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S-cone psychophysics

Published online by Cambridge University Press:  23 April 2014

HANNAH E. SMITHSON*
Affiliation:
Department of Experimental Psychology, University of Oxford, Oxford, UK
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Abstract

We review the features of the S-cone system that appeal to the psychophysicist and summarize the celebrated characteristics of S-cone mediated vision. Two factors are emphasized: First, the fine stimulus control that is required to isolate putative visual mechanisms and second, the relationship between physiological data and psychophysical approaches. We review convergent findings from physiology and psychophysics with respect to asymmetries in the retinal wiring of S-ON and S-OFF visual pathways, and the associated treatment of increments and decrements in the S-cone system. Beyond the retina, we consider the lack of S-cone projections to superior colliculus and the use of S-cone stimuli in experimental psychology, for example to address questions about the mechanisms of visually driven attention. Careful selection of stimulus parameters enables psychophysicists to produce entirely reversible, temporary, “lesions,” and to assess behavior in the absence of specific neural subsystems.

Information

Type
Review Articles
Copyright
Copyright © Cambridge University Press 2014 
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Fig. 1. (a and b) CIE 2006 “physiologically relevant” cone LMS cone fundamentals. Solid lines are sensitivities for the standard 2° observer (parameterized by age 32 years and field size 2°); (a) dashed lines are sensitivities for an older observer (age 60 years; field size 2°); (b) dashed lines are sensitivities for a standard 10° observer (age 32 years; field size 10°); (c) relative spectral energy distributions for the RGB primaries of an example CRT (Sony FD Trinitron); (d and e) MacLeod-Boynton chromaticity diagrams showing paired coordinates of stimuli produced from the CRT primaries and selected to be tritan increments from equal energy white (ΔL/L = 0.0; ΔM/M = 0; ΔS/S = 0.5) for the standard 2° observer and re-plotted in terms of the cone signals they offer to alternative observers. When the alternative observer is the same as the standard observer (solid black lines and crosses) the paired coordinates align with the tritan axis. When the alternative observers differ from the standard (solid cyan to purple series) the paired coordinates are rotated and displaced from the desired locus in color space; (d) alternative observers of age 20, 40, 50, 60, 70, and 80 years; (e) alternative observers with field size 3, 4, 5, 6, 7, 8, 9, and 10°.

Figure 1

Fig. 2. Stiles’ π mechanisms. Field sensitivities – the reciprocals of the field radiances (in log quanta s−1 deg−2) required to raise the threshold of each “isolated” π-mechanism by one log unit above its absolute threshold – of the seven photopic π mechanisms. Three are predominantly S-cone mechanisms (π1, π2, and π3), two M-cone (π4 and π4′), and two L-cone (π5 and π5′). [Data from Table 2(7.4.3) of Wyszecki and Stiles].