| Volume 2, Number 9, Article 6, Pages 645-652 |
doi:10.1167/2.9.6 |
http://journalofvision.org/2/9/6/ |
ISSN 1534-7362 |
Influence of chromaticity on vernier and stereo acuity
John Krauskopf |
Center for Neural Science,
New York University, New York, NY, USA |
|
Jason D. Forte |
Center for Neural Science,
New York University, New York, NY, USA |
|
Abstract
Vernier offset thresholds for targets modulated in luminance or isoluminantly along the L-M axis were confirmed to be equal for targets whose contrasts were equal multiples of those required for detection. On the other hand, stereoscopic depth thresholds were elevated by a factor of 10 or more for isoluminantly modulated targets. Thresholds for vernier targets are 2 or 3 times larger with a gap of 20 arcmin than for a gap of 1 arcmin for both isoluminant and luminance targets. On the other hand, stereo thresholds decrease by a factor of 2 to 3 for both classes of target over the same range. We consider our results in the light of recent electrophysiological and psychophysical evidence and conclude that our results are consistent with the notion that stereo thresholds are mediated by a single class of mechanism for targets modulated in luminance or isoluminantly. We test and reject the hypothesis that stereopsis is subserved by independent chromatic and luminance mechanisms.
History
Received February 4, 2002; published December 18, 2002
Citation
Krauskopf, J. & Forte, J. D. (2002). Influence of chromaticity on vernier and stereo acuity.
Journal of Vision, 2(9):6, 645-652,
http://journalofvision.org/2/9/6/,
doi:10.1167/2.9.6.
Keywords
color vision, binocular vision, stereopsis, vernier acuity
for related articles by these authors
for papers that cite this paper |
Here we compare the efficacy of chromatic and luminance
stimuli for vernier and stereoscopic judgments. Morgan and Aiba (1985) reported that vernier
thresholds were higher for equiluminant stimuli than with stimuli containing
luminance cues. The thresholds for the two stimuli may not have been comparable
because they were equated using detection thresholds based on stimulus width
rather than contrast. This resulted in chromatic and luminance stimuli with
different spatial parameters. The more appropriate measure, target contrast, was
not used, presumably for technical reasons. On the other hand, Krauskopf and Farell (1991) found that
vernier thresholds were equal for isoluminant and luminance targets if they were
equated in spatial frequency content and in contrast with respect to detection
thresholds. This suggests that chromatic and luminance information are equally
effective for vernier judgments. Similar results might have been expected for
stereo judgments because the information needed to deduce depth from a simple
stereo target is present in the stimulus offsets in the two eyes.
The evidence for the efficacy of chromatic contrast in
stereopsis is mixed. On the one hand, it has been held that chromatic signals
make no contribution to stereo judgments ( Livingstone & Hubel, 1987), whereas Scharff and Geisler (1992) concluded that, for
at least two of their three observers, color and luminance information were used
with equal neural efficiency in performing a stereo task. In a series of
studies, Kingdom and Simmons have expressed the view that contrast thresholds
for stereopsis were subserved by independent chromatic and luminance
stereoscopic mechanisms ( Kingdom &
Simmons, 1996; Kingdom, Simmons, &
Rainville, 1999) with the color stereoscopic mechanism being much weaker
than the luminance mechanism.
There are several models of how the visual system
processes spatial information that could explain differences between vernier and
stereo. One is the possibility that color is used only for a subset of spatial
tasks. Another possibility is that color is processed separately from luminance
by stereopsis mechanisms, but processed together by a single vernier mechanism.
A third possibility is that chromatic inputs are treated the same as luminance
ones, but transformations prior to those of interest handicap chromatic inputs
for stereo but not for vernier.
Here we report measurements of vernier and stereo
thresholds for stimuli of equal contrast relative to detection thresholds but
varying in elevation out of the isoluminant plane. We use a method that allows
us to attribute differences between vernier and stereo to mechanisms beyond
those responsible for initial encoding. We confirm that stereopsis is much
poorer for chromatic inputs, and that vernier is equally sensitive to chromatic
and luminance inputs.
Krauskopf and Li
(1999) found that thresholds for motion were independent of contrast for
luminance targets but strongly dependent on contrast for chromatic targets, a
convincing sign that different mechanisms process chromatic and luminance
stimuli.
