메뉴 건너뛰기




Volumn 242, Issue 10, 2005, Pages 2051-2060

The electron-gas pair density and its geminal representation II. The long-range asymptotics of the Kimball-Overhauser geminals

Author keywords

[No Author keywords available]

Indexed keywords


EID: 23944475117     PISSN: 03701972     EISSN: None     Source Type: Journal    
DOI: 10.1002/pssb.200540074     Document Type: Article
Times cited : (5)

References (50)
  • 1
    • 23944466717 scopus 로고    scopus 로고
    • note
    • 2(1|1′,)-∫d2γ(1|2)γ(2|1′) is a quadratic equation for the 1-matrix, supposed Χ2(1|1′, 2|2) is known. For reduced density matrices in general cf. [2-4], for the 2-matrix and its cumulant partitioning in particular cf. e.g. [5, 6], for inequalities cf. [7-9].
  • 5
    • 0037026940 scopus 로고    scopus 로고
    • P. Ziesche, Int. J. Quantum Chem. 90, 342 (2002). The last line of the Abstract has to be deleted.
    • (2002) Int. J. Quantum Chem. , vol.90 , pp. 342
    • Ziesche, P.1
  • 15
    • 0007212350 scopus 로고    scopus 로고
    • Phys. Rev. B 61, 7353 (2000);
    • (2000) Phys. Rev. B , vol.61 , pp. 7353
  • 16
    • 9744279225 scopus 로고    scopus 로고
    • Phys. Rev. B 66, 159901 (E) (2002).
    • (2002) Phys. Rev. B , vol.66
  • 18
    • 0000345634 scopus 로고
    • J. C. Kimball, Phys. Rev. A 7, 1648 (1973). Therein the cusp theorem for antiparallel-spin pairs of the Coulomb hole is derived, whereas
    • (1973) Phys. Rev. A , vol.7 , pp. 1648
    • Kimball, J.C.1
  • 26
    • 23944443575 scopus 로고    scopus 로고
    • B. Davoudi, M. Polini, R. Asgari, and M. P. Tosi, cond-mat/0206456.
    • B. Davoudi, M. Polini, R. Asgari, and M. P. Tosi, cond-mat/0206456.
  • 28
    • 23944470468 scopus 로고    scopus 로고
    • R. Asgari, M. Cardenas, M. Polini, B. Davoudi, and M. P. Tosi, cond-mat/0408293
    • R. Asgari, M. Cardenas, M. Polini, B. Davoudi, and M. P. Tosi, cond-mat/0408293.
  • 32
    • 1542338494 scopus 로고    scopus 로고
    • P. Ziesche, Phys. Rev. B 67, 233102 (2003). Therein the singlet/triplet PDs are erroneously normalized as g±(∞) = 1/2 instead of the correct normalization g±(∞) = 1.
    • (2003) Phys. Rev. B , vol.67 , pp. 233102
    • Ziesche, P.1
  • 34
    • 10844289649 scopus 로고    scopus 로고
    • s), instead of (the first line...). In Eq. (B.1) read sin (kr)k·n(k) instead of sin krk-n(k); similar corrections are in Eqs. (C.1), (C.5), (D.1) and Table D.1.
    • (2004) Phys. Stat. Sol. (b) , vol.241 , pp. 3544
    • Ziesche, P.1
  • 36
    • 23944450925 scopus 로고    scopus 로고
    • 3/2)Θ(1-k), cf. Refs. [8], [34-36]
    • 3/2)Θ(1-k), cf. Refs. [8], [34-36].
  • 43
    • 23944446412 scopus 로고    scopus 로고
    • note
    • pl) of the static structure factor S(q).
  • 44
    • 23944508862 scopus 로고    scopus 로고
    • note
    • c.
  • 46
    • 0003398526 scopus 로고
    • Density functional theory
    • Springer, Berlin
    • This divergence compensation resembles to some extent to the well-known error compensation of the exchange and correlation energy in DFT, cf. e.g. R. M. Dreizier and E. K. U. Gross, Density Functional Theory. An Approach to the Quantum Many-Body Problem (Springer, Berlin, 1990), p. 187, (ii).
    • (1990) An Approach to the Quantum Many-body Problem , pp. 187
    • Dreizier, R.M.1    Gross, E.K.U.2
  • 50
    • 23944479240 scopus 로고    scopus 로고
    • note
    • F, but roughly the reciprocal of the first-neighbor distance in such a Wigner lattice.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.