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The Journal of Neuroscience, July 15, 2002, 22(14):6158-6175
Space and Time Maps of Cone Photoreceptor Signals in Macaque
Lateral Geniculate Nucleus
R. Clay
Reid1, 2 and
Robert M.
Shapley1
1 Center for Neural Science, New York University, New
York, New York 10003, and 2 Department of Neurobiology,
Harvard Medical School, Boston, Massachusetts 02115
 |
ABSTRACT |
We studied neurons in the central visual field representation of
the lateral geniculate nucleus (LGN) in macaque monkeys by mapping
their receptive fields in space and time. The mapping was performed by
reverse correlation of a spike train of a neuron with pseudorandom,
binary level stimuli (m-sequence grids). Black and white m-sequence
grids were used to map the receptive field for luminance. The locations
of receptive field center and surround were determined from this
luminance map. To map the contribution of each cone class to the
receptive field, we designed red-green or blue-yellow
m-sequence grids to isolate the influence of that cone (long, middle,
or short wavelength-sensitive: L, M, or S). Magnocellular neurons
generally received synergistic input from L and M cones in both the
center and the surround. A minority had cone-antagonistic (M-L) input
to the surround. Red-green opponent parvocellular neurons received
opponent cone input (L+M
or M+L
) that overlapped in space, as
sampled by our stimulus grid, but that had somewhat different extents.
For example, an L+ center parvocellular neuron would be L+/M
in both
center and surround, but the L+ signal would be stronger in the center
and the M
signal stronger in the surround. Accordingly, the luminance
receptive field would be spatially antagonistic:
on-center/off-surround. The space-time maps also characterized
LGN dynamics. For example, magnocellular responses were transient,
red-green parvocellular responses were more sustained, and blue-on
responses were the most sustained for both luminance and cone-isolating
stimuli. For all cell types the surround response peaked 8-10 msec
later than the center response.
Key words:
receptive field; primate; color; LGN; lateral geniculate; retina; dynamics; cone photoreceptor; m-sequence
 |
INTRODUCTION |
The purpose of our experiments was
to investigate the possible roles in color vision of parvocellular and
magnocellular neurons in the lateral geniculate nucleus (LGN) of
Macaca fascicularis. Macaques have three types of cone
photoreceptor with peak sensitivities at different wavelengths: the L
cones at 565 nm, M cones at 535 nm, and S cones at 440 nm (Smith and
Pokorny, 1972
, 1975
; Baylor et al., 1987
). The spatial and temporal
maps of these photoreceptors to LGN neurons determine the responses of
the neurons to color. We sought to answer the following questions: (1)
How are cone photoreceptor signals mapped onto individual LGN cells?
(2) How is this mapping different, or similar, for parvocellular and
magnocellular neurons? (3) What is the time course of responses for
magnocellular and parvocellular neurons in both center and surround?
The influence of each cone class on a receptive field of a neuron was
measured with a combination of two techniques: m-sequence grids (a form
of white noise receptive field mapping) and cone-isolating stimuli
(Fig. 1, Stimuli) (Sutter,
1987
, 1992
; Reid and Shapley, 1992
; Reid et al., 1997
). Together, these
methods yield spatial maps of the responses evoked by each cone class
and, further, characterize the time evolution of these responses. Black
and white m-sequence grids were used to characterize the conventional receptive field for achromatic stimuli. From these achromatic measurements we estimated the spatial location and extent of the receptive field center and surround. Then the sign, magnitude, and
dynamics of the cone signals that provided the input to the center and
surround were determined from the cone maps. This enabled us to
determine the dynamics of cone inputs to center and surround in
magnocellular and parvocellular neurons. This also allowed us to test
hypotheses about the cone inputs to receptive field center and
surround.

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Figure 1.
The cone-specific and mixed surround models for
red-green opponent parvocellular neurons, specifically L-on/M-off type
I neurons [after Reid and Shapley (1992) , their Fig. 1].
Stimuli, Representations of the binary m-sequence grid
stimuli, which are either luminance modulated (between black and white)
or chromatically modulated between hues that modulate either L cones or
M cones in isolation. For the L-cone stimulus the red is
brighter than the mean (on); the green is darker than
the mean (off). For the M-cone stimulus the green is
brighter (on); the red is darker (off).
