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Journal of the Optical Society of America

Journal of the Optical Society of America

  • Vol. 70, Iss. 11 — Nov. 1, 1980
  • pp: 1306–1310

Contrast sensitivity measures and accuracy of image stabilization systems

Ülker Tulunay-Keesey and Robert Michael Jones  »View Author Affiliations


JOSA, Vol. 70, Issue 11, pp. 1306-1310 (1980)
http://dx.doi.org/10.1364/JOSA.70.001306


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Abstract

Recently, it has been argued that the precision of image stabilization is reflected in the magnitude of the differences in contrast sensitivity measures obtained with and without image stabilization. Here we present two sets of data, one showing large and the other small differences in contrast sensitivity to sinusoidal gratings viewed under stabilized and unstabilized, normal conditions. Both sets of data were obtained by the use of the same apparatus optimized for image stabilization. Large differences occur between unstabilized and stabilized measures of sensitivity only when the observer is allowed to scan the unstabilized test grating, or to prolong inspection of the stabilized target thus allowing for disappearance of the stabilized image. On the other hand, when the target is presented for a few seconds and the observer fixates on it, normal image motion, which results from eye movements of fixation, is found to enhance contrast sensitivity by only a small amount. It would appear, therefore, that the extent of reduction of sensitivity for a stabilized grating cannot be used as an index of the precision of image stabilization.

© 1980 Optical Society of America

Citation
Ülker Tulunay-Keesey and Robert Michael Jones, "Contrast sensitivity measures and accuracy of image stabilization systems," J. Opt. Soc. Am. 70, 1306-1310 (1980)
http://www.opticsinfobase.org/josa/abstract.cfm?URI=josa-70-11-1306


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References

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  18. Sekular20 has pointed out that phase alternating sinusoidal gratings can be expressed mathematically as the sum of two gratings drifting in opposite directions. This concept can be extended to any target whose contrast varies as a function of time, as when contrast is manipulated manually to determine thresholds. In this sense, none of the stimuli used by us or by others is free of moving components. In the case of the Gaussian presentation we used, the temporal variations can be specified. Each grating has a steady component at a fixed frequency and two components of the same frequency but half amplitude moving in opposite directions, with velocities that depend on the duration of the waveform. By assuming that the Gaussian is closely related to the raised cosine, it has been calculated that for a 5-cpd grating, with a period of 15 s, for example, the moving components have a velocity of 0.7 min arc/s.
  19. Kelly8 states that our data in Ref. 5 shows unaccountably low contrast sensitivity. These data were gathered on a subject with a generally low spatial contrast sensitivity (UTK) with the method of adjustment under careful fixation, conditions favorable to reduction of sensitivity by virtue of lengthy exposure to contrast. Our data in the same paper5 as well as in subsequent papers6 show a peak of contrast sensitivity between the frequencies of 2 and 4 cpd at contrast values ranging between 0.3 and 1%, levels as low as have been reported in the literature so far.
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  22. R. Sekular, A. Pantle, and E. Levinson, "Physiological Basis of Motion Perception," in Handbook of Physiology, VII Perception, edited by R. Held, W. Leibowitz, and H. L. Teuber (Springer-Verlag, New York, 1978).

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