To look for signs of difference in the functional
effects of chromaticity and luminance on stereo, we investigated how thresholds
were affected by contrast and spatial separation of targets. For example, Berry (1948) reported that vernier thresholds were
found to increase with increased target separation whereas stereo thresholds
remained constant. We revisited this issue using modern methods to further
establish the effect of spatial factors. We confirm Berry’s finding that
vernier thresholds increase with target separation (see also Sullivan, Oatley, & Sutherland, 1972). In
contrast with Berry, we find clear evidence that stereo acuity improves with
target separation for small separations (see also Westheimer & McKee, 1979). That the
pattern of thresholds for chromatic stereopsis mirrors those for luminance
suggests that the chromatic information is being used in the same way as
luminance information. This is evidence that chromatic inputs are functionally
equivalent (although weaker) to luminance ones for stereopsis.
We revisited the question of whether there are
independent chromatic and luminance stereopsis mechanisms ( Simmons & Kingdom, 1997). We measured
stereoscopic disparity thresholds for targets modulated solely in luminance and
for the same targets with an additional chromatic component. This sort of
mixture experiment is often hard to interpret because differences in the
predictions of alternative theories, such as energy addition and probability
summation, are small, but in this case, the predicted outcome is simple. If
there were independent stereo detection systems, threshold offsets for mixtures
should be equal to or less than those for pure luminance stimulus. In fact,
stereo thresholds were larger when an L-M component was added to a
luminance-defined target, leading to the conclusion that there are not
independent chromatic and luminance mechanisms for interpreting disparity.
The targets are illustrated in Figure 1. In the vernier task, the observer has
to report whether the bottom lines are offset to the right or left of the top
lines. In the stereo experiments, the displacement actually had two components.
One component provided the information about depth, the bottom target elements
being displaced nasally or temporally relative to the top target element. The
displacement was shared by the top and bottom elements so that one element moved
forward and the other backward with respect to the fixation point, which was
present between stimulus trials. In order to prevent the observer from making
the judgment solely on the basis of a monocular vernier basis, an additional
random displacement of both lower target elements was introduced. In all
experiments, stimulus duration was 1 s.
The stimuli were specified within the framework of the
DKL color space ( Derrington, Krauskopf, &
Lennie, 1984; Krauskopf, Williams,
& Heeley, 1982). In this space, in one of the chromatic axes in the
isoluminant plane (L-M), the S cone input is held constant whereas the L and M
cone inputs covary to keep luminance constant. The
other chromatic axis is one in which only the S
cone input varies. The third dimension is the luminance axis along which
variations of L, M, and S cone inputs vary
proportionally. Figure 1. Simulation of
stimuli used in vernier and stereo experiments. Stimuli were viewed
haploscopically, the left pair of gratings viewed by the left eye and the right
pair by the right eye. In the illustration, the lower targets are both shifted
to the right with respect to the top targets with a greater offset for the right
target than the left.
It is useful to specify the stimuli in these
experiments in polar coordinates. Hue is measured in degrees of azimuth around
the color circle starting from zero at the L end of the L-M axis. In the
experiments reported here, the stimuli were confined to the plane spanned by the
L-M and luminance axes of the DKL color space ( Derrington et al., 1984; Krauskopf et al., 1982). The relative
luminance component of the targets is expressed in terms of the angular
elevation of the direction of the modulation out of the isoluminant plane.
Because we would like to know about performance with
precisely isoluminant stimuli, and because individual differences are found, we
measured the elevation of each observer’s isoluminant plane with respect
to the nominal isoluminant plane defined by the CIE luminosity function ( Krauskopf, Wu, & Farell, 1996).
The stimuli were generated on a Sony 500PS monitor.
Each pixel subtended 1 arcmin, but, by subsampling the intensity values from an
extended sine table, the resolution of the stereo and vernier offsets was 2 arcs
( Krauskopf & Farell, 1991). The
frame buffer device was capable of producing 256 colors at 14-bit resolution for
each of the three guns. Control of intensity was linearized by the use of lookup
tables derived from calibration measurements. Throughout the experiments, the
mean chromaticity of the stimuli was that of equal-energy white; the mean
luminance was 50 cd/m -2. The stimuli, viewed through an haploscope,
were variants of those illustrated in Figure
1. The upper and lower patterned rectangles were each 120 min high and 60
min wide. The typical pattern was a 2 cycle/deg odd symmetric Gabor with a sigma
of 20 min.
