메뉴 건너뛰기




Volumn 59, Issue 8, 1999, Pages 5441-5451

Ab initio calculation of (formula presented) including the electron-hole interaction: Application to gan and (formula presented)

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000656146     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.5441     Document Type: Article
Times cited : (173)

References (45)
  • 12
    • 0032516988 scopus 로고    scopus 로고
    • Phys. Rev. Lett.M. Rohlfing and S.G. Louie, 81, 2312 (1998).
    • (1998) , vol.81 , pp. 2312
    • Rohlfing, M.1    Louie, S.G.2
  • 17
    • 85038285880 scopus 로고    scopus 로고
    • By “IR dielectric constant,” we mean (Formula presented) where (Formula presented) is much less than an electronic transition frequency, but much greater than a typical phonon frequency. This is often refered to as (Formula presented)
    • By “IR dielectric constant,” we mean (Formula presented) where (Formula presented) is much less than an electronic transition frequency, but much greater than a typical phonon frequency. This is often refered to as (Formula presented)
  • 20
    • 85038308137 scopus 로고    scopus 로고
    • (Formula presented) is current per area, so (Formula presented) has units of dipole moment per volume (polarization) if (Formula presented) is set to unity.
    • (Formula presented) is current per area, so (Formula presented) has units of dipole moment per volume (polarization) if (Formula presented) is set to unity.
  • 23
    • 85038271135 scopus 로고    scopus 로고
    • It should be noted that this is not the scheme currently recommended by R. Haydock for use in multiband systems. However, we have found that for all cases tested, our converged results are essentially identical to those of exact diagonalization. We thank R. Haydock and J.D. Joannopoulos for their cautionary remarks in this regard.
    • It should be noted that this is not the scheme currently recommended by R. Haydock for use in multiband systems. However, we have found that for all cases tested, our converged results are essentially identical to those of exact diagonalization. We thank R. Haydock and J.D. Joannopoulos for their cautionary remarks in this regard.
  • 24
    • 0029378555 scopus 로고
    • Random phases were employed to calculate the average density of one-electron states for a disordered two-dimensional system in R. Haerle, R. Haydock, and R.L. Te, Comput. Phys. Commun. 90, 81 (1995).
    • (1995) Comput. Phys. Commun. , vol.90 , pp. 81
    • Haerle, R.1    Haydock, R.2    Te, R.L.3
  • 33
    • 85038305180 scopus 로고    scopus 로고
    • For all calculations we use a (Formula presented) point shift, so that the (Formula presented) point (Formula presented) is shifted to (Formula presented) Such symmetry breaking is not problematic, because it becomes irrelevant when results are converged.
    • For all calculations we use a (Formula presented) point shift, so that the (Formula presented) point (Formula presented) is shifted to (Formula presented) Such symmetry breaking is not problematic, because it becomes irrelevant when results are converged.
  • 34
    • 85038344940 scopus 로고    scopus 로고
    • On close inspection, it is apparent that the peak positions in the theoretical results are slightly off from the measured positions. This may be related to the use of a simple (Formula presented)-independent shift and stretch of the LDA bands. Use of the full (Formula presented) band energies may lead to better agreement.
    • On close inspection, it is apparent that the peak positions in the theoretical results are slightly off from the measured positions. This may be related to the use of a simple (Formula presented)-independent shift and stretch of the LDA bands. Use of the full (Formula presented) band energies may lead to better agreement.
  • 37
    • 85038279409 scopus 로고    scopus 로고
    • M. Rohlfing and S.G. Louie have obtained similar results for the total density of excited states of GaAs with and without the electron-hole interaction (unpublished).
    • M. Rohlfing and S.G. Louie, M. Rohlfing and S.G. Louie have obtained similar results for the total density of excited states of GaAs with and without the electron-hole interaction (unpublished).
    • Rohlfing, M.1    Louie, S.G.2
  • 39
    • 0001559783 scopus 로고
    • 11.8 eV is the indirect gap inferred from the 12.1-eV direct gap (at room temperature) proposed in G.W. Rubloff, Phys. Rev. B 5, 662 (1972).
    • (1972) Phys. Rev. B , vol.5 , pp. 662
    • Rubloff, G.W.1
  • 40
    • 2342639969 scopus 로고
    • ). No mention of temperature appears here; we assume the measurements were performed at room temperature.
    • R. Tousey, Phys. Rev. 50, 1057 (1936). No mention of temperature appears here; we assume the measurements were performed at room temperature.
    • (1936) Phys. Rev. , vol.50 , pp. 1057
    • Tousey, R.1
  • 41
    • 0000149374 scopus 로고
    • ). Measurements were performed at room temperature.
    • T. Tomiki and T. Miyata, J. Phys. Soc. Jpn. 27, 658 (1969). Measurements were performed at room temperature.
    • (1969) J. Phys. Soc. Jpn. , vol.27 , pp. 658
    • Tomiki, T.1    Miyata, T.2
  • 42
    • 0001297493 scopus 로고
    • The data we reproduce here (Fig. 1010) are from a room-temperature measurement. This paper also presents data taken at 90 K; however, the differences between the 90 K and 300 K data are significantly smaller than the differences between either and our theoretical results.
    • J. Barth, R.L. Johnson, M. Cardona, D. Fuchs, and A.M. Bradshaw, Phys. Rev. B 41, 3291 (1990).The data we reproduce here (Fig. 1010) are from a room-temperature measurement. This paper also presents data taken at 90 K; however, the differences between the 90 K and 300 K data are significantly smaller than the differences between either and our theoretical results.
    • (1990) Phys. Rev. B , vol.41 , pp. 3291
    • Barth, J.1    Johnson, R.L.2    Cardona, M.3    Fuchs, D.4    Bradshaw, A.M.5
  • 44
    • 85038324173 scopus 로고    scopus 로고
    • Note that the value of (Formula presented) for (Formula presented) in the continuum (above the band gap) is sensitive to the choice of (Formula presented)
    • Note that the value of (Formula presented) for (Formula presented) in the continuum (above the band gap) is sensitive to the choice of (Formula presented)


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.