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  1. Herbert E. Ives, Phys. Rev. 38, 1209 (1931).
    [Crossref]
  2. W. Voigt, Physik. Zeits. 2, 303 (1901).
  3. R. S. Minor, Ann. d. Physik 10, 581 (1903).
    [Crossref]
  4. W. Meier, Ann. d. Physik 31, 1017 (1910).
    [Crossref]
  5. V. Fréedericksz, Ann. d. Physik 34, 780 (1911).
    [Crossref]
  6. P. Erochin, Ann. d. Physik 39, 213 (1912).
    [Crossref]
  7. Le Roy D. Weld, J. O. S. A. 6, 67 (1922).
    [Crossref]
  8. T. C. Fry, Plane Waves of Light, I, II and III, J. O. S. A. 15, 137 (1927); J. O. S. A. 16, 1 (1928), 307 (1932).
    [Crossref]
  9. T. C. Fry, J. O. S. A. 16, 1 (1928). Dr. Fry has asked us to call attention to an error, which crept into his paper in the process of changing over to a more logical system of notation than that in which it was originally written. The error first appeared in the unnumbered equation preceding (55), p. 23, where the factor r/c(ρ+1) should have been r/c(r+1) and was continued in Eq. (55), which should have been as given above. Beyond that point it does not again appear.
    [Crossref]
  10. L. R. Ingersoll and R. T. Birge, Phys. Rev. 29, 392 (1909).
  11. For the relation between K and K0 see T. C. Fry, J. O. S. A. 15, 143, 144 (1927), footnotes.
    [Crossref]
  12. R. W. Duncan and R. C. Duncan, Phys. Rev. 1, 294 (1913).
    [Crossref]
  13. Brian O’Brien, Phys. Rev. 27, 93 (1926).
    [Crossref]
  14. R. W. Wood, Phys. Rev. 44, 353 (1933).
    [Crossref]
  15. R. de L. Kronig, Nature 133, 211 (1934).
    [Crossref]
  16. C. Zener, Nature 132, 968 (1933).
    [Crossref]
  17. R. de L. Kronig, Proc. Roy. Soc. A133, 255 (1931). See relation (15). See also A. H. Wilson, Proc. Roy. Soc. A151, 282, 283, 284 (1935).
    [Crossref]

1934 (1)

R. de L. Kronig, Nature 133, 211 (1934).
[Crossref]

1933 (2)

C. Zener, Nature 132, 968 (1933).
[Crossref]

R. W. Wood, Phys. Rev. 44, 353 (1933).
[Crossref]

1931 (2)

R. de L. Kronig, Proc. Roy. Soc. A133, 255 (1931). See relation (15). See also A. H. Wilson, Proc. Roy. Soc. A151, 282, 283, 284 (1935).
[Crossref]

Herbert E. Ives, Phys. Rev. 38, 1209 (1931).
[Crossref]

1928 (1)

T. C. Fry, J. O. S. A. 16, 1 (1928). Dr. Fry has asked us to call attention to an error, which crept into his paper in the process of changing over to a more logical system of notation than that in which it was originally written. The error first appeared in the unnumbered equation preceding (55), p. 23, where the factor r/c(ρ+1) should have been r/c(r+1) and was continued in Eq. (55), which should have been as given above. Beyond that point it does not again appear.
[Crossref]

1927 (2)

For the relation between K and K0 see T. C. Fry, J. O. S. A. 15, 143, 144 (1927), footnotes.
[Crossref]

T. C. Fry, Plane Waves of Light, I, II and III, J. O. S. A. 15, 137 (1927); J. O. S. A. 16, 1 (1928), 307 (1932).
[Crossref]

1926 (1)

Brian O’Brien, Phys. Rev. 27, 93 (1926).
[Crossref]

1922 (1)

Le Roy D. Weld, J. O. S. A. 6, 67 (1922).
[Crossref]

1913 (1)

R. W. Duncan and R. C. Duncan, Phys. Rev. 1, 294 (1913).
[Crossref]

1912 (1)

P. Erochin, Ann. d. Physik 39, 213 (1912).
[Crossref]

1911 (1)

V. Fréedericksz, Ann. d. Physik 34, 780 (1911).
[Crossref]

1910 (1)

W. Meier, Ann. d. Physik 31, 1017 (1910).
[Crossref]

1909 (1)

L. R. Ingersoll and R. T. Birge, Phys. Rev. 29, 392 (1909).

1903 (1)

R. S. Minor, Ann. d. Physik 10, 581 (1903).
[Crossref]

1901 (1)

W. Voigt, Physik. Zeits. 2, 303 (1901).

Birge, R. T.

L. R. Ingersoll and R. T. Birge, Phys. Rev. 29, 392 (1909).

Duncan, R. C.

R. W. Duncan and R. C. Duncan, Phys. Rev. 1, 294 (1913).
[Crossref]

Duncan, R. W.

R. W. Duncan and R. C. Duncan, Phys. Rev. 1, 294 (1913).
[Crossref]

Erochin, P.

P. Erochin, Ann. d. Physik 39, 213 (1912).
[Crossref]

Fréedericksz, V.

V. Fréedericksz, Ann. d. Physik 34, 780 (1911).
[Crossref]

Fry, T. C.