The authors, the primary observers, had normal color
vision and were experienced in psychophysics. The research followed the tenets
of the World Medical Association Declaration of Helsinki and was approved by the
New York University Committee on Activities Involving Human Subjects.
Vernier thresholds are equal for isoluminant and
luminance varying targets equated for contrast relative to detection thresholds
( Krauskopf & Farell, 1991). In
order to test whether this is true for stereo thresholds, we first measured
contrast thresholds for detection of stimuli modulated in luminance and along
the L-M axis in the nominal isoluminant plane using a yes-no staircase
procedure. These measurements were used to produce a personalized set of DKL
coordinates for each observer ( Derrington et
al., 1984). The thresholds defined unit vectors along the cardinal
axes.
Furthermore, in order to test theoretical expectations,
we wanted to get the best estimate of each observer's isoluminant plane. Flicker
photometry is the standard method for defining luminance, and the isoluminant
plane of the DKL and other spaces are based on this definition. There is
evidence of individual and methodological difference in judgments of
isoluminance ( Livingstone & Hubel,
1987; Krauskopf et al., 1996). We
used a method of paired comparisons to estimate the elevation of the
observers’ isoluminant plane relative to the nominal plane ( Krauskopf et al., 1996). In this case, we
exploited the observation that stimuli modulated sinusoidally in space look like
square waves when modulated isoluminantly. Observers were asked to choose which
of a sequentially presented pair of stimuli varying in elevation about the L-M
axis of the nominal isoluminant plane appeared more “square.” Five
stimuli whose elevation straddled the isoluminant plane were presented 5 times
in all 20 pairwise combinations.
The frequency with which each stimulus was chosen
against all the others was plotted as a function of elevation ( Figure 2).
Such plots are well fit with a Gaussian. The value of
the abscissa at the peak of the Gaussian was taken as an estimate of the
elevation of the observer’s isoluminant plane. The value of the offset of
this observer's isoluminant plane, -25.6 deg, may seem surprisingly large but it
is typical. It is important to note that this elevation is expressed in observer
coordinates rather than machine units. In machine coordinates, the elevation
would be on the order of -5 deg. All of our observers required a negative
rotation out of the nominal isoluminant plane to obtain subjective
isoluminance.
There was no theoretical basis for choosing the
squareness criterion but it did have the advantage that the stimuli used to
establish isoluminance had the same structure as those used in the main
experiments. In this case, it was a felicitous one. The peak thresholds in Figure 4 occur at the elevations determined by
the method illustrated in Figure 2 and not at
the isoluminant point defined by flicker photometry (zero on the
abscissa). Figure 2. Paired-comparison
method. Points plot the proportion of times stimuli were judged to appear more
like a spatial square wave than stimuli of all the other elevations. Curve is a
Gaussian fit to the points. Peak: 0.85. Sigma: 8.7. Abscissa at peak: -25.6
deg.
Most of the measurements of vernier and stereo
thresholds were made using the method of constant stimuli. In the vernier
experiments, the observer reported whether the lower target appeared to be
offset to the left or right of the upper target. In the stereo experiments, the
observer reported whether the lower target appeared to be nearer or farther away
than the upper target.
Vernier and stereo thresholds are plotted as a function
of contrast in Figure 3 for luminance and L-M
modulated targets. Contrast is expressed logarithmically relative to detection
thresholds. Thresholds are expressed logarithmically relative to 1 arcs. In all
cases, the slopes are on the order of -0.5, in agreement with previous results
on vernier thresholds ( Krauskopf &
Farell, 1991) and on stereo thresholds ( Legge
& Gu, 1989; but see Westheimer
& Pettet, 1990). One line of slope -0.56 fits both the chromatic and
luminance data for vernier but the chromatic and luminance thresholds for stereo
cannot be fit with a single line. The chromatic thresholds are approximately 0.5
log units higher than would be projected from the luminance thresholds. This
effect is not as large as that shown in Figures
4 and 5. In these experiments, the
standard definition of isoluminance was used. In the subsequent experiments,
isoluminance was defined as illustrated in Figure
2 and the effects were, accordingly,
larger. Figure 3. Stereo thresholds and vernier
thresholds as a function of target contrast for luminance and isoluminant
targets. Contrasts are expressed logarithmically relative to contrast thresholds
for detection. Offsets are expressed logarithmically relative to 1 arcs. Lines
are linear least
squares fits. Results are for one observer.
