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INTRODUCTION |
Vergence eye
movements are critical for good binocular vision, serving to align both
eyes on the same object: the nearer the object of regard, the greater
the required convergence. The visual control of vergence depends
heavily on the slight difference in the positions of the images on the
two retinas, which is referred to as binocular disparity and
effectively defines the vergence error. Although there are a number of
complex visual cues to viewing distance that can influence vergence,
here we shall be concerned solely with disparity, which is the most
potent (for recent review, see Collewijn and Erkelens
1990
). The ability of pure disparity errors to drive vergence
was first demonstrated by Rashbass and Westheimer
(1961)
, who used a Wheatstone stereoscope to present identical
targets independently to the two eyes. Targets with crossed disparity
errors (equivalent to objects nearer than the plane of fixation)
elicited increased convergence, and targets with uncrossed disparity
errors (equivalent to objects farther than the plane of fixation)
elicited decreased convergence, exactly as expected of a negative
feedback system working to achieve and maintain appropriate binocular
alignment. Most studies have been concerned with horizontal
vergence, perhaps in large measure because it is the means by which
binocular alignment is shifted between objects in different depth
planes. However, good binocular vision requires that the two lines of
sight be aligned vertically as well as horizontally, and vertical
disparities have been shown to elicit appropriate vertical vergence,
although the effective range of disparities is much smaller, the
responses have much more sluggish dynamics, show more extensive spatial
integration, and are less sensitive to instruction, than the horizontal
vergence responses associated with horizontal disparities
(Howard et al. 1997
, 2000
; Kertesz
1983
; Stevenson et al. 1997
).
In the present study on humans, we have been concerned solely with the
initiation of vergence by disparity steps applied to large random-dot
stereograms. Previous studies on humans have generally, although not
always, used small targets and reported latencies ranging from 150 to
200 ms (Erkelens and Collewijn 1991
; Houtman et
al. 1977
, 1981
; Jones 1980
;
Mitchell 1970
; Rashbass and Westheimer
1961
; Westheimer and Mitchell 1956
). Using
monkeys, we have recently reported that, when large textured
patterns are used, horizontal disparity steps of suitable magnitude
consistently elicit horizontal vergence eye movements with latencies of
<55 ms (Busettini et al. 1994a
, 1996b
).
These short-latency vergence responses were in the appropriate
direction only when steps were small (<2-3°), and large steps (up
to 12.8°) yielded responses with both isogonal and orthogonal
components that were largely independent of whether the steps were
crossed or uncrossed, horizontal or vertical (so-called, "default"
responses). We argued that the responses to small disparity steps
reflected the operation of a servomechanism that normally functions to
correct residual vergence errors, and the (default) responses to large
steps were due to residual local correlations. We also reported that
small disparity steps applied in the immediate wake of a saccadic eye
movement yielded appropriately directed vergence eye movements with
much higher initial accelerations than did the same steps applied some time later. Further, this transient postsaccadic enhancement seemed to
be dependent, at least in part, on the visual stimulation associated with the prior saccade because similar, although sometimes weaker, enhancement was observed when the disparity steps were applied in the
wake of saccadelike shifts of the textured pattern (so-called, "simulated saccades"). In the present paper on humans, we report similar findings: latencies are short (although 25 ms or so longer than
in monkeys), there are default responses with large steps, and there is
transient enhancement in the wake of real and simulated saccades. The
only significant methodological difference between the present study
and our previous one on monkeys was the visual stimulus: the collage of
arbitrary geometrical shapes used previously was replaced by a
random-dot pattern, permitting a more formal description of the
stimulus. We also report here that initial vergence responses have
orthogonal components that reach an asymptote with steps of a few
degrees and persist (as default responses) with large steps. Further,
we show that the initial vergence responses to small disparity steps
(<2-3°) are relatively insensitive to eightfold changes in the size
of the texture elements (random dots), although responses to steps of
intermediate size (3-6°) are larger with larger elements. In
addition, we report that the vertical vergence responses to vertical
disparity steps have only slightly longer latencies but are appreciably
smaller in magnitude than the horizontal responses to horizontal steps,
although the general form of the disparity tuning curves is very
similar. Finally, we use the same new random-dot stimuli to extend our
earlier report on monkeys and show that the initial vergence responses
of monkeys share most of the features of the human, the differences
between the two species being quantitative rather than qualitative.
Some of these findings on humans have been published in abstract form (Busettini et al. 1994b
).
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METHODS |
The eye movements evoked by brief exposure to disparity steps
applied to large projected random-dot patterns were recorded from seven
adult human subjects. All procedures were approved by the Institutional
Review Committee concerned with the use of human subjects, and all
subjects provided informed consent. Three of the subjects (FM,
RK, and GM) each participated in numerous recording
sessions, and four more (MB, KP, HA, and JG) each
participated in only a few sessions on selected abbreviated paradigms.
All of these subjects had stereoacuities better than 40 s of arc
(Titmus test) and no known oculomotor or visual problems other than
refractive errors that were corrected with spectacles when necessary.
Only two subjects (FM and RK) had prior
experience (as subjects) in eye-movement studies. We also recorded the
vergence responses of three rhesus monkeys using the exact same stimuli
as for the human recordings to permit a quantitative comparison between
the two species. Except for the details of the stimuli (described in
Recording and stimulation procedures), the
methodology used on monkeys was exactly the same as in our earlier
study and will not be described here (Busettini et al.
1996b
).
Recording and stimulation procedures
The presentation of stimuli and the acquisition, display, and
storage of data were controlled by a PC (Hewlett Packard Vectra, 486)
using a Real-time EXperimentation software package (REX) developed by
Hays et al. (1982)
. The horizontal and vertical
positions of both eyes were recorded with an electromagnetic induction
technique (Robinson 1963
) using scleral search coils
embedded in silastin rings (Collewijn et al. 1975
).
Coils were placed in each eye following application of 1-2 drops of
anesthetic (proparacaine HCl), and wearing time ranged up to 73 min for
the three main subjects and 30 min for all others. The AC voltages
induced in the scleral search coils were led off to a phase-locked
amplifier that provided separate DC voltage outputs proportional to the
horizontal and vertical positions of the two eyes with corner
frequencies (
3 dB) at 1 kHz (CNC Engineering). The outputs from the
coils were calibrated at the beginning of each recording session by
having the subject fixate small target lights located at known
eccentricities along the horizontal and vertical meridia. Peak-to-peak
voltage noise levels were equivalent to an eye movement of 1-2 min of arc. Interocular distance was measured to the nearest millimeter.
