메뉴 건너뛰기




Volumn 59, Issue 19, 1999, Pages 12188-12191

Ab initio calculations of the dynamical response of copper

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000745904     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.12188     Document Type: Article
Times cited : (37)

References (37)
  • 8
    • 16444365490 scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.