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  1. H. R. Gordon, D. K. Clark, J. W. Brown, O. B. Brown, R. H. Evans, W. W. Broenkow, Appl. Opt. 22, 20 (1983).The notation used in this Letter is identical to that in this reference and hence will not be described here.
    [CrossRef] [PubMed]
  2. H. R. Gordon, Appl. Opt. 20, 207 (1981).
    [CrossRef] [PubMed]
  3. These were provided by R. W. Austin and have the property that variation of the sensor gain while viewing essentially homogeneous water masses results in no variation in the computed sensor radiance Lt.
  4. H. Neckel, D. Labs, Sol. Phys. 74, 231 (1981).
    [CrossRef]
  5. H. R. Gordon, D. K. Clark, Appl. Opt. 20, 4175 (1981).
    [CrossRef] [PubMed]
  6. D. W. Menzel, J. H. Ryther, Deep Sea Res. 6, 351 (1960).

1983 (1)

1981 (3)

1960 (1)

D. W. Menzel, J. H. Ryther, Deep Sea Res. 6, 351 (1960).

Broenkow, W. W.

Brown, J. W.

Brown, O. B.

Clark, D. K.

Evans, R. H.

Gordon, H. R.

Labs, D.

H. Neckel, D. Labs, Sol. Phys. 74, 231 (1981).
[CrossRef]

Menzel, D. W.

D. W. Menzel, J. H. Ryther, Deep Sea Res. 6, 351 (1960).

Neckel, H.

H. Neckel, D. Labs, Sol. Phys. 74, 231 (1981).
[CrossRef]

Ryther, J. H.

D. W. Menzel, J. H. Ryther, Deep Sea Res. 6, 351 (1960).

Appl. Opt. (3)

Deep Sea Res. (1)

D. W. Menzel, J. H. Ryther, Deep Sea Res. 6, 351 (1960).

Sol. Phys (1)

H. Neckel, D. Labs, Sol. Phys. 74, 231 (1981).
[CrossRef]

Other (1)

These were provided by R. W. Austin and have the property that variation of the sensor gain while viewing essentially homogeneous water masses results in no variation in the computed sensor radiance Lt.

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Figures (2)

Fig. 1
Fig. 1

Decay factor f(N) for CZCS bands 1, 2, and 3. The dashed curve is intended to guide the reader in recognizing the band 1 factors. The error bars on the right represent the error that would be generated in f(N) by uncertainties in C and .

Fig. 2
Fig. 2

Decay factor f(N) for CZCS band 1. The error bars represent the error induced by uncertainty in C. The points with the large error bars are in March and/or April, There are no error bars on the points with N < 4000 because Lw(λ) was directly measured for these.

Tables (2)

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Table I CZCS Calibration for the Various Sensor Gains

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Table II Derived Value of a(λ), b(λ), and c(λ)

Equations (3)

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L t ( λ ) = [ A ( λ ) D N ( λ ) + B ( λ ) ] C ( λ ) ,
L t calc = f ( N ) L t true
t ( λ i ) L w ( λ i ) = f 1 ( N , λ i ) L t ( λ i ) L r ( λ i ) S ( λ 1 , λ 4 ) [ L t ( λ 4 ) L r ( λ 4 ) t ( λ 4 ) L w ( λ 4 ) ] .

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