The subject was seated in a fiberglass chair with his/her head
stabilized by means of a chin support and forehead rest combined with a
head strap and faced a translucent tangent screen (distance, 33.3 cm;
subtense, 85 × 85°) onto which two identical, overlapping patterns were back-projected. Orthogonal polarizing filters in the two
projection paths and matching filters in front of each eye ensured that
each pattern was visible to only one eye: dichoptic stimulation. The
screen was constructed of material specially designed to retain the
polarization (Yamaboshi, Tokyo, Japan). The patterns consisted of black
circular dots with randomly distributed centers on a white background;
overlaps were freely allowed, resulting in irregular clustering, and
the screen image had equal amounts of black and white (50% coverage).
Dot diameters were 2° except for one special study in which this
parameter was varied systematically (when all dots had one of the
following diameters in a given experiment: 0.5, 1.1, 2.2, or 4.4°).
The luminance of the images on the screen was measured with a
photometer (Spectra Pritchard), sampling the screen through the
polarizing filters so as to mimic the subjects' view. With this
arrangement, the luminance measured through the matching polarizing
filters was 0.13 cd/m2 in the light areas of the
patterns and 0.0026 cd/m2 in the dark areas. The
equivalent measures through the nonmatching (orthogonal) polarizing
filters were 0.0011 cd/m2 in the light areas and
0.00060 cd/m2 in the dark areas. Subjects were
unaware of the "ghost" images seen through the orthogonal filters.
Pairs of mirror galvanometers (General Scanning, M3-S with vector
tuning) positioned in each of the two light paths in an X/Y
configuration were used to control the horizontal and vertical
positions (and thereby the horizontal and vertical disparities) of the
two images. These galvanometers were driven by the DAC outputs of the
PC at a rate of 1 kHz with a resolution of 12 bits (optical range,
±50°). Voltage signals separately encoding the horizontal and
vertical positions of both eyes together with the positions of the four
mirror galvanometers were low-pass filtered (Bessel, 6-pole, 180 Hz)
and digitized to a resolution of 16 bits, sampling at 1 kHz. All data
were stored on a hard disk and, after completion of each recording
session, were transferred to a workstation (Silicon Graphics) for
subsequent analysis. The rise time of the mirror galvanometers was <2
ms, and to determine their true dynamics and exact timing they were monitored with a Tektronix digital storage oscilloscope linked to a PC (386).
Paradigms
In a given experiment, the stimulus parameter(s) under study
were varied from trial to trial in a pseudorandom sequence, in part to
discourage prediction/anticipation, and in part to distribute any
effects due to short-term changes in nonvisual factors such as arousal,
attention, fatigue, and so forth. It was usual to collect data over
several sessions until each condition had been repeated a sufficient
number of times to permit good resolution of the responses to be
achieved (through averaging) even when we were exploring the limit of
the responsive range with stimuli of marginal efficacy.
STANDARD PARADIGM.
At the beginning of each trial, the two patterns on the screen were
positioned in register and overlapped exactly (zero disparity) for a
minimum period in excess of 1 s to allow adequate time for the
subject to acquire a convergent state appropriate for the near viewing
(33.3 cm). Disparity steps were initiated in the wake of a saccade into
the center of the screen because preliminary experiments had shown that
the vergence responses were subject to transient postsaccadic
enhancement. This was accomplished by having the subject transfer
fixation between suitably positioned target spots projected onto the
scene through polarizing filters so as to be seen by the right eye only
(to avoid any possible disparity conflict with the background
patterns). The initial target spot appeared 10° right of center
1 s after the beginning of the trial. When the subject's right
eye had been positioned within 1-2° of the spot for a period of time
that was randomly varied (1-1.5 s), the spot was extinguished and a
new one appeared at the center of the screen. This new target was
extinguished as soon as the computer detected a saccadic eye movement,
using as a criterion an eye speed >54°/s. If this saccade achieved a speed in excess of 180°/s and arrived within 4° of the position of
the new target (which was now no longer visible), then it was deemed
appropriate and the disparity step was initiated with a postsaccadic
delay of 50 ms (measured from the time when eye speed fell below
36°/s). We used the convention that rightward and upward movements
were positive, and stimulus disparity was computed by subtracting the
horizontal (or vertical) position of the right image from the
horizontal (or vertical) position of the left image. This meant that
horizontal disparity steps were positive when the left stimulus stepped
to the right and/or the right stimulus stepped to the left
(crossed-disparity steps), and negative when the left stimulus stepped
to the left and/or the right stimulus stepped to the right
(uncrossed-disparity steps); vertical disparity steps were positive
when the left stimulus stepped upward and/or the right stimulus stepped
downward (left-hyper disparity steps), and negative when the left
stimulus stepped downwards and/or the right stimulus stepped upward
(right-hyper disparity steps). The disparity steps had a rise time of
<2 ms and were applied symmetrically to the patterns seen by each of
the two eyes (equal amplitudes, opposite directions), except when
stated otherwise. The amplitude of the disparity steps varied from
trial to trial (absolute values: 0.2, 0.4, 0.8, 1.2, 1.6, 2.0, 2.4, 3.2, 4.0, 4.8, 5.6, 6.4, 9.6, and 12.8°), with crossed, uncrossed,
left-hyper, and right-hyper steps being randomly interleaved. Because
we were interested only in the initial vergence responses, exposure to
the disparity steps lasted only 200 ms, and, if there were no saccades
during this time, then the data were stored on a hard disk; otherwise,
the trial was aborted and subsequently repeated. At this point in the
paradigm, electro-magnetic shutters in the light paths were used to
blank both images for 500 ms, marking the end of the trial; when the
images reappeared, they were once more in register for the start of the
next trial. The projected patterns always filled the entire screen, and
their initial positions were pseudorandomized (9 positions, with
horizontal and/or vertical offsets of 0 or 10°) to reduce the impact
of local anisotropies in the patterns on the mean vergence responses.
Subjects were instructed to make saccades into the center of the
pattern by following the projected target spots and then to refrain
from making any further saccades until the screen was blanked,
signaling the end of the trial. Subjects were given no instructions in
regard to the disparity step stimuli but were asked to restrict their
blinks to the inter-trial period. Direct observation, in addition to
the eye movement profiles (blinks being associated with transient
horizontal convergence and downward version), indicated that subjects
had no problem following this instruction. By applying the disparity
steps in the immediate wake of centering saccades we ensured that
1) the subject was alert during the steps, 2) the
stimulus pattern was always centered on the retina at the onset of the
steps, and 3) the vergence responses were enhanced
(postsaccadic enhancement). Note that all experiments included control
trials in which no steps were applied (saccade-only trials).
DEPENDENCE ON A PRIOR SACCADE OR SIMULATED SACCADE.
Preliminary experiments (Busettini et al. 1994b
) had
revealed that, like ocular following (Gellman et al.
