The prism-induced vergence paradigms were performed on all six
subjects. First, control data were collected with both eyes viewing
without prisms (
Fig. 1A ). Then the same paradigm was performed with both eyes viewing but with
a horizontal Fresnel prism placed base out (30 cm/m = ∼17.1°)
in front of the right eye
(Fig. 1B) . The left eye wore no prism.
Subjects were asked to fuse the images of the LED. The vergence angle
was calculated and displayed. Next, there was a second control
experiment with both eyes viewing without prisms
(BE
2 paradigm). Then the prism was positioned in
front of the left eye (BE
LP paradigm). Finally,
another set of data with both eyes viewing without prisms was collected
(BE
3 paradigm). To summarize, the disparity
paradigm order was as follows: BE
1 (both eyes
viewing, no prisms, first control), BE
RP (both
eyes viewing, right eye wearing prism), BE
2 (both
eyes viewing, no prisms, second control), BE
LP (both eyes viewing, left eye wearing prism), and
BE
3 (both eyes viewing, no prisms, third
control).
It should be emphasized that in the BERP and
BELP paradigms, the eye that is looking through
the prism is converging to fuse the prism-induced disparity. The eye
that is not looking through the prism does not change its horizontal or
vertical position within the orbit, relative to the target positions,
even though the other eye is converging.
Because of the depth of their globes in the orbits and the relative
location of their nasal bridges, four subjects could not reliably see
the targets with the eye with the prism, when the targets were located
in some of the nasal positions, which corresponded to the most temporal
positions of the nonprism eye. Because fusion was lost in these
positions, they were not used for analysis of either eye. Accordingly,
analysis of the nonprism eye was based on the six nasal positions, and
analysis of the prism eye on the six temporal-most positions, in which
fusion was maintained by all subjects at all times. However, because of
the change in orbital position of the prism eye during convergence,
temporal positions with the prism in place were approximately 15°
more nasal than the temporal positions of the control paradigm.
Therefore, calculations of Listing’s plane in the control paradigm
were based on the six nasal positions for all eyes.
In the binocular and monocular control paradigms, in which all subjects
could see all nine LEDs, we determined the effects of choosing a subset
of points (relatively nasal or temporal) on the calculated orientation
of Listing’s plane. There was a small but consistent apparent“
temporal rotation” (mean 2.4° ± 0.6° RE- and LE-paradigm,
mean 2.0° ± 0.8° in the BE
1-paradigm) of the
horizontal primary position, when the six nasal-most LEDs were selected
instead of all nine LEDs. Selecting the six temporal-most LEDs for the
calculation (instead of all nine LEDs) led to an apparent “nasal
rotation” of the horizontal primary position of a similar magnitude
(mean 1.7° ± 0.9° in the RE- and LE-paradigms, mean 1.9° ±
0.5° in the BE
1-paradigm). Thus, there is a
small but consistent influence on the calculation of horizontal primary
position, which depends on the LEDs selected; using relatively nasal
eye positions leads to more temporal rotation of the primary position,
and vice versa. Our data, as has been reported
previously,
9 indicate that Listing’s “plane” is not a
true plane but is curved and that the departures from a planar surface
may be greater for more eccentric eye positions. This feature
emphasizes the importance of matching, as closely as possible, the
orbital positions used to calculate Listing’s planes in the
corresponding control and vergence paradigms.