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5
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0000209506
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-
Phys. Rev. BS.B. Zhang, D. Tomanek, M.L. Cohen, S.G. Louie, and M.S. Hybertsen, 40, 3162 (1989);
-
(1989)
Phys. Rev. B
, vol.40
, pp. 3162
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-
Zhang, S.B.1
Tomanek, D.2
Cohen, M.L.3
Louie, S.G.4
Hybertsen, M.S.5
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12
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0032516988
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Phys. Rev. Lett.M. Rohlfing and S.G. Louie, 81, 2312 (1998).
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(1998)
, vol.81
, pp. 2312
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Rohlfing, M.1
Louie, S.G.2
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15
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0032070791
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S. Albrecht, L. Reining, R. Del Sole, and G. Onida, Phys. Rev. Lett. 80, 4510 (1998).
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(1998)
Phys. Rev. Lett.
, vol.80
, pp. 4510
-
-
Albrecht, S.1
Reining, L.2
Del Sole, R.3
Onida, G.4
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17
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85038285880
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-
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)
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-
-
-
20
-
-
85038308137
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-
(Formula presented) is current per area, so (Formula presented) has units of dipole moment per volume (polarization) if (Formula presented) is set to unity.
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(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
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85038271135
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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.
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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.
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24
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0029378555
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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
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Haerle, R.1
Haydock, R.2
Te, R.L.3
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26
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0000217676
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-
). Measurements were performed at room temperature.
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W.R.L. Lambrecht, B. Segall, J. Rife, W.R. Hunter, and D.K. Wickenden, Phys. Rev. B 51, 13 516 (1995). Measurements were performed at room temperature.
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(1995)
Phys. Rev. B
, vol.51
, pp. 13
-
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Lambrecht, W.R.L.1
Segall, B.2
Rife, J.3
Hunter, W.R.4
Wickenden, D.K.5
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27
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0000045472
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S. Logothetidis, J. Petalas, M. Cardona, and T.D. Moustakas, Phys. Rev. B 50, 18 017 (1994).
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(1994)
Phys. Rev. B
, vol.50
, pp. 18
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-
Logothetidis, S.1
Petalas, J.2
Cardona, M.3
Moustakas, T.D.4
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28
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0031998227
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T. Wethkamp, K. Wilmers, N. Esser, W. Richter, O. Ambacher, H. Angerer, G. Jungk, R.L. Johnson, and M. Cardona, Thin Solid Films 313-314, 745 (1998).
-
(1998)
Thin Solid Films
, vol.313-314
, pp. 745
-
-
Wethkamp, T.1
Wilmers, K.2
Esser, N.3
Richter, W.4
Ambacher, O.5
Angerer, H.6
Jungk, G.7
Johnson, R.L.8
Cardona, M.9
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29
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85038345506
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C. Janowitz, M. Cardona, R.L. Johnson, T. Cheng, T. Foxon, O. Gunther, and G. Jungk, BESSY Jahresbericht Report No. 230, 1994 (unpublished).
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(1994)
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Janowitz, C.1
Cardona, M.2
Johnson, R.L.3
Cheng, T.4
Foxon, T.5
Gunther, O.6
Jungk, G.7
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32
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0000630807
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A. Rubio, J.L. Corkill, M.L. Cohen, E.L. Shirley, and S.G. Louie, Phys. Rev. B 48, 11 810 (1993).
-
(1993)
Phys. Rev. B
, vol.48
, pp. 11
-
-
Rubio, A.1
Corkill, J.L.2
Cohen, M.L.3
Shirley, E.L.4
Louie, S.G.5
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33
-
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85038305180
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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.
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-
-
-
34
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85038344940
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-
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.
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-
-
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37
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85038279409
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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).
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Rohlfing, M.1
Louie, S.G.2
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38
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0001315394
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A.J. Fischer, W. Shan, J.J. Song, Y.C. Chang, R. Horning, and B. Goldenberg, Appl. Phys. Lett. 71, 1981 (1997).
-
(1997)
Appl. Phys. Lett.
, vol.71
, pp. 1981
-
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Fischer, A.J.1
Shan, W.2
Song, J.J.3
Chang, Y.C.4
Horning, R.5
Goldenberg, B.6
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39
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0001559783
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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
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Rubloff, G.W.1
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40
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2342639969
-
-
). No mention of temperature appears here; we assume the measurements were performed at room temperature.
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R. Tousey, Phys. Rev. 50, 1057 (1936). No mention of temperature appears here; we assume the measurements were performed at room temperature.
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(1936)
Phys. Rev.
, vol.50
, pp. 1057
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Tousey, R.1
-
41
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0000149374
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-
). Measurements were performed at room temperature.
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T. Tomiki and T. Miyata, J. Phys. Soc. Jpn. 27, 658 (1969). Measurements were performed at room temperature.
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(1969)
J. Phys. Soc. Jpn.
, vol.27
, pp. 658
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Tomiki, T.1
Miyata, T.2
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42
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0001297493
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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
-
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Barth, J.1
Johnson, R.L.2
Cardona, M.3
Fuchs, D.4
Bradshaw, A.M.5
-
44
-
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85038324173
-
-
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)
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