1990
), disparity vergence was subject to transient postsaccadic
enhancement, and we now conducted a series of experiments in which the
postsaccadic delay was varied systematically to characterize the time
course of the enhancement. Stimuli were 1.6° crossed- and
uncrossed-disparity steps, and the postsaccadic delay intervals were
50, 100, 200, 400, and 800 ms (randomly interleaved).
The possibility that the enhancement in the wake of a saccade was due
to the visual reafference produced by the saccade sweeping the image of
the pattern across the retina was investigated by applying the
disparity steps in the wake of a saccadelike shift of the pattern on
the screen. The saccadelike shift (or simulated saccade) was applied
800 ms after the initial centering saccade, pilot studies having
indicated that the postsaccadic enhancement of disparity vergence had
decayed to negligible levels within that period. These shifts were
generated from a look-up table that reproduced the profile of a
representative centering saccade previously recorded from the subject
under study. Because all of the centering saccades were leftward, the
simulated saccades had to be rightward to replicate the retinal events
correctly. Preliminary experiments, however, indicated that subjects
often made anticipatory tracking responses to these simulated saccades, despite attempts to avoid doing so. For this reason we used both rightward and leftward simulated saccades, randomly interleaved, which
largely eliminated the problem. The disparity steps (crossed and
uncrossed, 1.6°) were then applied in the wake of these simulated saccades with delay intervals of 50, 100, 200, 400, and 800 ms (randomly interleaved). Only the data obtained with the rightward saccadelike shifts were used for the comparison with the data obtained
with real (leftward) saccades.
OCULAR FOLLOWING: DEPENDENCE ON A PRIOR SACCADE OR SIMULATED
SACCADE.
To allow a direct comparison of the effects of a prior saccade or
simulated saccade on disparity vergence with those on ocular following
(Gellman et al. 1990
), additional experiments were
undertaken that were identical to those just described except that the
disparity steps were replaced with conjugate steps in which the
patterns seen by both eyes stepped together 0.8° (leftward or
rightward): ocular following stimulus. Note that the previous study of
the dependence of human ocular following on a prior saccade used
velocity step stimuli (Gellman et al. 1990
).
Data collection and analysis
The horizontal and vertical eye position data obtained during
the calibration procedure were each fitted with a third-order polynomial that was then used to linearize the horizontal and vertical
eye position data recorded during the experiment proper. The latter
were then smoothed with a cubic spline of weight
107, selected by means of a cross-validation
procedure (Eubank 1988
), and all subsequent analyses
utilized these splined data. To be consistent with our conventions for
defining the polarity of the disparity stimuli, rightward and upward
eye movements were defined as positive, and vergence position was
computed by subtracting the horizontal (or vertical) position of the
right eye from the horizontal (or vertical) position of the left eye.
This meant that horizontal vergence was positive (denoting increased
convergence) when the left eye moved rightward with respect to the
right eye, or the right eye moved leftward with respect to the left
eye. Likewise, vertical vergence was positive when the left eye moved upward with respect to the right eye, or the right eye moved downward with respect to the left eye (so-called, left sursumvergence or right
deorsumvergence). Horizontal (or vertical) version position, equivalent
to cyclopean gaze position, was computed by averaging the horizontal
(or vertical) positions of the two eyes. Vergence (or version) velocity
was obtained by two-point backward differentiation of the vergence (or
version) position data.
The vergence position and vergence velocity temporal profiles recorded
in all of the trials using a given stimulus condition were displayed
together (synchronized to the disparity step) with an interactive
graphics program that allowed the deletion of the occasional trials
with saccades or blinks.
To best illustrate the temporal structure of the responses, mean
vergence velocity profiles were computed for each stimulus condition.
To eliminate any effects due to postsaccadic vergence drift, the mean
vergence velocity profile recorded during the control saccade-only
trials was subtracted from the mean vergence velocity profiles obtained
for each stimulus condition. All of the vergence velocity traces in the
figures have been so adjusted, and upward deflections of these traces
represent convergent or left sursumvergent velocities.
LATENCY MEASURES.
An objective algorithm was used to estimate the latency of onset of
vergence using data obtained with disparity steps that gave
close-to-maximal responses. Visual inspection of the mean vergence
velocity profiles had indicated that the average latencies were
generally 75-85 ms. Accordingly, the individual vergence velocity
profiles over the time window, 52-118 ms (measured with respect to the
onset of the disparity step), were fitted with a function that assumed
that, up to a time, T, the response profiles were flat
(preresponse period), and then incremented linearly (response period).
The fitting was done using the nonlinear regression method implemented
in BMDP 3R (Dixon et al. 1990
), based on a modified
Gauss-Newton algorithm (Jennrich and Sampson 1968
). For times <T, the function had a constant value
(P1), and for times
T,
the function had a value, at time t, of
P1 + [P2(t
T)]. The value of the baseline
(P1), the starting point of the linear segment (T, which was our estimate of the response latency),
and the slope of the linear segment
(P2), were all free parameters. Starting values were 75 ms (T), 0°/s
(P1), and
0°/s2 (P2).
AMPLITUDE MEASURES.
Estimates of the amplitude of the initial disparity vergence response
were obtained by measuring the change in vergence position over a 67-ms
time interval starting 90 ms after the onset of the disparity step. It
will be seen that the mean latency of onset is about 80 ms so that this
amplitude measure is restricted to the period prior to the closure of
the feedback loop, when eye movements begin to influence the disparity:
initial open-loop response. The measures from all trials were then used
to calculate the mean change in vergence, together with the SD, for
each stimulus condition. Of course, sampling the response at a fixed
time with respect to the onset of the stimulus meant that the sample
would be sensitive to changes in the latency of onset of the response. The latency of vergence showed little dependence on any of the stimulus
parameters examined in the present study, although the initial vergence
responses could become vanishingly small as the limits of the response
range were explored. (At such times, response-locked measures would
default to later components of the response.) To eliminate any effects
due to postsaccadic vergence drift, the mean change in vergence during
the saccade-only (control) trials was subtracted from the mean change
in vergence for each stimulus condition, and these adjusted measures
are the ones given in the text and plotted in the figures (where they
are referred to as "change in vergence position").
OCULAR FOLLOWING.
The analysis of the ocular following data was very similar to that of
the vergence data except that it was carried out on the splined
position measures obtained from the right eye. Quantitative estimates
of the amplitudes of the initial responses were obtained by measuring
the change in eye position during the 67-ms time interval starting 90 ms after the onset of the conjugate position step, and two-point
backward differentiation was used to obtain eye velocity profiles. The
position measures and velocity temporal profiles obtained for all
trials were then averaged for each stimulus condition, and any effects
due to postsaccadic drift were eliminated by subtracting the data
obtained from saccade-only (control) trials. These adjusted
eye-position measures (referred to as "change in eye position") and
eye-velocity temporal profiles are used for all figures and textual references.