Stereo and vernier thresholds are plotted for two
observers as a function of elevation of the modulation out of the isoluminant
plane in Figure 4. Vernier thresholds are
independent of elevation as expected of equally detectable stimuli if photons
caught are used efficiently. Stereo thresholds are an order of magnitude higher
for isoluminant stimuli than for luminance-modulated stimuli. For both
observers, the stereo thresholds peak in the vicinity of the estimated elevation
of the isoluminant plane.
Could the observers be using the information contained
in the luminance component of the stimuli? Informal estimates of stereo
thresholds as a function of elevation of targets out of the isoluminant plane
were made assuming that only the luminance component of the tests were processed
in evaluating target depth and that stereo thresholds are inversely proportional
to the square root of target contrast (as shown in Figure 3). Observed thresholds in the vicinity
of isoluminance exceeded these estimates, suggesting that not all the available
information is used. The finding that thresholds were higher than expected from
the luminance component led us to perform the mixture experiment described
later.
Berry (1948) reported
that vernier thresholds increased with the size of the gap between the bottom
and top targets, whereas stereo thresholds remained approximately constant,
independent of the gap. We made similar measurements to see whether these
functions might be different for chromatic and luminance targets. In Figure 5, measurements of stereo and vernier
thresholds for target modulated in luminance and isoluminantly are plotted as a
function of the size of the gap between the top and bottom
elements. Figure 4. Offset thresholds for vernier and
stereo targets as a function of elevation of the test stimuli out of the
isoluminant plane. Contrast was set at the maximum possible for isoluminant
targets and at equal contrast relative to detection threshold for all other
elevations. Observer J.F.'s isoluminant plane was estimated to be -26 deg out of
the canonical isoluminant plane. Observer J.K.’s isoluminant plane was
estimated to be -18 deg out of the canonical isoluminant plane. These angles are
expressed in a space with threshold normalized axes, which accounts for the
seemingly large magnitude of the deviation of the isoluminant plane. The gap
between the top and bottom targets was 1 arcmin for the vernier experiments and
10 arcmin for the stereo experiments.
Vernier thresholds are essentially the same for targets
modulated in luminance and along the L-M cardinal axis, confirming Krauskopf and Farell (1991). Thresholds
for vernier targets are 2 to 3 times larger with a gap of 20 arcmin than with a
gap of 1 arcmin. The trends for stereo thresholds are quite different.
Thresholds decrease with increasing gap by a factor of about 2 to 3, confirming
Westheimer and McKee (1979). The
outstanding result is the marked elevation for the stereo thresholds for targets
modulated isoluminantly compared to those modulated in luminance (a factor on
the order of 10-fold), confirming the results plotted in Figure 4. Figure 5. Vernier and
stereo thresholds as a function of the gap between upper and lower target
elements for targets modulated in luminance and isoluminantly along the L-M
cardinal axis. Contrast is set at the maximum possible for isoluminant targets
and equal contrast relative to thresholds for luminance targets. Thresholds were
measured using a method of constant stimuli.
The stimuli used in the mixture experiment are
illustrated in Figure 6. Stereo thresholds
were measured by the standard staircase procedure for targets defined purely by
luminance and for targets with the same luminance modulation to which was added
a large chromatic component.
Median thresholds for three observers for the three
conditions are presented in Figure 7. If
stereo disparity is processed by independent chromatic and luminance mechanisms,
disparity thresholds should at least be as low for mixtures of chromatic- and
luminance-modulated targets as they are for
targets modulated only in luminance. This result would be expected whatever the
postulated mechanism of summation: probability summation, energy summation, etc.
But the performance of two of the observers is clearly poorer for the mixed
stimuli and tends to be poorer for the third
observer. Figure 6. Modulation
directions of stimuli used in mixture experiments. Red arrows represent
luminance targets with modulation 0.3. Green arrows represent stimuli composed
of the 0.3-luminance modulation and 0.7 of the maximum modulation available in
the L-M direction. Blue arrows are the same as the green but with the phase of
the luminance component inverted.
Figure 7.
Median disparity thresholds for three observers for targets modulated in
luminance and for the same stimuli to which a substantial L-M component had been
added. Individual analyses of variance revealed significant conditions effects
at the 1% level of significance for two of the three observers.
It should be noted that the luminance component was
added in both phases with respect to the isoluminant component. This guarded
against the possibility that the L-M component was not truly isoluminant, and
thus might add constructively or destructively to the luminance modulation.
