-
8
-
-
16444365490
-
-
B. Farid, et al., Phys. Rev. B 44, 13 349 (1991);
-
(1991)
Phys. Rev. B
, vol.44
, pp. 13 349
-
-
Farid, B.1
-
21
-
-
85037889768
-
-
This cutoff corresponds to keeping approximately (Formula presented) vectors in the plane-wave expansion.
-
This cutoff corresponds to keeping approximately (Formula presented) vectors in the plane-wave expansion.
-
-
-
-
29
-
-
85037910276
-
-
An important issue is the role of the numerical damping (Formula presented), introduced in the evaluation of Eq. (2). We have performed calculations with three different values of (Formula presented), and 0.4 eV, and we have found no differences apart from some noise at 0.1 and 0.2 eV.
-
An important issue is the role of the numerical damping (Formula presented), introduced in the evaluation of Eq. (2). We have performed calculations with three different values of (Formula presented), and 0.4 eV, and we have found no differences apart from some noise at 0.1 and 0.2 eV.
-
-
-
-
33
-
-
33645426115
-
-
The pseudopotential for Cu reproduces within a few percent all the structural properties of this material.
-
N. Troullier and J. L. Martins, Phys. Rev. B 43, 1993 (1991).The pseudopotential for Cu reproduces within a few percent all the structural properties of this material.
-
(1991)
Phys. Rev. B
, vol.43
, pp. 1993
-
-
Troullier, N.1
Martins, J.L.2
-
35
-
-
85037915032
-
-
We have also solved Eq. (1) with all off-diagonal elements of the polarizability excluded, and we have found quantitative deviations from the full calculations of about 10–20 % for energies above 30 eV. Calculations, as obtained with inclusion of local-field effects, have ben performed with use of (Formula presented) (Formula presented), and (Formula presented) vectors in Eq. (1), and the results presented here have been found to be well converged, for all values of the wave vector (Formula presented) used in our calculations, with 15 (Formula presented) vectors in the representation of the matrix (Formula presented).
-
We have also solved Eq. (1) with all off-diagonal elements of the polarizability excluded, and we have found quantitative deviations from the full calculations of about 10–20 % for energies above 30 eV. Calculations, as obtained with inclusion of local-field effects, have ben performed with use of (Formula presented) (Formula presented), and (Formula presented) vectors in Eq. (1), and the results presented here have been found to be well converged, for all values of the wave vector (Formula presented) used in our calculations, with 15 (Formula presented) vectors in the representation of the matrix (Formula presented).
-
-
-
-
36
-
-
85037887817
-
-
The plasma frequency of a free-electron gas with the electron density equal to that of valence (Formula presented) electrons in Cu is (Formula presented).
-
The plasma frequency of a free-electron gas with the electron density equal to that of valence (Formula presented) electrons in Cu is (Formula presented).
-
-
-
-
37
-
-
85037906257
-
-
In the case of Cu, there exists an excitation gap in the L point of the BZ for energies between 20 eV and 30 eV above the Fermi level.
-
In the case of Cu, there exists an excitation gap in the L point of the BZ for energies between 20 eV and 30 eV above the Fermi level.
-
-
-
|