Phoria measurement
Dissimilar target images were presented to the two eyes
dichoptically, and the subjects' verbal reports of their relative positions were used to bring the targets into subjective alignment using a staircase procedure, thereby providing an estimate of each
subject's phoria. Subjects viewed the tangent screen in the usual way,
and separate projectors with orthogonal polarizers were used to present
an upright cross (+) continuously to one eye and an oblique cross (×)
transiently to the other. Each cross was black on a white background
and spanned 2.3° with arms 10 min of arc thick. The subject fixated
the upright cross, and, following a warning tone, the oblique cross
appeared for 50 ms. The subject was required to report the horizontal
and vertical position of the oblique cross with respect to the upright
cross, i.e., right/left/aligned, above/below/aligned. If the subject reported misalignment, then, on the next trial, the oblique cross was
repositioned, by a discrete amount, so as to reduce its apparent horizontal and vertical separation from the upright cross. If the
subject reported alignment along one or the other axis, no adjustment
was made along that axis for the next trial. At the start of each block
of trials, the oblique cross could have horizontal and vertical offsets
(relative to the upright cross) of 0, +5, or
5° (varied randomly).
The repositioning steps were initially 2°, and then reduced with each
successive report of alignment or reversal in the apparent
misalignment, to 1°, then to 0.5°, and finally to 0.2°. When the
horizontal and vertical steps had both decremented to 0.2°, the
oblique cross had invariably reached an asymptotic position, and the
block was continued for 20 more trials before starting a new block with
a new misalignment. Each subject completed 9-20 blocks of trials, and
his/her phoria was estimated from the average misalignment of the 2 crosses for the last 20 trials in each block.
 |
RESULTS |
Vergence responses to horizontal disparity steps
Horizontal disparity steps of suitable amplitude applied to large
random-dot patterns elicited consistent horizontal vergence responses
at short latencies. Figure 1 shows sample
horizontal vergence velocity temporal profiles from 1 subject in
response to 174 horizontal crossed-disparity steps of 2° applied 50 ms after 10° leftward centering saccades. Data are shown for all trials except the few (8) contaminated with saccades. Also shown in
Fig. 1 is the mean horizontal vergence velocity profile (±SD), together with the mirror galvanometer feedback signals indicating the
horizontal positions of the images seen by the left and right eyes. The
estimated mean latency (objectively determined, see METHODS) for the data shown in Fig. 1 was 82.5 ms and is
indicated by the arrows. For 2° crossed-disparity steps such as those
used in Fig. 1, the mean latency for seven subjects was 80.9 ± 3.9 (SD) ms. Individual mean latencies (±SD), together with the number of measures contributing to the estimates (when the latency algorithm converged) and the total number of trials from which the data were
drawn (after rejecting trials with saccades or blinks), were as
follows: 82.5 ± 4.8 ms (subject RK, n = 174/174), 86.0 ± 8.7 ms (FM, 140/144), 84.6 ± 11.6 ms (GM, 147/177), 78.0 ± 6.2 ms (JG,
147/148), 77.7 ± 9.2 ms (KP, 165/168), 81.6 ± 7.0 ms (MB, 169/172), and 75.6 ± 9.2 ms
(HA, 31/32). Because our major concern was with the initial
open-loop vergence responses, the temporal profiles in all figures are
discontinued 180 ms after the onset of the disparity steps.

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Fig. 1.
Sample disparity-vergence responses to multiple presentations of a 2°
crossed-disparity step applied 50 ms after 10° leftward centering
saccades (subject RK). Individual vergence velocity
profiles (n = 174), obtained by differentiating
splined vergence position traces and then subtracting the mean vergence
velocity trace obtained in saccade-only control trials (to eliminate
any effects due to postsaccadic drift). Data are collected together
from several recording sessions. Arrow: estimated latency of onset.
Calibration bar applies to ocular vergence traces only. Upward
deflections represent convergent velocities.
|
|
BINOCULAR RESPONSE TO A BINOCULAR STIMULUS.
These short latencies are similar to those reported for the ocular
following elicited by conjugate ramps applied to large textured
patterns (Gellman et al. 1990
). Because visual motion detectors can integrate position steps over time to generate an apparent motion signal (Mikami et al. 1986a
,b
;
Newsome et al. 1986
), it was possible that the
short-latency vergence responses resulted from independent monocular
tracking, in which each eye tracked the apparent motion that it saw,
rather than from the binocular misalignment per se. To test this idea,
we restricted the step to one eye only, leaving the other eye to view a
stationary pattern. The movements of the eye that saw the stationary
pattern were of particular interest; any effects on this eye due to the monocular apparent-motion cues should have been either negligible (if
motion stimuli affected only the eye that saw the motion) or in the
same direction as the motion (if motion stimuli at either eye affected both eyes), whereas any effects on this eye due to the
binocular misalignment (stereo) cues should have been in the direction
opposite to the apparent motion stimulus.
Figure 2 shows the data from one such
experiment in which horizontal crossed-disparity steps of 2.4° were
applied by 1) shifting the pattern seen by the left eye
1.2° rightward and the pattern seen by the right eye 1.2° leftward
(
), 2) shifting the pattern seen by the left eye 2.4°
rightward (· · ·), or 3) shifting the pattern seen
by the right eye 2.4° leftward (- - - - -). There was good
convergence regardless of whether the displacement step was seen by one
or both eyes, although the initial vergence acceleration was slightly
smaller when only one eye saw the step. Further, the eye that saw the
stationary pattern always moved in a direction appropriate
for a stereo-driven response, that is, in the direction opposite to the apparent motion stimulus: when only the
right eye saw a step (leftward), the left eye moved to the right, and when only the left eye saw a step (rightward) then the right eye moved
to the left. It is of interest that the version responses were always
extremely weak (see bottom traces in Fig. 2), despite the
fact that in the asymmetric cases there were changes in the apparent
cyclopean alignment of the stimuli. Essentially identical data were
obtained from two other subjects (FM and GM).

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Fig. 2.
The effect on the horizontal vergence and version velocity responses of
restricting the horizontal disparity step to one eye. Crossed-disparity
steps of 2.4° were applied by 1) shifting the images
seen by the left and right eyes equally ( ), 2)
shifting the image seen by the right eye leftward while the other image
remained stationary (- - - - -), 3) shifting the
image seen by the left eye rightward while the other image remained
stationary (· · ·). All traces are means (n = 183). Zero on the abscissa indicates the time of onset of the
disparity steps. Subject RK.
|
|
DEPENDENCE ON THE MAGNITUDE AND DIRECTION OF THE STEPS.