Model, Diagrammatic representations of receptive fields,
color-coded in terms of the cone-isolating stimuli that drive them. In
the cone-specific surround model (first row) the
L-on center (L+) is opposed by an M-off surround (M ). In the mixed
surround model the L-on center is opposed both by M-off and L-off
surround (L and M ). Predicted Results, Spatial
weighting functions as mapped with the luminance, L-cone, and M-cone
stimuli. Responses are coded in false color: on (+) in
red and off ( ) in blue. Responses of
the center cone type, the L cone, represent the critical test between
models. In the cone-specific surround the L-cone responses are
exclusively on. In the mixed surround (arrow), the
L-cone responses are on-center/off-surround.
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Magnocellular neurons in the LGN receive mixed cone inputs to their
receptive field centers and, in most cases, to their surrounds. By
contrast, we found direct evidence for the idea that excitation and
inhibition in almost all red-green opponent parvocellular neurons
(within 13° of the fovea) are both cone-specific. Mixed cone input to
the surround would be observable experimentally as an antagonistic
center/surround relationship for a single cone class, specifically the
cone class of the center (see Fig. 1, arrow). Most
red-green opponent parvocellular neurons had center/surround antagonistic responses to a luminance stimulus (type I cells; Wiesel
and Hubel, 1966
), but the spatial map of cone-isolated responses was
monophasic, with a profile resembling a bell-shaped curve. It would be
difficult to prove the surround absolutely specific, but our results
are consistent with others (Lee et al., 1998
) in finding the
random-surround model very improbable.
The time course of cone signals is also important for color vision. The
dynamics of parvocellular and magnocellular neurons differ for both
black and white and cone-isolating stimuli: for all stimuli the
magnocellular responses are more transient. Another dynamic result is
that surround signals are slower than center signals for magnocellular
and red-green opponent parvocellular neurons and for their
cone-isolated inputs. As discussed below, this probably is not
caused by processes within the LGN but, instead, arises from the
properties of retinal circuitry and synapses.
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MATERIALS AND METHODS |
Cynomolgus monkeys, M. fascicularis
(n = 5), were anesthetized initially with ketamine (10 mg/kg, i.m.) and intravenous sodium thiamylal (25 mg/kg, supplemented
as needed) and maintained in an anesthetized state during the
experiment with urethane (20-30 mg/kg per hr, i.v.). Temperature, EKG,
EEG, blood pressure, and expired CO2 were
monitored continuously throughout the experiment. Eyes were dilated
with 1% atropine and were protected with contact lenses with a 3 mm
artificial pupil. The animals were paralyzed with gallamine
triethiodide (20-40 mg/hr, i.v.). To minimize residual eye movements
under paralysis, we fixed metal posts to the scleras just beyond the
limbus with cyanoacrylate glue. Refractive errors were corrected to
within one-half diopter with lenses placed in front of the eyes. Lenses
were chosen by optimizing the response of a parvocellular neuron to an
achromatic drifting grating of high spatial frequency.
Action potentials of neurons in the LGN were recorded with glass-coated
tungsten microelectrodes (Alan Ainsworth, London, UK). The Discovery
software package (DataWave Systems, Longmont, CO) was used to
discriminate the spikes of individual neurons. In some cases two
neurons were recorded simultaneously from the same electrode and were
discriminated by their amplitude and waveform. Distinctions between
magnocellular and parvocellular neurons were made on the basis of
alternation of eye preference between laminas and from visual response
properties such as color opponency and contrast sensitivity for grating stimuli.
Protocol for receptive field studies. For each cell the
color specificity and receptive field location were determined
qualitatively with hand-held stimuli. Then the receptive field was
centered on the screen, and quantitative studies were performed, both
with sinusoidal gratings and with pseudorandom binary white noise
stimuli (m-sequence grids; see below). All cells were studied with
m-sequence grids in the luminance, L-cone, and M-cone-isolating
conditions (see below). Parvocellular neurons, which are relatively
insensitive to luminance contrast, were studied with 100% luminance
contrast. Magnocellular neurons were studied with 25% luminance
contrast (with one exception, studied with 100% contrast), which is
approximately equal to the contrast of the L- and M-cone-isolating
stimuli. Most parvocellular neurons also were studied with S-cone
isolating m-sequence grids, except for nine red-green opponent
parvocellular cells that responded poorly to S-cone-isolating gratings
or to blue hand-held stimuli. Three of the magnocellular cells were studied with S-cone-isolating m-sequence grids as well.
