Abstract
1. The paper which precedes this investigated the nerve interaction between two flashes, λ at centre (Fig. 1a) and ϕ on the surround region (but not on the centre). The size of the inhibitory nerve signal V generated by ϕ is given by V = ϕ(ϕ + σ), where σ is the semi-saturation constant.
2. A former paper (Alpern & Rushton, 1967) had shown that when the flash ϕ falls upon a steady background θ, V suffers attenuation in the G-box (Fig. 1b) down to the fraction θD/(θD + θ) where θD is the eigengrau or receptor noise. Thus, in general, the nerve signal N is given by [Formula: see text].
3. This formula had only been established for a moderate range of values. In this paper we use extreme values to explore the limits of its validity. We find the equation to be true over the entire intensity range where N is measurable.
4. Six different types of experiment have been performed to test various features of the equation. For instance, if log N is plotted against log ϕ for various fixed values of θ, the curve is always the same with simply a vertical shift. And the shift is equal to log(1 + θ/θD) for all values both of θ and of ϕ.
5. The most interesting curve is the plot of log ϕ against log θ for fixed N. This is similar to the Weber—Fechner increment threshold but the criterion is not that ϕ be strong enough to be detected, but strong enough to generate an N signal just sufficient to inhibit some fixed λ flash. These curves (below the onset of saturation) are all the same except for vertical separation, and prove that the condition for flash detection is that a fixed signal, N0, is generated of size 10-5 of the maximum signal obtainable (i.e. with ϕ large and θ zero).
6. With strong backgrounds the curves of (5) above exhibit a marked saturation of the Aguilar & Stiles' type (1954). The family of curves each with a fixed N value shows a remarkable symmetry (Fig. 8) which in fact follows from the equation in (2) above. It has nothing to do with bleached pigment, but follows from the equation in (1) above. V there cannot exceed unity, thus when scaled by the G-box below the criterion level, further increase in ϕ will not bring improvement.
Full text
PDF


















Selected References
These references are in PubMed. This may not be the complete list of references from this article.
- ALPERN M. ROD-CONE INDEPENDENCE IN THE AFTER-FLASH EFFECT. J Physiol. 1965 Feb;176:462–472. doi: 10.1113/jphysiol.1965.sp007561. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Alpern M., Rushton W. A. The nature of rise in threshold produced by contrast-flashes. J Physiol. 1967 Apr;189(3):519–534. doi: 10.1113/jphysiol.1967.sp008182. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Alpern M., Rushton W. A., Torii S. The size of rod signals. J Physiol. 1970 Jan;206(1):193–208. doi: 10.1113/jphysiol.1970.sp009006. [DOI] [PMC free article] [PubMed] [Google Scholar]
- BARLOW H. B. Increment thresholds at low intensities considered as signal/noise discriminations. J Physiol. 1957 May 23;136(3):469–488. doi: 10.1113/jphysiol.1957.sp005774. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Blakemore C. B., Rushton W. A. The rod increment threshold during dark adaptation in normal and rod monochromat. J Physiol. 1965 Dec;181(3):629–640. doi: 10.1113/jphysiol.1965.sp007787. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Naka K. I. Computer assisted analysis of S-potentials. Biophys J. 1969 Jun;9(6):845–859. doi: 10.1016/S0006-3495(69)86422-2. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Naka K. I., Rushton W. A. S-potentials from luminosity units in the retina of fish (Cyprinidae). J Physiol. 1966 Aug;185(3):587–599. doi: 10.1113/jphysiol.1966.sp008003. [DOI] [PMC free article] [PubMed] [Google Scholar]
- RUSHTON W. A. Rhodopsin measurement and dark-adaptation in a subject deficient in cone vision. J Physiol. 1961 Apr;156:193–205. doi: 10.1113/jphysiol.1961.sp006668. [DOI] [PMC free article] [PubMed] [Google Scholar]