Vergence responses were often not exactly aligned with the direction of
the disparity steps and could include appreciable orthogonal components
("directional errors"). That is, responses to horizontal steps
included vertical vergence, and responses to vertical steps included
horizontal vergence. Like the isogonal components, these orthogonal
components showed a highly systematic dependency on the amplitude and
direction of the disparity step, but the form of this dependency
differed markedly for the two components and will be described separately.
Isogonal components.
With small horizontal disparity steps (<3°), the very earliest
isogonal (i.e., horizontal) components of the vergence responses were
always in the compensatory direction, i.e., the direction that reduced
the seen disparity, so that crossed steps resulted in increased
convergence and uncrossed steps resulted in decreased convergence. This
is evident from the horizontal vergence velocity profiles shown for
each of three subjects in the middle rows of Fig.
3 (stimuli, crossed steps) and Fig.
4 (stimuli, uncrossed steps): see data
labeled
h. Over the range
approximately ±1°, larger steps resulted in larger responses, as
expected of a disparity-driven, depth-tracking servo system: see traces
in continuous line. Responses began to saturate with larger stimuli,
however, generally reaching a maximum with steps of only 1.6
2.4°.
As steps exceeded these levels, response profiles declined in amplitude
but then gradually assumed a form that persisted with even the largest
steps (12.8°) and was idiosyncratic: see traces in dashed line. (It
will become apparent later, when we discuss the quantitative details,
that all responses of all subjects reached asymptotic levels as steps reached
7°.) Thus some subjects (RK, FM, KP, and
HA) responded to the largest steps with increased
convergence and others (GM and MB) with
decreased convergence, regardless of whether the steps were
crossed or uncrossed. In fact, for a given subject, the vergence
responses to the largest steps were always roughly the same, regardless
of whether the steps were positive or negative, horizontal or vertical.
This is made clear in Fig. 5, which shows the vergence velocity temporal profiles that were elicited when the
12.8° steps were applied in each of the four directions: crossed, uncrossed, left hyper, and right hyper. It follows from this that the
initial responses were anticompensatory with large steps in one or the
other direction: uncrossed steps in some subjects (RK, FM,
KP, and HA) and crossed steps in others (GM
and MB).

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Fig. 3.
The vergence-velocity responses elicited by crossed-disparity steps:
dependence on the amplitude of the step (sample mean traces for 3 subjects). Top row: vertical vergence velocity
( v) over time (ordinate) is plotted
against horizontal vergence velocity
( h) over time (abscissa); dots on
traces at 100, 120, 140, and 160 ms measured from the onset of the
step; tick marks on the axes are at 1°/s intervals.
Middle and bottom rows:
temporal profiles for horizontal vergence velocity
( h) and vertical vergence velocity
( v), respectively; numbers at ends of
traces, disparity steps (in deg); continuous lines, responses (to small
disparity steps) that increment as stimulus amplitude increases; dashed
lines, responses (to larger steps, indicated by numbers in parentheses)
that decrement as stimulus amplitude increases; calibration bars,
2°/s; abscissa, time from onset of the disparity steps; upward
deflections represent convergent ( h)
and left-sursumvergent ( v)
velocities. Column A, subject RK;
column B, subject FM; column C, subject
GM.
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Fig. 4.
The vergence-velocity responses elicited by uncrossed-disparity steps:
dependence on the amplitude of the step (sample mean traces for 3 subjects). Layout and conventions as for Fig. 3.
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Fig. 5.
The vergence-velocity responses elicited by 12.8° disparity steps
(sample mean traces for 3 subjects). Layout and conventions as for Fig.
3.
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It is also evident from Figs. 3 and 4 that the time course of the
individual vergence response profiles could vary considerably, some
showing a gradual climb toward a peak, others peaking rapidly (especially in GM), and yet others showing a reasonably
steady climb except for a brief dip here and there. These declines and dips began at latencies considerably less than twice the reaction time
and so were unrelated to the closing of the visual feedback loop. The
response profiles of subject GM clearly differed from those
of RK and FM in their transiency (as well as in
their polarity with large steps).
The dependence of the initial (open-loop) isogonal responses on the
magnitude and direction of the horizontal disparity steps was examined
quantitatively by measuring the change in horizontal vergence position
over the 67-ms time interval starting 90 ms after the onset of the
disparity step. Disparity tuning curves based on these measures had the
general form of the derivative of a Gaussian and are shown in Fig.
6A (
,
, and
) for
each of the three subjects whose response profiles are shown in Figs. 3-5. In these plots, responses are compensatory when they fall in either the top right quadrant (in which crossed disparity
steps produced increases in convergence) or the bottom
left quadrant (in which uncrossed disparity steps produced
decreases in convergence). For small steps (<1°), the
curves all have roughly linear positive slopes passing through zero:
this is the servo range over which small increases in the input
elicited roughly proportional increases in the output in the
appropriate (compensatory) direction. (We will return to this issue
later.) All curves peak with steps of 1-2° and then decline toward
an asymptote that, for a given subject, is very similar for crossed and
uncrossed steps, so that responses to steps in one direction are
compensatory (in the top right or bottom left
quadrants), whereas the responses to steps in the other direction
are anticompensatory (in the top left or bottom right
quadrants). Figure 6A also includes the horizontal
vergence measures for the responses to the largest vertical
disparity steps (12.8°): see the open symbols plotted at the right
and left extremes labeled "Vertical steps (left hyper)," and
"Vertical steps (right hyper)." Student's t-test failed
to reveal any significant differences at the 0.05 level among the
horizontal responses of a given subject to the four 12.8° stimuli
(crossed, uncrossed, left hyper, and right hyper).

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Fig. 6.
The dependence of vergence responses on the amplitude of the horizontal
disparity steps: tuning curves (3 subjects). Mean change-in-vergence
measures (ordinate) are plotted ( , , and
) against the amplitude of the disparity step
(abscissa). A: horizontal (isogonal) vergence responses;
curves indicate the least-squares best fits obtained using Eq. 2, for which r2 averaged 99.3%.
B: vertical (orthogonal) vergence responses; curves
indicate the least-squares best fits obtained using Eq. 1, for which r2 averaged >90%
despite the poor fit for the crossed-step data of subject
FM (r2 = 59.8%). Open symbols
are the mean change-in-vergence measures obtained with 12.8° vertical
disparity steps (data for right-hyper steps shown at
left, data for left-hyper steps shown at
right). Key identifies the data from each of the 3 subjects. Error bars, 1 SD.
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Orthogonal components.