Chromatic calibration and cone-isolating stimuli. The visual
stimuli were generated on a PDP-11 computer that controlled a visual
stimulator designed and built in the Laboratory of Biophysics at the
Rockefeller University (Milkman et al., 1980
). The visual stimulator
drove a color monitor (Tektronix S690) at a refresh rate of 135 Hz
(note below that the stimulus itself was updated every other frame, or
at 67.5 Hz). The luminance of each of the three phosphors was
linearized by means of a lookup table. A white point and mean luminance
then were chosen (x = 0.33, y = 0.35; luminance = 75 cd/m2 or, in one
animal, 170 cd/m2, corresponding to 675 and 1530 trolands, respectively). At the values corresponding to this
white point, the radiance spectrum of each of the red, green, and blue
phosphors was measured in 2 nm increments between 430 and 690 nm (Photo
Research Spectrascan Spectroradiometer PR 703A).
The absorption spectra of the three cones were used to create
cone-isolating stimuli (Estevez and Spekreijse, 1974
, 1982
). Spectra
from human psychophysical data [from Boynton (1979)
, based on 2°
data from Smith and Pokorny (1972
, 1975
)] were used because they
incorporate both preretinal as well as retinal absorption; no such data
are available for macaques. The efficacy of each of the three phosphors
in exciting the three cone classes is calculated by taking the dot
product of each phosphor radiance spectrum (taken at its mean) with
each cone absorption spectrum. These dot products are the excitation
values of the cones by the respective phosphors; they form a 3 × 3 matrix, T, that characterizes the linear transformation
between phosphor space (r, g, b) and cone space (l, m,
s).
The physical contrasts by which the phosphors are modulated
(conr,
cong, and
conb) are defined as their fractional deviation from the mean. Similarly, cone contrasts (CONl,
CONm, and CONs) are
defined as their fractional deviation from their mean excitation. The
relationship between physical contrasts and cone contrasts take on a
simple form if the mean luminances are normalized to 1.0, and the
matrix, T, is normalized row by row so that the mean cone
excitations are also 1.0. In this case the cone contrasts are given
by:
where CON is the vector form of the cone contrasts
and con is the vector form of the phosphor contrasts.
The physical contrasts, conr,
cong, and conb, which
yield cone-isolating stimuli, can be obtained by calculating the
inverse of the transformation matrix T. The maximal
contrasts obtainable in this study (determined by phosphors and by our
chosen white point) were:
For each cone-isolating stimulus there are a bright phase and a
dark phase, which correspond to the two states that a pixel may be set
in a binary m-sequence. For instance, for the L-cone stimulus there is
a bright, unsaturated red and darker, more saturated green. These
colors excite the L cone 24% more and 24% less than the mean, respectively.
The cone-isolating stimuli were checked in two ways. First the actual
spectra of the cone-isolating stimuli, for instance the bright red and
dark green of the L-cone stimulus, were measured with the
spectroradiometer. The original calculation of cone-isolating stimuli
(above) assumes perfect linearity of the three phosphors. By taking the
dot product of the measured spectra with the cone absorption spectra,
we could assess more directly the cone excitations (and thus contrasts)
that they evoked, both for the "isolated" cone as well as for the
"silenced" cones. If the silenced cone contrasts were >0.5% (as
they were in several cases), the physical contrasts of the three
phosphors were varied systematically until the silenced cone contrasts
were <0.5%. A second check on the stimulus was provided by a human
protanope volunteer, who was virtually unable to differentiate the
L-cone stimulus from a uniform gray screen.
Mapping with m-sequence grids: spatiotemporal weighting function.
Receptive field mapping with white-noise stimuli has been described in detail by us and by others (Citron et al., 1981
; Emerson
et al., 1987
; Jacobson et al., 1993
; Reid et al., 1997
). The approach
is very similar to the reverse-correlation method (Jones and Palmer,
1987
). In the Jones and Palmer method only one pixel is modulated from
the mean level during each stimulus frame. We used the binary
m-sequence method (Sutter, 1987
, 1992
; Reid et al., 1997
) in which
every pixel takes on one of two values with equal probability during
each frame. The m-sequence stimulus is much richer than the sparse
Jones and Palmer (1987)
stimulus (cf. Reid et al., 1997
) and drives
neurons in the LGN quite vigorously. Receptive fields thus can be
mapped both quickly and with low noise.
