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References

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  1. N. G. Jerlov, Tellus 7, 218 (1955).
    [Crossref]
  2. T. Hatch and S. P. Choate, Franklin Inst. 210, 793 (1930).
    [Crossref]
  3. A. Ivanoff, Compt. rend. 246, 2636 (1958).
  4. A. Ivanoff, Compt. rend. (to be published).
  5. N. G. Jerlov, Repts. Swedish Deep-Sea Expedition III, 3 (1951).

1958 (1)

A. Ivanoff, Compt. rend. 246, 2636 (1958).

1955 (1)

N. G. Jerlov, Tellus 7, 218 (1955).
[Crossref]

1951 (1)

N. G. Jerlov, Repts. Swedish Deep-Sea Expedition III, 3 (1951).

1930 (1)

T. Hatch and S. P. Choate, Franklin Inst. 210, 793 (1930).
[Crossref]

Choate, S. P.

T. Hatch and S. P. Choate, Franklin Inst. 210, 793 (1930).
[Crossref]

Hatch, T.

T. Hatch and S. P. Choate, Franklin Inst. 210, 793 (1930).
[Crossref]

Ivanoff, A.

A. Ivanoff, Compt. rend. 246, 2636 (1958).

A. Ivanoff, Compt. rend. (to be published).

Jerlov, N. G.

N. G. Jerlov, Tellus 7, 218 (1955).
[Crossref]

N. G. Jerlov, Repts. Swedish Deep-Sea Expedition III, 3 (1951).

Compt. rend. (1)

A. Ivanoff, Compt. rend. 246, 2636 (1958).

Franklin Inst. (1)

T. Hatch and S. P. Choate, Franklin Inst. 210, 793 (1930).
[Crossref]

Repts. Swedish Deep-Sea Expedition (1)

N. G. Jerlov, Repts. Swedish Deep-Sea Expedition III, 3 (1951).

Tellus (1)

N. G. Jerlov, Tellus 7, 218 (1955).
[Crossref]

Other (1)

A. Ivanoff, Compt. rend. (to be published).

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Figures (2)

Fig. 1
Fig. 1

Diagram of apparatus used. A quarter wavelength plate, not represented on the figure, transforms the linearly polarized light issued from the prism G into circularly polarized light, in order to eliminate possible variations in the photocathode’s sensitivity with different planes of polarization. A cube of diffusing glass is introduced from time to time in the tank C, in order to check the bulb’s and the multiplier phototube’s stabilities.

Fig. 2
Fig. 2

Numbers along the diagram represent the depth in meters. The scattering coefficient β had been taken equal to 1 for a clear double-distilled water (for which p was equal to 79%). Instead of using the degree of polarization p (which is the ratio of the intensity of the polarized fraction of light to the total intensity), it can be more convenient to use directly the ratio ρ between the minimal and the maximal intensities obtained by turning the prism G. The relationship is p=(1−ρ)/(1+ρ).