The vergence responses to horizontal disparity steps also included
orthogonal (i.e., vertical) components that were smaller, slower to
develop, and generally less transient than the isogonal responses: see
Figs. 3 and 4 (
v traces). The
vergence velocity profiles in Figs. 3 and 4 suggest that the latency of
the orthogonal components was generally 20-30 ms longer than that of
the isogonal components. Unfortunately, this could not be confirmed
with our objective algorithm because of the small amplitude of the
orthogonal components, and we used the same measurement interval as for
the isogonal components (90-157 ms). The response measures plotted in
Fig. 6B indicate that these orthogonal responses developed roughly exponentially with increases in step size, generally reaching an asymptote with steps of only a few degrees. These orthogonal components were not simply methodological artifacts due to misalignment of the visual stimuli with respect to the eye coil signals or x/y coil cross talk because 1) for a
given stimulus, the orthogonal responses could be in
opposite directions in different subjects (the sign was
idiosyncratic); 2) for a given subject, the temporal response profiles and disparity tuning curves for the orthogonal component (
v traces in Figs. 3
and 4, curves in Fig. 6B, respectively) were not simply
scaled down versions of those for the isogonal component
(
h traces in Figs. 3 and 4,
curves in Fig. 6A, respectively); 3) for a given
subject, the orthogonal vergence responses for crossed and uncrossed
steps had the same sign: compare the
v traces in Figs. 3 and 4, and
also compare the data for positive and negative disparity steps in Fig.
6B. Like the isogonal (horizontal) vergence responses, for a
given subject, the orthogonal (vertical) vergence responses to the
largest horizontal steps (12.8°) were the same regardless of whether
the steps were crossed, uncrossed, left hyper, or right hyper: see the
traces labeled,
v, in Fig. 5,
and the data plotted at the right and left extremes of Fig. 6B. Student's t-test failed to reveal any
significant differences at the 0.05 level among the vertical vergence
responses to the largest steps in the four directions tested.
It is now clear that the (default) responses to large horizontal (or
vertical) steps were "oblique," with both horizontal and vertical
components that were idiosyncratic: three subjects showed increased
convergence combined with left sursumvergence (RK, FM, and
HA), two showed decreased convergence with right sursumvergence (GM and MB), and one showed
increased convergence with right sursumvergence (KP).
Dynamic directional errors.
Compared with the isogonal components, the orthogonal components were
small and slow to develop, so that directional errors were generally
modest for the very earliest vergence responses to horizontal disparity
steps. The temporal development of the directional errors is best
appreciated from x/y plots of the horizontal and vertical
vergence velocity over time: top row of Figs. 3 and 4. For
steps less than
2°, the x/y vergence velocity traces
start out near the origin and keep fairly close to the horizontal
(isogonal) axis before gradually veering away. (Note that the dots on
the x/y vergence velocity traces occur 100, 120, 140, and
160 ms, after the onset of the step.) As steps exceeded
2°, the
amplitudes of the isogonal components now shifted toward the
asymptotes, allowing the orthogonal components, which were now maximal,
to introduce increasingly large directional errors. Note that the similarity of the responses to large steps in each of the four directions is evident not only from superimposing the temporal profiles
of
h and of
v but also from superimposing
the x/y plots in which these two parameters are plotted
against one another (see Fig. 5, top row).
Vergence responses to vertical disparity steps
Vertical disparity steps of suitable amplitude elicited consistent
vertical vergence responses at short latencies. Using the vertical
vergence velocity data obtained with 1.2° left-hyper steps, mean
latency (±SD) determined by our objective method was 85.1 ± 3.4 ms for four subjects. Individual mean latencies (±SD), together with
the number of measures contributing to the estimates and the total
number of trials from which the data were drawn, were 86.9 ± 12.4 ms (subject RK, n = 159/179), 84.9 ± 12.3 ms (FM, 122/145), 88.2 ± 14.3 ms (GM,
152/177), and 80.5 ± 11.5 ms (HA, 26/31). These
latencies are on average 3 ms longer than those listed earlier for the
isogonal vergence responses (of these same 4 subjects) to horizontal
disparity steps.
BINOCULAR RESPONSE TO A BINOCULAR STIMULUS.
Once again, we tested the possibility that these short-latency
(isogonal) vergence responses might have resulted from independent monocular tracking, rather than from disparity per se, by restricting the steps to one eye only, leaving the other eye to view a stationary pattern. The results of one such experiment on subject RK
are shown in Fig. 7, in which vertical
positive-disparity steps (that is, left-hyper steps) of 1.2° were
applied by 1) shifting the pattern seen by the left eye
0.6° upward and the pattern seen by the right eye 0.6° downward
(
), 2) shifting the pattern seen by the left eye 1.2°
upward (· · ·), or 3) shifting the pattern seen by
the right eye 1.2° downward (- - - - -). The outcome was essentially the same as for horizontal vergence in that monocular steps
were almost as effective as binocular ones in producing (isogonal)
vergence, and the eye that saw the stationary pattern always
moved in a direction appropriate for a stereo-driven response: when
only the right eye saw a step (downward), the left eye moved upward,
and when only the left eye saw a step (upward) then the right eye moved
downward. Essentially identical data were obtained from two other
subjects (FM and GM).

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Fig. 7.
The effect on the vertical vergence and version velocity
responses of restricting the vertical disparity step to 1 eye.
Left-hyper steps of 1.2° were applied by 1) shifting
the images seen by the left and right eyes equally ( ),
2) shifting the image seen by the right eye downward
while the other image remained stationary (- - - - -),
3) shifting the image seen by the left eye upward while
the other image remained stationary (· · ·). All traces are
means (n = 182). Zero on the abscissa indicates the
time of onset of the disparity steps. Subject RK.
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DEPENDENCE ON THE MAGNITUDE AND DIRECTION OF THE STEPS.
The vergence data obtained with vertical steps showed a pattern of
dependence on the amplitude and direction of the steps strongly
resembling that reported above for horizontal steps. The relevant data
for vertical steps are shown in Figs.
8
10, which are organized like Figs. 3-5 to permit a ready comparison with
the data for horizontal steps. It is evident from these figures that
the disparity tuning curves for the data obtained with vertical steps
had the same general form as the curves obtained with horizontal steps:
the curves for the isogonal component resembled the derivative of a
Gaussian, and the curves for the orthogonal component were exponential
(with the same polarity for positive and negative stimuli). However,
there were consistent quantitative differences between the two sets of
data.

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Fig. 8.
The vergence-velocity responses elicited by left-hyper disparity steps:
dependence on the amplitude of the step (sample mean traces for 3 subjects). Top row: vertical vergence velocity
( v) over time (ordinate) plotted
against horizontal vergence velocity
( h) over time (abscissa); dots on
traces at 100, 120, 140, and 160 ms measured from the onset of the
step. Middle and bottom
rows: temporal profiles for horizontal vergence velocity
( h) and vertical vergence velocity
( v), respectively. Other conventions
as for Fig. 3.
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Fig. 9.