The stimulus (illustrated in Fig. 1) consisted of a 16 × 16 grid
of pixel (8 × 8 for the first of five experiments). We used different pixel sizes, ranging from 7.5 min (used for most
parvocellular neurons) to 26 min (for peripheral magnocellular
neurons). For parvocellular neurons the size was chosen to be
approximately equal to the diameter of receptive field centers at a
given eccentricity (Lee et al., 1998
) (see Results, Parvocellular
spatial weighting functions). We used large pixels (only slightly
smaller than the receptive field center) so that individual pixels were
more effective in driving the surround. Pixels were therefore too large
to characterize the exact size of the center but certainly not too
large to identify a spatially distinct surround mechanism (see
Results). Even with large pixels, however, single-pixel responses in
the surround were much weaker than in the center. We dealt with this
problem by spatial averaging [see below; also see Reid et al. (1997)
, their Discussion].
For every frame of the stimulus each pixel was assigned one of two
values according to a binary m-sequence (Sutter, 1987
), updated every
other refresh cycle of the monitor, or every 14.8 msec (two frames at
135 Hz). A complete m-sequence had 216
1 = 65,535 frames, which spanned ~16 min. The sequence was split
into eight parts that were run separately. A complete set of
interleaved cone-isolating and luminance m-sequences lasted 4 × 15 = 64 min; data were used if at least three-eighths of the m-sequence was completed (~24 min total).
The neuronal spike trains were correlated with the input m-sequences to
yield the spatiotemporal weighting function (sometimes called the
receptive field), K(x,y,tk),
proportional to the first-order Wiener kernel (in units of spikes/sec)
(Victor, 1992
; Reid et al., 1997
). For example, if
K(x,y,tk) = 2, then on the
average at k
msec after the presentation of a positive
(bright) stimulus at position (x,y), the neuron fired 2 spikes/sec more than the mean rate. If
K(x,y,tk) =
2, then the neuron
fired 2 spikes/sec fewer spikes after the bright phase.
For ease of comparison, all weighting functions (first-order kernels)
in this work will be presented after normalization in units of
(spikes/sec)/(unit contrast). For instance, the L-cone weighting
function, Kl, is normalized by the contrast of
the L-cone stimulus, CONl:
With this normalization the expected value of the luminance
weighting function is particularly simple under the assumption that
single-cone responses add together linearly. Because a luminance stimulus has equal contrast for all three cone classes, the normalized luminance weighting function, Klum, should be
given by:
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Definition of center and surround. To analyze the
sign (on or off), strength, and time course of center and surrounds, we had to separate the spatial weighting function measured with the m-sequence grid stimulus into two regions. The distinction between center and surround regions was straightforward for the spatially opponent luminance weighting function, but for the spatially
nonopponent weighting functions measured with cone-isolating stimuli
(see Figs. 1, 5), the distinction often was less clear. We therefore defined the center from the luminance spatial weighting function by the
following procedure. First the single largest response in the
spatiotemporal weighting function (as mapped with the luminance stimulus) was located. This largest response defined the pixel with the
greatest sensitivity at the peak latency. Next, we took the average of
the spatial weighting functions at the peak latency and the next frame,
to improve signal/noise. If the rebound (see Fig. 5, below) began in
the frame after the peak, then only the peak frame was used (as in Fig.
2, below). Then, pixels were included in the center region if the
responses (1) were of the same sign as the strongest response, (2) were
>2 SD above the measurement noise, and (3) formed a region that was
contiguous with the peak pixel (cf. Usrey and Reid, 2000
; Usrey et al.,
2000
). The surround region of the weighting function was defined as all
pixels that were in a ring around the center region, four pixels wide.
Narrower rings sometimes missed the edges of the surround; wider rings tended to add noise to our estimates of surround responses.
