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  1. W. H. Stainton, J. Opt. Soc. Am. 16, 26 (1928).
    [Crossref]
  2. J. Schouten and L. Ornstein, J. Opt. Soc. Am. 29, 168 (1939).
    [Crossref]
  3. W. C. Calvert, dissertation, University of California at Los Angeles (August, 1955).
  4. Boynton, Bush, and Enoch, J. Opt. Soc. Am. 44, 56 (1954).
    [Crossref] [PubMed]
  5. R. Boynton and G. Kandel, J. Opt. Soc. Am. 47, 275 (1957).
    [Crossref] [PubMed]
  6. H. K. Hartline, J. Opt. Soc. Am. 30, 239 (1940).
    [Crossref]
  7. H. K. Hartline, Am. J. Physiol. 121, 400 (1938).
  8. H. deLange, J. Opt. Soc. Am. 48, 777 (1958).
    [Crossref]
  9. H. deLange, thesis, Technical University, Delft (June, 1957).
  10. The so-called Weber-Fecher law exemplifies this nonlinearity. See reference 9, Sec. 1.2.
  11. H. deLange, J. Opt. Soc. Am. 44, 380 (1954).
    [Crossref]
  12. H. deLange, Physica 18, 935 (1952).
    [Crossref]
  13. Dissertation project undertaken in 1956, University of California at Los Angeles, to be reported subsequently.(Part of this report submitted to the Journal of the Optical Society of America on May7, 1958).
  14. G. M. Byram, J. Opt. Soc. Am. 34, 718 (1944), see especially p. 730.
    [Crossref]
  15. Riggs, Ratliff, Cornsweet, and Cornsweet, J. Opt. Soc. Am. 43, 495 (1953).
    [Crossref] [PubMed]
  16. R. W. Ditchburn, Optica Acta, Paris 1, 171 (1955).
    [Crossref]
  17. Riggs, Armington, and Ratliff, J. Opt. Soc. Am. 44, 315 (1954).
    [Crossref] [PubMed]
  18. G. M. Byram, J. Opt. Soc. Am. 34, 571 (1944).
    [Crossref]
  19. G. Higgins and K. Stultz, J. Opt. Soc. Am. 43, 1136 (1953).
    [Crossref] [PubMed]

1958 (1)

1957 (1)

1955 (1)

R. W. Ditchburn, Optica Acta, Paris 1, 171 (1955).
[Crossref]

1954 (3)

1953 (2)

1952 (1)

H. deLange, Physica 18, 935 (1952).
[Crossref]

1944 (2)

1940 (1)

1939 (1)

1938 (1)

H. K. Hartline, Am. J. Physiol. 121, 400 (1938).

1928 (1)

Armington,

Boynton,

Boynton, R.

Bush,

Byram, G. M.

Calvert, W. C.

W. C. Calvert, dissertation, University of California at Los Angeles (August, 1955).

Cornsweet,

deLange, H.

H. deLange, J. Opt. Soc. Am. 48, 777 (1958).
[Crossref]

H. deLange, J. Opt. Soc. Am. 44, 380 (1954).
[Crossref]

H. deLange, Physica 18, 935 (1952).
[Crossref]

H. deLange, thesis, Technical University, Delft (June, 1957).

Ditchburn, R. W.

R. W. Ditchburn, Optica Acta, Paris 1, 171 (1955).
[Crossref]

Enoch,

Hartline, H. K.

H. K. Hartline, J. Opt. Soc. Am. 30, 239 (1940).
[Crossref]

H. K. Hartline, Am. J. Physiol. 121, 400 (1938).

Higgins, G.

Kandel, G.

Ornstein, L.

Ratliff,

Riggs,

Schouten, J.

Stainton, W. H.

Stultz, K.

Am. J. Physiol. (1)

H. K. Hartline, Am. J. Physiol. 121, 400 (1938).

J. Opt. Soc. Am. (12)

Optica Acta, Paris (1)

R. W. Ditchburn, Optica Acta, Paris 1, 171 (1955).
[Crossref]

Physica (1)

H. deLange, Physica 18, 935 (1952).
[Crossref]

Other (4)

Dissertation project undertaken in 1956, University of California at Los Angeles, to be reported subsequently.(Part of this report submitted to the Journal of the Optical Society of America on May7, 1958).

W. C. Calvert, dissertation, University of California at Los Angeles (August, 1955).

H. deLange, thesis, Technical University, Delft (June, 1957).

The so-called Weber-Fecher law exemplifies this nonlinearity. See reference 9, Sec. 1.2.

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Figures (2)

F. 1
F. 1

Visual frequency response curves plotted in logarithmic coordinates; i.e., threshold values of the modulation ratio, m, defined by the stimulus wave form f(t) = B(1+m cosωt); retinal illuminance level, B = 103 trolands. Comparison of three different spatial patterns: (a) deLange’s observer V with 2° sharp-edged field and light surround8 (open squares); (b) observer P with Ganzfeld stimulus described in text (open circles); and (c) observer P with 4° sharp-edged field and dark surround (filled circles).

F. 2
F. 2

Visual frequency response curves at the 1-troland level, with same three spatial patterns as in Fig. 1: (a), deLange’s observer L8; (b) and (c), observer D.