The vergence-velocity responses elicited by right-hyper disparity
steps: dependence on the amplitude of the step (sample mean traces for
3 subjects). Layout and conventions as for Fig. 8.
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Fig. 10.
The dependence of vergence responses on the amplitude of the vertical
disparity steps: tuning curves (3 subjects). Mean change-in-vergence
measures (ordinate) are plotted (in filled symbols) against the
amplitude of the disparity step (abscissa). A: vertical
(isogonal) vergence responses; curves indicate the least-squares best
fits obtained using Eq. 2, for which
r2 averaged 99.4%. B:
horizontal (orthogonal) vergence responses; curves indicate the
least-squares best fits obtained using Eq. 1, for which
r2 averaged >90% despite the poor fit for
the left-hyper data of subject FM
(r2 = 70.9%). Open symbols are the
mean change-in-vergence measures obtained with 12.8° horizontal
disparity steps (data for uncrossed steps shown at left, data for
crossed steps shown at right). Key identifies the data
from each of the 3 subjects. Error bars, 1 SD.
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Over the important servo range (that is, the range over which the slope
of the isogonal tuning curve was positive), the isogonal responses to
vertical steps were weaker and peaked at lower disparities than the
isogonal responses to horizontal steps. To illustrate this point, we
have collected together in one plot (Fig.
11) all of the isogonal responses to
both horizontal (filled symbols, continuous line) and vertical steps
(open symbols, dashed or dotted lines) for all three subjects. To
further render comparisons easier, in Fig. 11 we have plotted
absolute response measures on the ordinate, restricted the
abscissa to 2° or less, and used a logarithmic scale. The most
salient features of the data in Fig. 11 are as follows: 1)
the highest curves for the vertical-step data overlap the lowest curves
for the horizontal-step data; 2) over the range of low
disparities examined here, the shapes of the curves undergo a
transition from convex upward (lowest curves) to concave upward (highest curves), one consequence being that, 3) the lower
curves tend to peak earlier (i.e., at lower disparities) than the
higher curves; 4) for stimuli in a given plane (horizontal
or vertical), the curves tended to be steeper for the steps that evoked
responses in the direction of the default: crossed and left hyper for
RK and FM, uncrossed and right hyper for
GM.

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Fig. 11.
Isogonal vergence responses to horizontal and vertical disparity steps.
Ordinate, absolute mean change-in-vergence measures; abscissa,
amplitude of disparity step (logarithmic scale). Filled symbols and
continuous lines, horizontal responses (thick: crossed steps; thin,
uncrossed steps); open symbols and dashed or dotted lines, vertical
responses (dotted: left-hyper steps; dashed, right-hyper steps).
Circles, subject RK; squares, subject FM;
diamonds, subject GM. Error bars, 1 SD.
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The orthogonal (horizontal) responses to vertical steps were much
stronger than the orthogonal (vertical) responses to horizontal steps,
with latencies this time that were comparable with those of the
isogonal components. One consequence was that vergence directional
errors could be much greater with vertical disparity steps. In fact,
for vertical steps greater than
1.5°, the orthogonal responses
were actually greater than the isogonal responses. For vertical steps
>5°, default responses predominated, and both the horizontal and the
vertical vergence response measures were independent of whether the
steps were positive or negative, horizontal or vertical (see also Fig.
5). The large directional errors with vertical disparity steps are most
easily appreciated from the x/y plots of the horizontal and
vertical vergence velocity over time (Figs. 8 and 9, top
rows). These x/y vergence velocity traces all start out
near the origin, but only the traces resulting from very small steps
(0.4°) consistently kept fairly close to the vertical (isogonal)
axis; most responses to vertical steps >0.4° veered off in a
horizontal direction almost immediately, although occasional ones kept
fairly close to the vertical axis at first. Of course, the
x/y trajectories obtained with the largest vertical steps
are essentially the same as those obtained with the largest horizontal
steps (Fig. 5).
Quantitative comparison of the disparity tuning curves for
horizontal and vertical steps
We fitted mathematical functions to the change-in-vergence
measures for both the isogonal and orthogonal components of the vergence responses, and these functions are plotted as smooth curves in
Figs. 6 and 10. The function parameters provide a succinct summary of
the data and permit quantitative comparisons of the responses of the
different subjects and, for a given subject, of the responses to
horizontal versus vertical steps. Later, the function parameters will
be used to compare the data for different stimulus patterns (large-dot
patterns vs. small-dot patterns), as well as for human versus monkey.
The following exponential function (Eq. 1) was fitted to the
mean orthogonal responses of each subject
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(1)
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where d is the disparity error created by the step,
Ao is the asymptotic level of the
exponential, C is an offset, and
Bo is the space constant. It is clear
from the curves in Figs. 6B and 10B that
Eq. 1 generally provided a good fit to the orthogonal data
with the exception of the responses of FM to crossed steps, which were unusual in showing a slight overshoot before settling at the
asymptotic level. The best-fit parameters for all three subjects are
listed in Table 1, which also includes an
estimate of the goodness of fit, r2,
based on the percentage of the disparity-induced variation in vergence
explained by the the sum of squares due to regression, with
compensation for the mean: mean corrected
r2 (Cumming and Parker
1999
; Engelman 1999
). Most of the fits were clearly very good, r2 averaging more
than 90%, despite the poor fit for the data of FM. Table 1
indicates that the space constant, Bo,
showed considerable inter-subject variation (range: 0.39-3.35°) and,
for a given subject, could show substantial directional asymmetries for
crossed versus uncrossed and right-hyper versus left-hyper stimuli.
Excluding the crossed-step data for FM (because the fit was
poor), Bo was always larger for the
vertical vergence responses than for the horizontal, on average, by
130% (1.93 vs. 0.84°). It is also evident from Table 1 that
Ao and C were generally
negatively correlated. For example, on average, C is
21%
of Ao (correlation coefficient 0.96)
for the horizontal responses to vertical steps and
11% of
Ao (0.74) for the vertical responses
to horizontal steps. This means that the exponential fit generally
showed a reversal in sign for the smallest disparities. Often, this
reversal occurred below 0.2° (the smallest step that we used), and no
reversal was evident in the recorded data. In such cases, it is
possible that the y-offset in Eq. 1
(C) actually compensates for a small x-offset in
the data, such as might occur, for example, if there were a small dead
zone within which disparity is ineffective. This raises the possibility
that an x-offset might be more appropriate in Eq. 1 than the y-offset that we have used. However, in
other cases, the recorded responses to the smallest steps showed a
clear reversal in sign: for examples, see the data of GM
(uncrossed) and RK (crossed) in Fig. 6B. In such
cases, where the fitted exponential function must show sign reversal, a
separate y-offset term is critical.
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Table 1.