The observers found the stereo task more difficult to
perform with stimuli modulated chromatically than with stimuli modulated in
luminance, and the psychometric functions tended to be shallower for
chromatically modulated stimuli. No such effects were noted in the vernier
case.
The data presented in Figures 3, 4,
and 5 reveal that when detectability is
controlled, stereo depth thresholds are substantially higher for targets
modulated isoluminantly than for ones modulated in luminance. The effect is
large, a factor of 10 or more. In comparison, vernier thresholds exhibit the
same dependence on contrast relative to threshold, showing there is a clear
difference in the utility of color information for stereo and vernier
mechanisms.
Could the stereo thresholds at isoluminance be a
manifestation of luminance artifacts? The very size of the elevation of the
stereo thresholds compared to those for luminance-modulated targets would seem
to rule out such an explanation. The contrasts of stimuli in Figures 4 and 5 are
approximately 1 log above detection threshold. The stereo thresholds at
the observers’ isoluminant elevation are a log unit or more higher than
those for luminance-modulated targets. If we extrapolate using Figure 3, the implied contrast of the luminance
artifact would be 1 log unit or more below detection threshold.
One possible explanation for poorer chromatic stereo
performance is that the frequency components useful in making stereo judgments
are poorly transmitted by the chromatic mechanisms. The spatial modulation
sensitivity curves for luminance-modulated stimuli are band pass, whereas those
for isoluminantly modulated stimuli tend to be low pass. Equating stimuli in
terms of detection thresholds may tend to handicap the isoluminant stimuli
slightly to the extent that their detection is mediated by low spatial
frequencies, which may contribute little to the detection
of stereo offsets, whereas detection of
luminance targets is mediated by higher spatial frequencies. Analysis of this
factor for vernier thresholds suggested that it was very small ( Krauskopf & Farell, 1991). It is
unlikely to be sufficiently large in the case of stereo to account for the
difference in stereo thresholds for luminance and isoluminant targets.
Another potential reason for a difference in chromatic
and luminance stereo performance could be that there are separate mechanisms for
processing luminance-modulated stimuli and chromatic-modulated stimuli ( Simmons & Kingdom, 1997). There is evidence
for distinct chromatic and luminance mechanisms for motion perception. Krauskopf and Li (1999) found a marked
dependence on contrast for the detection of motion in a single target in the
visual field for chromatic targets while confirming the contrast independence of
thresholds for luminance targets ( McKee, Silverman,
& Nakayama, 1986). Krauskopf and Li
(1999) concluded that the mechanism that processed retina-relative signals
was not responsive to chromatic signals but that both classes of signal were
processed by a mechanism that interprets object-relative signals. We found no
difference in functional dependence in the case of stereo thresholds lessening
the support for independent mechanisms. In fact, the results presented in Figures 3 and 5 show parallel effects of contrast and gap for
luminance and isoluminant tests. If color and luminance are processed by a
single stereo mechanism, the question remains why color information is not as
useful.
Several lines of evidence converge to support the
notion that the same kinds of mechanism support stereo judgments for chromatic
and luminance targets and reveal why depth perception is, nevertheless, poorer
for isoluminant stimuli.
Vernier offsets can be seen monocularly, and do not
require information from the eyes to be combined, whereas stereopsis requires
processing of information from both eyes. Current models of vernier (see Klein & Levi, 1985; Wilson, 1986) are based on orientation-selective
filters with properties similar to the receptive fields of cortical neurons
found at the earliest stages of visual processing (although recent masking
studies suggest that psychophysical performance may involve combinations of
these filters and binocular processes [see Levi,
Klein, & Carney, 2000]). Physiological models of stereopsis are based on
cortical neurons that can compute disparity ( Anzai,
Ohzawa, & Freeman, 1999; Cumming &
DeAngelis, 2001; DeAngelis, Ohzawa, &
Freeman, 1991; Dodd, Krug, Cumming, &
Parker, 2001). The additional stage of processing information from both eyes
in stereopsis may handicap color inputs for depth judgments.
To be useful for depth perception, cortical neurons
require receptive fields that are positioned at roughly corresponding points in
the two retinas and with similar selectivity along various dimensions, including
spatial frequency and orientation. Although not mentioned in the literature,
another requirement is that receptive fields have similar preferred directions
in color space. The physiological evidence suggests there are proportionally
fewer neurons preferring isoluminant stimuli at successively higher stages of
processing ( Lennie, Krauskopf, & Sclar,
1990). Those binocular neurons that do have significant chromatic
sensitivity are unlikely to have inputs that have highly correlated preferred
directions in color space.
