色差和消色差对比阈值的时空变化。

D H Kelly
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引用次数: 284

摘要

以恒定速度移动正弦光栅的视网膜图像(补偿眼球运动)在刺激场的每个点提供可控的空间和时间频率。利用这种速度控制技术,我们测量了等亮度,红/绿光栅的检测阈值作为其空间和时间频率的函数。用这种方法得到的彩色对比阈值表面与以前测量的消色差对比阈值表面类似,但结果有很大的不同。对于非常低的时间频率(低于0.2 Hz),色度灵敏度随时间频率的降低而稳定下降。低于0.01 Hz,即使在最大对比度下,彩色图案也会完全消失(尽管消色差或同色图案不会)。在0.2 Hz以上的区域,消色差阈值和彩色阈值都可以用相同的类接受场模型来解释。将该模型的中心分量和环绕分量相加,形成彩色阈值面;当任一组分的符号反转时,它们形成消色差。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spatiotemporal variation of chromatic and achromatic contrast thresholds.

Moving the retinal image of a sinusoidal grating at a constant velocity (compensated for eye movements) provides controlled spatial and temporal frequencies at every point in the stimulus field. Using this controlled-velocity technique, we have measured the detection threshold for isoluminance, red/green gratings as a function of their spatial and temporal frequencies. The chromatic contrast-threshold surface obtained in this way is analogous to the achromatic contrast-threshold surface measured previously, but the results are quite different. For very low temporal frequencies (below 0.2 Hz), the chromatic sensitivity decreases steadily with decreasing temporal frequency. Below 0.01 Hz, chromatic patterns disappear completely even at maximum contrast (although achromatic or homochromatic patterns do not). In the region above 0.2 Hz, both achromatic and chromatic thresholds can be explained by the same receptive-field-like model. When the center and the surround components of this model are additively combined, they form the chromatic threshold surface; when the sign of either component is reversed, they form the achromatic one.

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期刊介绍: OSA was published by The Optical Society from January 1917 to December 1983 before dividing into JOSA A: Optics and Image Science and JOSA B: Optical Physics in 1984.
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