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References

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  1. W. König, Handbuch der Physik, Vol. 20, p. 242. n and k, as used in the present paper, are the same as König’s n0 and (n0ϰ0).
  2. G. Pfestorf, Ann. d. Physik 81, 906 (1926).
    [Crossref]
  3. C. Boeckner, J. Opt. Soc. Am. 19, 7 (1929).
    [Crossref]
  4. H. M. O’Bryan, J. Opt. Soc. Am. 22, 739 (1932).
    [Crossref]
  5. R. Tousey, Phys. Rev. 50, 1057 (1936).
    [Crossref]

1936 (1)

R. Tousey, Phys. Rev. 50, 1057 (1936).
[Crossref]

1932 (1)

1929 (1)

1926 (1)

G. Pfestorf, Ann. d. Physik 81, 906 (1926).
[Crossref]

Boeckner, C.

König, W.

W. König, Handbuch der Physik, Vol. 20, p. 242. n and k, as used in the present paper, are the same as König’s n0 and (n0ϰ0).

O’Bryan, H. M.

Pfestorf, G.

G. Pfestorf, Ann. d. Physik 81, 906 (1926).
[Crossref]

Tousey, R.

R. Tousey, Phys. Rev. 50, 1057 (1936).
[Crossref]

Ann. d. Physik (1)

G. Pfestorf, Ann. d. Physik 81, 906 (1926).
[Crossref]

J. Opt. Soc. Am. (2)

Phys. Rev. (1)

R. Tousey, Phys. Rev. 50, 1057 (1936).
[Crossref]

Other (1)

W. König, Handbuch der Physik, Vol. 20, p. 242. n and k, as used in the present paper, are the same as König’s n0 and (n0ϰ0).

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Figures (5)

Fig. 1
Fig. 1

Curves of constant reflection coefficient illustrating the application of the graphical method to a particular example.

Fig. 2
Fig. 2

Curves showing the relation between n and k for certain values of the reflection coefficient at 45°, for unpolarized incident light.

Fig. 3
Fig. 3

Curves showing the relation between n and k for certain values of the reflection coefficient at 60°, for unpolarized incident light.

Fig. 4
Fig. 4

Curves showing the relation between n and k for certain values of the reflection coefficient at 75°, for unpolarized incident light.

Fig. 5
Fig. 5

Curves showing the relation between n and k for certain values of the reflection coefficient at 85°, for unpolarized incident light.

Equations (4)

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R s = a 2 + b 2 - 2 a cos i + cos 2 i a 2 + b 2 + 2 a cos i + cos 2 i , R p = R s · a 2 + b 2 - 2 a sin i · tan i + sin 2 i · tan 2 i a 2 + b 2 + 2 a sin i · tan i + sin 2 i · tan 2 i ,
2 a 2 = [ ( n 2 - k 2 - sin 2 i ) 2 + 4 n 2 k 2 ] 1 2 + [ ( n 2 - k 2 ) - sin 2 i ] , 2 b 2 = [ ( n 2 - k 2 - sin 2 i ) 2 + 4 n 2 k 2 ] 1 2 - [ ( n 2 - k 2 ) - sin 2 i ] .
R = f ( i , n , k , p ) ,
R 1 = f 1 ( n , k ) , R 2 = f 2 ( n , k ) .