Recordings of single-unit activity in V1 indicate that
most cells respond well to monocular stimuli modulated in luminance and that
fewer prefer isoluminant or nearly isoluminant stimuli ( Lennie et al., 1990; although see Johnson, Hawken, & Shapley, 2001).
Furthermore, the data from Lennie et al.
(1990) suggest that nonoriented neurons show greater chromatic response than
simple cells, which in turn are more selective for color than complex cells.
Nonoriented receptive fields are often found in input layers of visual cortex,
and there is some evidence that many complex cells are formed from combinations
of simple cells (see Martinez & Alonso,
2001; Spitzer & Hochstein, 1988). If
the classification of cell types ( Lennie et al.,
1990) is consistent with hierarchical stages of processing in V1, then it
suggests that chromatic sensitivity progressively diminishes with successive
visual computations.
Electrophysiological findings suggest that
proportionally fewer binocular neurons respond well to isoluminant stimuli than
to luminance stimuli. Furthermore, the angular difference in the vectors of best
response to stimuli to the two eyes appears to be inversely related to their
average elevation. The stimuli that provide a balanced input to the two eyes are
those that bisect the angle between the two vectors. Stimuli along other
directions will suffer more of a mismatch in effectiveness for chromatic stimuli
than for luminance stimuli.
We suggest that diminished chromatic sensitivity in
visual cortex and differences in the chromatic tunings of binocular cells result
in both a reduction in contrast and a mismatch in the strength of the signals
from the two eyes. Psychophysical results show that mismatches in the contrast
of stereo targets elevate thresholds ( Legge &
Gu, 1989). This may explain the elevated psychophysical thresholds for depth
judgments with isoluminant stimuli (but see Truchard, Ohzawa, & Freeman, 2000).
Depth thresholds for isoluminant stimuli are higher
than luminance stimuli when stimulus contrast is equated relative to detection
thresholds. Vernier thresholds are similar for isoluminant and luminance stimuli
and covary as a function of target separation. Depth thresholds for isoluminant
and luminance stimuli also covary as a function of target separation, suggesting
that they are mediated by a functionally similar mechanism.
Disparity thresholds are higher for targets modulated
with mixtures of luminance modulation and chromatic modulation than for targets
modulated only in luminance. This is strong evidence against the hypothesis that
there are independent chromatic and luminance mechanisms for evaluating
disparity.
Our results are consistent with a single stereopsis
mechanism for isoluminant and luminance stimuli. Elevated stereo thresholds for
isoluminant targets may be explained by physiological evidence that binocular
combinations of chromatic inputs are fewer and less correlated in the preferred
color direction than luminance inputs. The effect of lower signal strength and
correlation is consistent with psychophysical evidence that shows contrast
reduction and imbalance elevate depth thresholds.
This work was made possible by grant EY06638 from the
National Eye Institute. The authors would like to thank Peter Lennie for
commenting on the manuscript and Jon Peirce and Isabelle Mareschal for
assistance as observers and for technical discussion. Commercial Relationships:
None.
Anzai, A., Ohzawa, I., &
Freeman, R. D. (1999). Neural mechanisms for encoding binocular disparity:
Receptive field position versus phase. Journal
of Neurophysiology, 82, 874-890. [PubMed]
Berry, R. N. (1948). Quantitative
relations among vernier, real depth, and stereoscopic depth acuities.
Journal of Experimental Psychology, 38,
708-721.
Cumming, B. G., & DeAngelis,
G. C. (2001). The physiology of stereopsis.
Annual Review of Neuroscience, 24,
203-238. [PubMed]
DeAngelis, G. C., Ohzawa, I.,
& Freeman, R. D. (1991). Depth is encoded in the visual cortex by a
specialized receptive field structure. Nature,
352, 156-159. [PubMed]
Derrington, A. M., Krauskopf,
J., & Lennie, P. (1984). Chromatic mechanisms in lateral geniculate nucleus
of macaque. Journal of Physiology, 357,
241-265. [PubMed]
Dodd, J. V., Krug, K., Cumming, B.
G., & Parker, A. J. (2001). Perceptually bistable three-dimensional figures
evoke high choice probabilities in cortical area MT.
Journal of Neuroscience, 21, 4809-4821.