T. C. Fry, J. O. S. A. 16, 1 (1928). Dr. Fry has asked us to call attention to an error, which crept into his paper in the process of changing over to a more logical system of notation than that in which it was originally written. The error first appeared in the unnumbered equation preceding (55), p. 23, where the factor r/c(ρ+1) should have been r/c(r+1) and was continued in Eq. (55), which should have been as given above. Beyond that point it does not again appear.
[Crossref]

For the relation between K and K0 see T. C. Fry, J. O. S. A. 15, 143, 144 (1927), footnotes.
[Crossref]

T. C. Fry, Plane Waves of Light, I, II and III, J. O. S. A. 15, 137 (1927); J. O. S. A. 16, 1 (1928), 307 (1932).
[Crossref]

Ingersoll, L. R.

L. R. Ingersoll and R. T. Birge, Phys. Rev. 29, 392 (1909).

Ives, Herbert E.

Herbert E. Ives, Phys. Rev. 38, 1209 (1931).
[Crossref]

Kronig, R. de L.

R. de L. Kronig, Nature 133, 211 (1934).
[Crossref]

R. de L. Kronig, Proc. Roy. Soc. A133, 255 (1931). See relation (15). See also A. H. Wilson, Proc. Roy. Soc. A151, 282, 283, 284 (1935).
[Crossref]

Meier, W.

W. Meier, Ann. d. Physik 31, 1017 (1910).
[Crossref]

Minor, R. S.

R. S. Minor, Ann. d. Physik 10, 581 (1903).
[Crossref]

O’Brien, Brian

Brian O’Brien, Phys. Rev. 27, 93 (1926).
[Crossref]

Voigt, W.

W. Voigt, Physik. Zeits. 2, 303 (1901).

Weld, Le Roy D.

Le Roy D. Weld, J. O. S. A. 6, 67 (1922).
[Crossref]

Wood, R. W.

R. W. Wood, Phys. Rev. 44, 353 (1933).
[Crossref]

Zener, C.

C. Zener, Nature 132, 968 (1933).
[Crossref]

Ann. d. Physik (4)

R. S. Minor, Ann. d. Physik 10, 581 (1903).
[Crossref]

W. Meier, Ann. d. Physik 31, 1017 (1910).
[Crossref]

V. Fréedericksz, Ann. d. Physik 34, 780 (1911).
[Crossref]

P. Erochin, Ann. d. Physik 39, 213 (1912).
[Crossref]

J. O. S. A. (4)

Le Roy D. Weld, J. O. S. A. 6, 67 (1922).
[Crossref]

T. C. Fry, Plane Waves of Light, I, II and III, J. O. S. A. 15, 137 (1927); J. O. S. A. 16, 1 (1928), 307 (1932).
[Crossref]

T. C. Fry, J. O. S. A. 16, 1 (1928). Dr. Fry has asked us to call attention to an error, which crept into his paper in the process of changing over to a more logical system of notation than that in which it was originally written. The error first appeared in the unnumbered equation preceding (55), p. 23, where the factor r/c(ρ+1) should have been r/c(r+1) and was continued in Eq. (55), which should have been as given above. Beyond that point it does not again appear.
[Crossref]

For the relation between K and K0 see T. C. Fry, J. O. S. A. 15, 143, 144 (1927), footnotes.
[Crossref]

Nature (2)

R. de L. Kronig, Nature 133, 211 (1934).
[Crossref]

C. Zener, Nature 132, 968 (1933).
[Crossref]

Phys. Rev. (5)

Herbert E. Ives, Phys. Rev. 38, 1209 (1931).
[Crossref]

R. W. Duncan and R. C. Duncan, Phys. Rev. 1, 294 (1913).
[Crossref]

Brian O’Brien, Phys. Rev. 27, 93 (1926).
[Crossref]

R. W. Wood, Phys. Rev. 44, 353 (1933).
[Crossref]

L. R. Ingersoll and R. T. Birge, Phys. Rev. 29, 392 (1909).

Physik. Zeits. (1)

W. Voigt, Physik. Zeits. 2, 303 (1901).

Proc. Roy. Soc. (1)

R. de L. Kronig, Proc. Roy. Soc. A133, 255 (1931). See relation (15). See also A. H. Wilson, Proc. Roy. Soc. A151, 282, 283, 284 (1935).
[Crossref]

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Figures (11)

Fig. 1
Fig. 1

Diagram of the formation of spot patterns for plane and elliptically polarized light.

Fig. 2
Fig. 2

The optical system.

Fig. 3
Fig. 3

Spot patterns; comparison and reflection negatives for λ3650.

Fig. 4
Fig. 4

Relation between comparison and reflection patterns.

Fig. 5
Fig. 5

Comparison plates, showing variation of spot spacing with wave-length. Top row, left to right, λ4358, 4047, 3650. Bottom row, λ3341, 3126, 2536.

Fig. 6
Fig. 6

Tube for preparing alkali metal surfaces.

Fig. 7
Fig. 7

Quartz prism with potassium mirror attached.

Fig. 8
Fig. 8

Dispersion curves of N and K0 for potassium.

Fig. 9
Fig. 9

Reflecting power of potassium.

Fig. 10
Fig. 10

Calculated transmissions for several thicknesses of potassium.

Fig. 11
Fig. 11

Comparison of experimentally determined optical constants with those calculated from Kronig’s theory.

Tables (2)

Tables Icon

Table III Optical constants of potassium.

Tables Icon

Table IV Transmission.

Equations (4)

Equations on this page are rendered with MathJax. Learn more.

ϕ = ( d / D ) × 180 ,             θ = ( d 1 / D 1 ) × 90.
N + i K 0 = tan I [ ( ρ + 1 ) 2 - 4 ρ sin 2 I ( ρ + 1 ) 2 ] 1 2 ,
ρ = e i ϕ tan θ .
λ 3650 I 60 ° ϕ 39 ° 3 6 θ 45.0 ° N 1.477 N ( I . C . T . ) 1.475 .