 79
-
-
Liu, H.X.1
Zhang, H.L.2
Ren, H.L.3
Ouyang, S.X.4
Yuan, R.Z.5
-
13
-
-
0000141731
-
-
V S. Stepanyuk, W. Hergert, P. Rennert, K. Wildberger, R. Zeller, and P H. Dederichs, Phys. Rev. B54, 14 121 (1996).
-
(1996)
Phys. Rev. B
, vol.54
, pp. 14-121
-
-
Stepanyuk, V.S.1
Hergert, W.2
Rennert, P.3
Wildberger, K.4
Zeller, R.5
Dederichs, P.H.6
-
14
-
-
0001020840
-
-
E A. Smirnova, I A. Abrikosov, B. Johansson, Y K. Vekilov, A N. Baranov, V S. Stepanyuk, W. Hergert, and P H. Dederichs, Phys. Rev. B59, 14 417 (1999).
-
(1999)
Phys. Rev. B
, vol.59
, pp. 14-417
-
-
Smirnova, E.A.1
Abrikosov, I.A.2
Johansson, B.3
Vekilov, Y.K.4
Baranov, A.N.5
Stepanyuk, V.S.6
Hergert, W.7
Dederichs, P.H.8
-
16
-
-
0000233454
-
-
M I. Trioni, S. Marcotulio, G. Santoro, V. Bortolani, G. Palumbo, and G P. Brivio, Phys. Rev. B58, 11 043 (1998).
-
(1998)
Phys. Rev. B
, vol.58
, pp. 11-43
-
-
Trioni, M.I.1
Marcotulio, S.2
Santoro, G.3
Bortolani, V.4
Palumbo, G.5
Brivio, G.P.6
-
17
-
-
0001023577
-
-
B. Drittler, M. Weinert, R. Zeller, and P H. Dederichs, Phys. Rev. B39, 930 (1989).
-
(1989)
Phys. Rev. B
, vol.39
, pp. 930
-
-
Drittler, B.1
Weinert, M.2
Zeller, R.3
Dederichs, P.H.4
-
19
-
-
0000144117
-
-
M I. Trioni, G P. Brivio, S. Crampin, and J E. Inglesfield, Phys. Rev. B53, 8052 (1996).
-
(1996)
Phys. Rev. B
, vol.53
, pp. 8052
-
-
Trioni, M.I.1
Brivio, G.P.2
Crampin, S.3
Inglesfield, J.E.4
-
21
-
-
85038322544
-
-
J.M. Ziman, (Cambridge University Press, Cambridge, 1964)
-
J.M. Ziman, Principles of the Theory of Solids (Cambridge University Press, Cambridge, 1964).
-
-
-
-
26
-
-
85038339075
-
-
P. Young, (Cambridge University Press, Cambridge, 1988)
-
P. Young, Density Functional Theory (Cambridge University Press, Cambridge, 1988).
-
-
-
-
27
-
-
85038317482
-
-
We performed the LDA calculation of the isolated atom energy (formula presented) with the same muffin tin radius used for the interacting impurity system. While this choice does not provide the best attainable value of (formula presented) it allows for a compensation of the errors in the core level energy evaluation when computing (formula presented) The jellium vacancy energy (formula presented) is calculated with respect to the ideal jellium with optimized parameters. On the one hand, with this choice of the energy reference system, the quantity (formula presented) represents the energy required to introduce an atom in a substrate vacancy. On the other hand, such energy difference retains a variational nature because (formula presented) and (formula presented) are fixed additive constants
-
We performed the LDA calculation of the isolated atom energy (formula presented) with the same muffin tin radius used for the interacting impurity system. While this choice does not provide the best attainable value of (formula presented) it allows for a compensation of the errors in the core level energy evaluation when computing (formula presented) The jellium vacancy energy (formula presented) is calculated with respect to the ideal jellium with optimized parameters. On the one hand, with this choice of the energy reference system, the quantity (formula presented) represents the energy required to introduce an atom in a substrate vacancy. On the other hand, such energy difference retains a variational nature because (formula presented) and (formula presented) are fixed additive constants.
-
-
-
-
29
-
-
85038277138
-
-
http://math.nist.gov/DFTdata/atomdata/tables/ptable.html
-
URL http://math.nist.gov/DFTdata/atomdata/tables/ptable.html.
-
-
-
|