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References

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  1. A. S. Barker, Phys. Rev. 165, 917 (1988).
    [Crossref]
  2. S. Roberts, D. D. Coon, J. Opt. Soc. Amer. 52, 1023 (1962).
    [Crossref]
  3. W. L. Bond, J. Appl. Phys. 36, 1674 (1965).
    [Crossref]
  4. H. Ehrenreich, H. R. Phillipp, J. C. Phillips, Phys. Rev. Lett. 8, 59 (1962).
    [Crossref]

1988 (1)

A. S. Barker, Phys. Rev. 165, 917 (1988).
[Crossref]

1965 (1)

W. L. Bond, J. Appl. Phys. 36, 1674 (1965).
[Crossref]

1962 (2)

H. Ehrenreich, H. R. Phillipp, J. C. Phillips, Phys. Rev. Lett. 8, 59 (1962).
[Crossref]

S. Roberts, D. D. Coon, J. Opt. Soc. Amer. 52, 1023 (1962).
[Crossref]

Barker, A. S.

A. S. Barker, Phys. Rev. 165, 917 (1988).
[Crossref]

Bond, W. L.

W. L. Bond, J. Appl. Phys. 36, 1674 (1965).
[Crossref]

Coon, D. D.

S. Roberts, D. D. Coon, J. Opt. Soc. Amer. 52, 1023 (1962).
[Crossref]

Ehrenreich, H.

H. Ehrenreich, H. R. Phillipp, J. C. Phillips, Phys. Rev. Lett. 8, 59 (1962).
[Crossref]

Phillipp, H. R.

H. Ehrenreich, H. R. Phillipp, J. C. Phillips, Phys. Rev. Lett. 8, 59 (1962).
[Crossref]

Phillips, J. C.

H. Ehrenreich, H. R. Phillipp, J. C. Phillips, Phys. Rev. Lett. 8, 59 (1962).
[Crossref]

Roberts, S.

S. Roberts, D. D. Coon, J. Opt. Soc. Amer. 52, 1023 (1962).
[Crossref]

J. Appl. Phys. (1)

W. L. Bond, J. Appl. Phys. 36, 1674 (1965).
[Crossref]

J. Opt. Soc. Amer. (1)

S. Roberts, D. D. Coon, J. Opt. Soc. Amer. 52, 1023 (1962).
[Crossref]

Phys. Rev. (1)

A. S. Barker, Phys. Rev. 165, 917 (1988).
[Crossref]

Phys. Rev. Lett. (1)

H. Ehrenreich, H. R. Phillipp, J. C. Phillips, Phys. Rev. Lett. 8, 59 (1962).
[Crossref]

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Figures (1)

Fig. 1
Fig. 1

Experimental absorption coefficient α and experimental refractive index curve n compared to Eq. (2) (solid line through circles) for GaP. One of the absorption peaks occurs at 181 cm−1 and the other broad flat peak at 148 → 151 cm−1.

Tables (2)

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Table I Comparison of Experimental and Calculated Index Data for GaP

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Table II Dielectric Parameters for GaP at 300 K

Equations (4)

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κ ( ν ) = / 0 = 1 + i S i ν i 2 ( ν i 2 - ν 2 + i ν γ i ) - 1 ,
κ ( ν ) = 1 + i = 1 3 S e i ν e i 2 ( ν e i 2 - ν 2 ) - 1 + [ S 0 ν 0 2 ( 1 - j = 1 2 S 1 j ) ] / [ ( ν 0 2 - ν 2 + i ν γ 0 ) - ν 0 2 j = 1 2 S 1 j ν j 2 ( ν j 2 - ν 2 + i ν γ j ) - 1 ] ,
κ D C = κ ( ν = 0 ) = ( 1 + S e 1 + S e 2 + S e 3 ) + S 0 = κ + S 0 .
κ ( ν ) κ + i = 1 3 S e i ( ν / ν i ) 2 - S 0 ( ν 0 / ν ) 2 = κ + Δ κ e - Δ κ i ,

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