Of the stimulus attributes that affect reaction time, the two relationships that have been most clearly described are contrast and luminance. These relationships are often modeled by Piéron's law (Piéron,
1914; Piéron,
1920; Piéron,
1952; see also Hughes & Kesley,
1984; Pins & Bonnet,
1996; Jaskowski & Sobieralska,
2004; Taylor, Carpenter, & Anderson,
2006). This law describes how, for a given scenario, we will respond slowly to stimuli that are at or near the threshold of our detection. From there, as the intensity of the stimulus increases, our reaction time decreases following a negative power function, until it reaches an asymptote.
Given the well-known deficits in contrast sensitivity in the amblyopic eye, a natural question is whether the prolonged reaction times are simply a consequence of reduced stimulus visibility. One advantage of measuring reaction time in amblyopic participants is that they can serve as their own control, thus eliminating the challenges associated with cognitive effects.
To address this question, we will measure saccadic reaction time to perifoveal stimuli as a function of
effective stimulus contrast (i.e., contrast scaled by the amblyopic eye's contrast threshold). Thus, rather than plotting reaction time versus contrast in percent, we plot reaction versus contrast in threshold units (CTU), and use a modified version of Piéron's law described by Burr, Fiorentini, and Morrone (
1998) to the reaction times measured in this study:
\(\def\upalpha{\unicode[Times]{x3B1}}\)\(\def\upbeta{\unicode[Times]{x3B2}}\)\(\def\upgamma{\unicode[Times]{x3B3}}\)\(\def\updelta{\unicode[Times]{x3B4}}\)\(\def\upvarepsilon{\unicode[Times]{x3B5}}\)\(\def\upzeta{\unicode[Times]{x3B6}}\)\(\def\upeta{\unicode[Times]{x3B7}}\)\(\def\uptheta{\unicode[Times]{x3B8}}\)\(\def\upiota{\unicode[Times]{x3B9}}\)\(\def\upkappa{\unicode[Times]{x3BA}}\)\(\def\uplambda{\unicode[Times]{x3BB}}\)\(\def\upmu{\unicode[Times]{x3BC}}\)\(\def\upnu{\unicode[Times]{x3BD}}\)\(\def\upxi{\unicode[Times]{x3BE}}\)\(\def\upomicron{\unicode[Times]{x3BF}}\)\(\def\uppi{\unicode[Times]{x3C0}}\)\(\def\uprho{\unicode[Times]{x3C1}}\)\(\def\upsigma{\unicode[Times]{x3C3}}\)\(\def\uptau{\unicode[Times]{x3C4}}\)\(\def\upupsilon{\unicode[Times]{x3C5}}\)\(\def\upphi{\unicode[Times]{x3C6}}\)\(\def\upchi{\unicode[Times]{x3C7}}\)\(\def\uppsy{\unicode[Times]{x3C8}}\)\(\def\upomega{\unicode[Times]{x3C9}}\)\(\def\bialpha{\boldsymbol{\alpha}}\)\(\def\bibeta{\boldsymbol{\beta}}\)\(\def\bigamma{\boldsymbol{\gamma}}\)\(\def\bidelta{\boldsymbol{\delta}}\)\(\def\bivarepsilon{\boldsymbol{\varepsilon}}\)\(\def\bizeta{\boldsymbol{\zeta}}\)\(\def\bieta{\boldsymbol{\eta}}\)\(\def\bitheta{\boldsymbol{\theta}}\)\(\def\biiota{\boldsymbol{\iota}}\)\(\def\bikappa{\boldsymbol{\kappa}}\)\(\def\bilambda{\boldsymbol{\lambda}}\)\(\def\bimu{\boldsymbol{\mu}}\)\(\def\binu{\boldsymbol{\nu}}\)\(\def\bixi{\boldsymbol{\xi}}\)\(\def\biomicron{\boldsymbol{\micron}}\)\(\def\bipi{\boldsymbol{\pi}}\)\(\def\birho{\boldsymbol{\rho}}\)\(\def\bisigma{\boldsymbol{\sigma}}\)\(\def\bitau{\boldsymbol{\tau}}\)\(\def\biupsilon{\boldsymbol{\upsilon}}\)\(\def\biphi{\boldsymbol{\phi}}\)\(\def\bichi{\boldsymbol{\chi}}\)\(\def\bipsy{\boldsymbol{\psy}}\)\(\def\biomega{\boldsymbol{\omega}}\)\(\def\bupalpha{\unicode[Times]{x1D6C2}}\)\(\def\bupbeta{\unicode[Times]{x1D6C3}}\)\(\def\bupgamma{\unicode[Times]{x1D6C4}}\)\(\def\bupdelta{\unicode[Times]{x1D6C5}}\)\(\def\bupepsilon{\unicode[Times]{x1D6C6}}\)\(\def\bupvarepsilon{\unicode[Times]{x1D6DC}}\)\(\def\bupzeta{\unicode[Times]{x1D6C7}}\)\(\def\bupeta{\unicode[Times]{x1D6C8}}\)\(\def\buptheta{\unicode[Times]{x1D6C9}}\)\(\def\bupiota{\unicode[Times]{x1D6CA}}\)\(\def\bupkappa{\unicode[Times]{x1D6CB}}\)\(\def\buplambda{\unicode[Times]{x1D6CC}}\)\(\def\bupmu{\unicode[Times]{x1D6CD}}\)\(\def\bupnu{\unicode[Times]{x1D6CE}}\)\(\def\bupxi{\unicode[Times]{x1D6CF}}\)\(\def\bupomicron{\unicode[Times]{x1D6D0}}\)\(\def\buppi{\unicode[Times]{x1D6D1}}\)\(\def\buprho{\unicode[Times]{x1D6D2}}\)\(\def\bupsigma{\unicode[Times]{x1D6D4}}\)\(\def\buptau{\unicode[Times]{x1D6D5}}\)\(\def\bupupsilon{\unicode[Times]{x1D6D6}}\)\(\def\bupphi{\unicode[Times]{x1D6D7}}\)\(\def\bupchi{\unicode[Times]{x1D6D8}}\)\(\def\buppsy{\unicode[Times]{x1D6D9}}\)\(\def\bupomega{\unicode[Times]{x1D6DA}}\)\(\def\bupvartheta{\unicode[Times]{x1D6DD}}\)\(\def\bGamma{\bf{\Gamma}}\)\(\def\bDelta{\bf{\Delta}}\)\(\def\bTheta{\bf{\Theta}}\)\(\def\bLambda{\bf{\Lambda}}\)\(\def\bXi{\bf{\Xi}}\)\(\def\bPi{\bf{\Pi}}\)\(\def\bSigma{\bf{\Sigma}}\)\(\def\bUpsilon{\bf{\Upsilon}}\)\(\def\bPhi{\bf{\Phi}}\)\(\def\bPsi{\bf{\Psi}}\)\(\def\bOmega{\bf{\Omega}}\)\(\def\iGamma{\unicode[Times]{x1D6E4}}\)\(\def\iDelta{\unicode[Times]{x1D6E5}}\)\(\def\iTheta{\unicode[Times]{x1D6E9}}\)\(\def\iLambda{\unicode[Times]{x1D6EC}}\)\(\def\iXi{\unicode[Times]{x1D6EF}}\)\(\def\iPi{\unicode[Times]{x1D6F1}}\)\(\def\iSigma{\unicode[Times]{x1D6F4}}\)\(\def\iUpsilon{\unicode[Times]{x1D6F6}}\)\(\def\iPhi{\unicode[Times]{x1D6F7}}\)\(\def\iPsi{\unicode[Times]{x1D6F9}}\)\(\def\iOmega{\unicode[Times]{x1D6FA}}\)\(\def\biGamma{\unicode[Times]{x1D71E}}\)\(\def\biDelta{\unicode[Times]{x1D71F}}\)\(\def\biTheta{\unicode[Times]{x1D723}}\)\(\def\biLambda{\unicode[Times]{x1D726}}\)\(\def\biXi{\unicode[Times]{x1D729}}\)\(\def\biPi{\unicode[Times]{x1D72B}}\)\(\def\biSigma{\unicode[Times]{x1D72E}}\)\(\def\biUpsilon{\unicode[Times]{x1D730}}\)\(\def\biPhi{\unicode[Times]{x1D731}}\)\(\def\biPsi{\unicode[Times]{x1D733}}\)\(\def\biOmega{\unicode[Times]{x1D734}}\)\begin{equation}\tag{1}{\rm{RT}} = \alpha /\log \left( {C/{C_t}} \right) + {\rm{R}}{{\rm{T}}_{{\rm{Asym}}}}\end{equation}
where RT is the reaction time,
α is the constant determining the steepness of the curve,
C the stimulus contrast (in percent),
Ct the observer's contrast threshold (in percent) and RT
Asym is the reaction time asymptote. This function, which we will refer to as the
Burr fit, goes to infinity at threshold and has a single estimate of contrast dependency (
α), measured in ms, divided by log contrast expressed in threshold units. Because the Burr fit describes data already transformed into units of threshold, it has fewer degrees of freedom than the Piéron fit, and provides a better estimate of the asymptote.
Figure 1 illustrates several potential outcomes of manipulating α and RT
Asym. The top panel shows three curves that are parallel over the entire range. The gray curve represents a normal or nonamblyopic eye. The blue curve represents the amblyopic eye with identical α and RT
Asym—this is the prediction if the saccadic delay of the amblyopic eye is purely a consequence of the reduced visibility of the stimulus. Scaling the visibility by the contrast threshold, simply shifts the AE curve along the abscissa, resulting in superimposition of the curves of the two eyes. The red curve illustrates the amblyopic eye with identical α, but with RT
Asym higher in the AE (i.e., an irreducible delay in the response of the amblyopic eye). The bottom panel shows that increasing or decreasing α, which determines the slope, with no change in RT
Asym would result in the two curves converging at the asymptote. In both situations, manipulating contrast produced equivalent reaction times for high contrast stimuli.
Equating for contrast sensitivity may not produce the same asymptotic values (RT
Asym) for the two eyes of some amblyopic observers, particularly for strabismic amblyopes. In a large-scale study, McKee et al. (
2016) found prolonged saccadic latencies to perifoveal stimuli when fixating with the amblyopic eye, especially in strabismic amblyopes. They argued that deficits in contrast sensitivity could not explain the long average saccadic reaction time of the strabismic amblyopic eyes because the average contrast sensitivity of the strabismic amblyopes was essentially equal to that of the anisometropic amblyopes, but the average saccadic reaction time of the anisometropes was significantly shorter than that of the strabismics. However, this argument is based on indirect evidence. The current study will make detailed measurements of saccadic reaction time as a function of equivalent contrast in both strabismic and anisometropic amblyopes to determine if they differ.
What might account for an irreducible delay (i.e., an increased RT
Asym), in saccadic reaction time in amblyopic observers? McKee et al. (
2016) speculated that “the frequent microsaccades and the accompanying attentional shifts, made while strabismics struggle to maintain fixation with their amblyopic eyes, result in all types of reactions being irreducibly delayed” (p. 12).