Best-fit parameters when Eq. 1 was fitted to the mean orthogonal
responses obtained with horizontal and vertical disparity steps
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The following function (Eq. 2) was fitted to the isogonal
responses
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(2)
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The first term in Eq. 2 accounts for the nonzero
asymptote, and, because this was independent of the direction of the
step, we assumed that it shared the exponential development of the
response to the orthogonal stimulus. Accordingly, the first term is an exponential function with an asymptotic level,
Ai, and a space constant,
Bi. The latter was fixed at the value
of the space constant that was obtained when Eq. 1 was
fitted to the pooled orthogonal data: for the horizontal isogonal fits,
we pooled the horizontal responses to right-hyper and left-hyper steps,
and for the vertical isogonal fits, we pooled the vertical responses to
crossed and uncrossed steps. The second term in Eq. 2 is a
Gabor function, in which
is the Gaussian width, f and
are the spatial frequency and phase of the cosine term, and
G is a gain factor. Because the data were usually not
symmetrical about zero, we incorporated a parameter, D, to
allow the peak of the Gaussian to shift, and, because the rate at which
responses incremented (with small disparities) was sometimes
appreciably greater than the rate at which they decremented (with
higher disparities), we scaled the disparity, d, by a
compression factor, F, which could have values ranging downward from unity. A value for F of unity indicates no
asymmetry, and lower values indicate that the rising phase of the
tuning curve was steeper than the falling phase (increased skew). It is
clear from the curves in Figs. 6A and 10A that
Eq. 2 provided a good fit to the isogonal data for all three
subjects, and the best-fit parameters for these curves are listed in
Table 2, together with an estimate of the
goodness of fit (again, r2), and
P, the peak-to-peak amplitude of the best-fit functions. The
mean r2 indicates that, on average,
the fit accounted for 99.4% of the disparity-induced variation in
vergence. Table 2 indicates that the amplitude (P), Gaussian
width (
), and compression factor (F) were consistently
greater for the responses to horizontal steps than for the responses to
vertical steps: on average, P by 241%,
by 43%, and
F by 31%. The spatial frequency (f) and phase
(
) were quite variable (range for f, 0.028-0.164
cycles/deg; range for
, 263.5-278.6°), but neither showed
consistent differences between horizontal and vertical. The differences
in F indicate that the asymmetry in the rising and falling
phases of the tuning curves was greater for the vertical data.
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Table 2.
Best-fit parameters when Eq. 2 was fitted to the mean isogonal
responses obtained with horizontal and vertical disparity steps
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Dependence on the size of the elements in the visual patterns
All of the above vergence responses were obtained with random-dot
patterns in which the individual dots each had a diameter of 2°, and
we now report the effects of changing the diameter of the dots up to
eightfold while maintaining the same overall coverage (50%). These
experiments were carried out on monkeys as well as humans to allow a
comparison of the two species. We know from the study of
Busettini et al. (1996b)
that the disparity tuning
curves for the isogonal horizontal responses of the monkey have the
same general form as the curves of humans, resembling the derivative of
a Gaussian with a nonzero asymptote. However, that earlier study did
not document the orthogonal responses or the responses to vertical
disparity steps and employed visual stimuli (irregular patterns) that
cannot be formally described, so that direct quantitative comparisons
with the present human data were not possible. We therefore undertook a
comparison study on three monkeys and three humans using the same
stimulus patterns.
The vergence responses of humans and monkeys showed a similar
dependence on the size of the individual dots in the disparity stimuli,
and Fig. 12 shows some representative
data from one human subject. The most obvious effect on the isogonal
disparity tuning curves was on the falling phase: for both horizontal
and vertical steps, the transition from the peak to the asymptote
tended to be more gradual as the dot size increased. The peak responses tended to occur at slightly higher disparities with the larger dots,
but effects on the initial rapid rise to the peak were generally small
and effects on the asymptote were somewhat variable. The latter was
also evident in the orthogonal disparity tuning curves, and, in Fig.
12, B and D, this effect partially obscures a
tendency for the space constant to increase with dot size.

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Fig. 12.
The dependence of vergence responses on the size of the individual
random dots: tuning curves for a sample subject (RK).
Mean change-in-vergence measures (ordinate) are plotted against the
amplitude of the disparity step (abscissa). Top:
isogonal vergence responses to horizontal (A) and
vertical (C) disparity steps; curves indicate the
least-squares best fits obtained using Eq. 2, for
which r2 averaged 99.5%.
Bottom: orthogonal vergence responses to horizontal
(B) and vertical (D) disparity steps;
curves indicate the least-squares best fits obtained using Eq. 1, for which r2 averaged 97.3 ± 1.7% (mean ± SD). Key identifies the diameters of the dots.
Error bars, 1 SD.
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Such quantitative effects were assessed by fitting Eq. 1 to
the orthogonal data and Eq. 2 to the isogonal data, and the
best-fit parameters are summarized in Tables
3 and 4,
respectively, which show average data for the three humans and the
three monkeys. The fits for the isogonal data were all extremely good
for the human data (r2, 99.4 ± 0.2% mean ± SD) and only slightly less so for the monkey data
(r2, 97.9 ± 1.5% mean ± SD).1 The fits for
some of the orthogonal data were poor, especially for the monkey
vertical responses (to horizontal steps), mostly because the latter
were vanishingly small and sometimes showed a very slight transient
overshoot similar to that of subject FM seen in Figs.
6B and 10B. (Note that this was of little
consequence for the fits of Eq. 2 to the monkey's vertical
isogonal responses because the latter had correspondingly small
asymptotes: see Ai in Table 4.) If the
monkey vertical response data are excluded, however,
r2 for the orthogonal fits exceeded
0.8 in 32/36 data sets; again, the (4) data sets that were fitted
poorly were of very small amplitude and showed slight overshoot.
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Table 3.
Best-fit parameters when Eq. 1 was fitted to the mean orthogonal
responses obtained with horizontal and vertical disparity steps using
patterns with dots of various sizes
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Table 4.
Best-fit parameters when Eq. 2 was fitted to the mean isogonal
responses obtained with horizontal and vertical disparity steps using
patterns with dots of various sizes
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Regarding the best-fit isogonal parameters, the only one that
consistently showed a systematic dependence on dot size was the
Gaussian width (
), which increased with increasing dot size. For
example, the value of
with the largest dots exceeded that with the
smaller ones (on average) by 47% in humans (horizontal, 41%;
vertical, 53%) and 152% in monkeys (133%, 172%). The compression factor, F, and the spatial frequency, f,
sometimes showed a slight tendency to decrease with increasing dot
size, and this, together with the changes in
, largely accounted for
the more gradual transition from the peak to the asymptote as the dot
size increased. The only orthogonal par