| Literature DB >> 35153699 |
Abstract
The pupils of the eyes reflexively constrict in light and dilate in dark to optimize retinal illumination. Non-visual cognitive factors, like attention, arousal, decision-making, etc., also influence pupillary light response (PLR). During passive viewing, the eccentricity of a stimulus modulates the pupillary aperture size driven by spatially weighted corneal flux density (CFD), which is the product of luminance and the area of the stimulus. Whether the scope of attention also influences PLR remains unclear. In this study, we contrasted the pupil dynamics between diffused and focused attentional conditions during decision-making, while the global CFD remained the same in the two conditions. A population of 20 healthy humans participated in a pair of forced choice tasks. They distributed attention to the peripheral decision cue in one task, and concentrated at the center in the other to select the target from four alternatives for gaze orientation. The location of this cue did not influence participants' reaction time (RT). However, the magnitude of constriction was significantly less in the task that warranted attention to be deployed at the center than on the periphery. We observed similar pupil dynamics when participants either elicited or canceled a saccadic eye movement, which ruled out pre-saccadic obligatory attentional orientation contributing to PLR. We further addressed how the location of attentional deployment might have influenced PLR. We simulated a biomechanical model of PLR with visual stimulation of different strengths as inputs corresponding to the two attentional conditions. In this homeomorphic model, the computational characteristic of each element was derived from the physiological and/or mechanical properties of the corresponding biological element. The simulation of this model successfully mimicked the observed data. In contrast to common belief that the global ambient luminosity drives pupillary response, the results of our study suggest that the effective CFD (eCFD) determined via the luminance multiplied by the size of the stimulus at the location of deployed attention in the visual space is critical for the magnitude of pupillary constriction.Entities:
Keywords: countermanding; decision-making; eye movement; human; model simulation; pupillometry
Year: 2022 PMID: 35153699 PMCID: PMC8826249 DOI: 10.3389/fnhum.2021.755383
Source DB: PubMed Journal: Front Hum Neurosci ISSN: 1662-5161 Impact factor: 3.169
FIGURE 1Schematic of temporal sequence of events in novel choice-countermanding (CC) tasks. Following the fixation duration, four cyan-magenta checker boxes appeared peripherally along with a small gray broken circle around the fixation spot. After 500 ms, the fixation spot and the broken circle disappeared, and all four peripheral checker boxes were masked by gray squares simultaneously (go-signal). (A) In the central cueing task, in the majority (60%) of trials (no-stop trials), participants were instructed to select the largest circumferential gap of broken circle (magnified in the inset) and to orient the gaze to one of the squares in the direction of the largest gap. (D) In the peripheral cueing task, in 60% of total trials (no-stop trials), participants were asked to select the checker box with the largest proportion of magenta color (magnified in the inset) and to orient their gaze to the location of the selected target following the disappearance of the fixation spot within a predetermined fixed period. Eye traces from representative saccades in no-stop trials are shown by white dots. (E) In the remaining trials (40%) of each task (stop trials), the fixation spot reappeared after a random delay [i.e., stop-signal delay (SSD)] to instruct participants to withhold their eye movements. No-stop and stop trials were randomly interleaved in each task. Gaze position and the pupillary response from representative trials are demonstrated in panels (B,C), respectively.
Parameters used for the simulation of a biomechanical model of pupillary light response (PLR).
| Model parameter | Value | Description | Referring Supplementary Equations |
| α | 3.66 | Off slope of isometric twitch of sphincter | 20 |
| α | 0.48 | Off slope of isometric twitch of dilator | 14 |
| β | 8.12 | On slope of isometric twitch of sphincter | 20 |
| β | 1.44 | On slope of isometric twitch of dilator | 14 |
|
| 0.14 | Visual delay to parasympathetic PLR pathway | 20 |
|
| 0.69 | Visual delay to sympathetic PLR pathway | 14 |
|
| 0.09 | Passive tension coefficient for sphincter | 15 |
|
| 0.72 | Passive tension coefficient for dilator | 9 |
|
| 0.36 | Passive tension coefficient for sphincter | 15 |
|
| 0.75 | Passive tension coefficient for dilator | 9 |
|
| 85.33 | Elasticity coefficient for sphincter | 17 |
|
| 15.17 | Elasticity coefficient for dilator | 11 |
|
| 1.49 | Length of sphincter at rest | 15 |
|
| 1.07 | Length of dilator at rest | 9 |
|
| 3.75 | Length of sphincter at which | 17 |
|
| 4.58 | Length of sphincter at which | 11 |
|
| 2.70 | Initial radius of pupil | 1, 4, 9, 11, |
|
| 5.00 | Maximum radius of pupil | 9, 11 |
|
| 950.93 | Maximum active tension in sphincter | 17 |
|
| 119.41 | Maximum active tension in dilator | 11 |
|
| 13.18 | Viscous coefficients at the phase of stretch | 2, 22 |
|
| 69.10 | Viscous coefficients at the phase of release | 2, 22 |
|
| 0.05 | Static component of parasympathetic activity | 24, 25 |
|
| 0.15 | Static component of sympathetic activity | 23, 25 |
|
| 0.63 | Dynamic component of parasympathetic autonomic activity | 24, 26 |
|
| −0.54 | Dynamic component of sympathetic autonomic activity | 23, 26 |
| λ | 1 | Gain | 26 |
|
| CCP: 30 | Visual input (effective corneal flux density) | 7, 14, 20 |
FIGURE 2Population average of performance and reaction time (RT). (A) The average percentage of rewarded trials (i.e., correct no-stop and canceled stop trials) in peripheral (light gray) and central (dark gray) cueing for no-stop and stop conditions. (B) The average saccadic RT in correct no-stop and non-canceled stop trials in the peripheral (light gray) and central (dark gray) cueing task. (C) The average percentage of error/failure in stopping a saccade gradually increased as SSD increased in the peripheral (light gray) and central (dark gray) cueing task. Error bars indicate SE of corresponding mean.
FIGURE 3Influence of a decision cue on the pupil dynamics relative to the cue onset (A–C) and saccade onset (D,E) in the peripheral (solid) and central (dashed) cueing task. The smoothened, normalized, and baseline-corrected pupil size averaged across trials pooled from the population of 20 participants in panels (A,D) the correct no-stop, (B,E) non-canceled stop, and (C) correct stop condition. The gray patches are overlaid on the traces to show corresponding SE of the mean pupil size. (F) The population average of tonic pre-stimulus pupil size in the eye tracker’s unit during the fixation period in correct no-stop, non-canceled stop, and correct stop trials in the peripheral (light gray) and central (dark gray) cueing task.
FIGURE 4(A) A schematic of Usui and Hirata (1995) model of pupillary muscle plants. The model determined the non-linear interactions between the dynamic properties of sphincter and dilator muscle components as they received inputs from the parasympathetic and sympathetic division of the autonomic nervous system (ANS), respectively. Refer the Supplementary Material and Table 1 for details of parameters. (B) The influence of stimulus strength on simulated pupil dynamics from stimulus onset. Simulation of a biomechanical model of pupillary aperture (Usui and Hirata, 1995) with the two different stimulus strengths yielded stimulus amplitudes of 30 (solid) and 20 (dashed). Simulated pupil dynamics mimic the behavioral data (see Figures 3A–C). The gray patches are overlaid on the traces to show corresponding SE of the mean pupil size.