[PubMed]
Johnson, E. N., Hawken, M. J.,
& Shapley, R. (2001). The spatial transformation of color in the primary
visual cortex of the macaque monkey. Nature
Neuroscience, 4, 409-416. [PubMed]
Kingdom, F. A., &
Simmons, D. R. (1996). Stereoacuity and colour contrast.
Vision Research, 36, 1311-1319. [PubMed]
Kingdom, F. A., Simmons, D.
R., & Rainville, S. (1999). On the apparent collapse of stereopsis in
random-dot-stereograms at isoluminance. Vision
Research, 39, 2127-2141. [PubMed]
Klein, S. A., & Levi, D. M.
(1985). Hyperacuity thresholds of 1 sec: Theoretical predicitions and empirical
validation. Journal of the Optical Society of
America A, 2, 1170-1190. [PubMed]
Krauskopf, J., &
Farell, B. (1991). Vernier acuity: Effects of chromatic content, blur and
contrast. Vision Research, 31, 735-749.
[PubMed]
Krauskopf, J., & Li,
X. (1999). Effect of contrast on detection of motion of chromatic and luminance
targets: Retina-relative and object-relative movement.
Vision Research, 39, 3346-3350. [PubMed]
Krauskopf, J., Williams,
D. R., & Heeley, D. W. (1982). Cardinal directions of color space.
Vision Research, 22, 1123-1131. [PubMed]
Krauskopf, J., Wu, H. J.,
& Farell, B. (1996). Coherence, cardinal directions and higher-order
mechanisms. Vision Research, 36,
1235-1245. [PubMed]
Legge, G. E., & Gu, Y. C.
(1989). Stereopsis and contrast. Vision
Research, 29, 989-1004. [PubMed]
Lennie, P., Krauskopf, J., &
Sclar, G. (1990). Chromatic mechanisms in striate cortex of macaque.
Journal of Neuroscience, 10, 649-669.
[PubMed]
Levi, D. M., Klein, S. A., &
Carney, T. (2000). Unmasking the mechanisms for Vernier acuity: Evidence for a
template model for Vernier acuity. Vision
Research, 40, 951-972. [PubMed]
Livingstone, M. S., &
Hubel, D. H. (1987). Psychophysical evidence for separate channels for the
perception of form, color, movement, and depth.
Journal of Neuroscience, 7, 3416-3468.
[PubMed]
Martinez, L. M., & Alonso,
J. M. (2001). Construction of complex receptive fields in cat primary visual
cortex. Neuron, 32, 515-525. [PubMed]
McKee, S. P., Silverman, G. H.,
& Nakayama, K. (1986). Precise velocity discrimination despite random
variations in temporal frequency and contrast.
Vision Research, 26, 609-620. [PubMed]
Morgan, M. J., & Aiba, T. S.
(1985). Positional acuity with chromatic stimuli.
Vision Research, 25, 689-695. [PubMed]
Scharff, L. V., & Geisler,
W. S. (1992). Stereopsis at isoluminance in the absence of chromatic
aberrations. Journal of the Optical Society of
America A, 9, 868-876. [PubMed]
Simmons, D. R., & Kingdom,
F. A. (1997). On the independence of chromatic and achromatic stereopsis
mechanisms. Vision Research, 37,
1271-1280. [PubMed]
Spitzer, H., & Hochstein, S.
(1988). Complex-cell receptive field models.
Progress in Neurobiology, 31, 285-309.
[PubMed]
Sullivan, G. D., Oatley, K.,
& Sutherland, N. S. (1972). Vernier acuity as affected by target length and
separation. Perception and Psychophysics,
12, 438-444.
Truchard, A. M., Ohzawa, I.,
& Freeman, R. D. (2000). Contrast gain control in the visual cortex:
Monocular versus binocular mechanisms. Journal
of Neuroscience, 20, 3017-3032. [PubMed]
Westheimer, G., &
McKee, S. P. (1979). What prior uniocular processing is necessary for
stereopsis? Investigative Ophthalmology and
Visual Science, 18, 614-621.
Westheimer, G., &
Pettet, M. W. (1990). Contrast and duration of exposure differentially affect
vernier and stereoscopic acuity. Proceedings
of the Royal Society of London. Series B: Biological Sciences, 241,
42-46. [PubMed]
Wilson, H. R. (1986). Responses
of spatial mechanisms can explain hyperacuity.
Vision Research, 26, 453-469. [PubMed]
|