Temporal weighting functions. Once the center and surround
were defined, the time courses of their responses were obtained by
summing over all pixels in each region. These functions of time,
C(tk) and
S(tk), are termed the temporal
weighting functions of the center and the surround regions,
respectively. Time was binned at the update period of the stimulus,
14.8 msec. By our convention the 0.0 msec bin corresponds to responses
in the first stimulus frame, between 0.0 and 14.8 msec. Peak times (see
Fig. 17, below) were determined by interpolation with a cubic spline between data points. For the purpose of assigning an
interpolated time between data points, both for the spline fits and for
the abscissas of the temporal weighting functions (see Figs. 4, 7, 10,
11, below), data points were assigned to the middle of each bin (by
adding 7.4 msec). For instance, the bin that spanned from 14.8 to 29.6 msec was assigned to 23.2 msec.
 |
RESULTS |
Spatiotemporal mapping with cone-isolating and luminance stimuli
was performed on 33 parvocellular neurons and 9 magnocellular neurons
in the macaque LGN. The first-order kernels, calculated by reverse
correlation between a spike train of a neuron and m-sequence grids (see
Materials and Methods), are estimates of the spatiotemporal weighting
function of a neuron. Spatiotemporal weighting functions, measured
separately for each cone class, answered the three questions we posed
in this study. (1) How are cone photoreceptor signals mapped onto
individual LGN cells? (2) How is this mapping different, or similar,
for parvocellular and magnocellular neurons? (3) What is the time
course of the cone inputs to center and surround?
Visual fields of parvocellular neurons ranged from 3 to 13°
eccentric, and those of the magnocellular neurons ranged from 3 to
23°. Of the 33 parvocellular neurons, 27 had antagonistic input from
the L and M cones (red-green opponent), and two were not
color-opponent (broadband). Four neurons found among the lower parvocellular layers had strong S-cone input (blue-yellow opponent). The dominant inputs to the 31 color-opponent cells were L-on, 9; L-off,
8; M-on, 5; M-off, 5; S-on, 3; and S-off, 1.
Magnocellular spatial weighting functions
The data from magnocellular neurons consistently showed additive
convergence of L and M cones onto the receptive field center. This can
be observed in Figure 2, which displays
spatial weighting functions of a single off-center magnocellular
neuron. Data are shown for the frame at peak latency; separate
weighting functions are shown for L-cone, M-cone, and luminance
stimuli. For magnocellular cells this peak latency is in the range of
15-30 msec. Below each spatial weighting function we show the radial
weighting function, the values of the spatial weighting functions
summed over concentric annuli, as a function of the distance from
receptive field center.

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Figure 2.
Top, Spatial weighting functions of
an off-center magnocellular neuron (23° eccentric) measured with
L-cone-isolating, M-cone-isolating, and luminance-modulated stimuli.
Each panel corresponds to the same region of visual
space, 5.2° on a side. On responses are coded in red
and off in blue; the brighter the red or
blue, the stronger the response. All maps, L- and M-cone
isolating and luminance, have an off-center/on-surround organization.
Individual pixels (0.43°) are outlined in black.
Pixels in the center (defined as in Materials and
Methods) are outlined in white. Surround is a ring of
four pixels around the center. Data are smoothed by a function that
falls to <10% at one-half pixel. Delay between stimulus and response,
15-30 msec. Bottom, Radial weighing functions
calculated from the spatial weighting function above (see Materials and
Methods). For comparison with the spatial weighting function, the
radial weighing function is reflected about the origin so that each
value is shown twice. To facilitate comparison, we have given all
responses in units of spikes/(sec · C), where
C is the cone contrast of the stimulus (see Materials
and Methods).
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The radial weighting functions are shown in units of (spikes/sec)/(unit
contrast), as are all weighing functions throughout the paper. As noted
in Materials and Methods, when weighting functions are normalized by
the stimulus contrast, the luminance weighting function is expected to
equal the sum of the cone-isolated weighting functions. In general, the
luminance weighting functions were very close to this linear
prediction, particular for the receptive field center. Magnocellular
center responses were, on average, 75% of the linear prediction;
parvocellular center responses were, on average, 90% of the linear
prediction (analysis not shown).
The L- and M-cone spatial weighting functions are very similar for the
neuron in Figure 2, meaning that the L and M cones produce similar
signals when they excite such magnocellular cells. In particular, both
L and M cones have off or "decrement excitatory" responses in the
receptive field center of the cell; they have the same sign of
response. In this neuron, which is representative of magnocellular
cells of type III (Wiesel and Hubel, 1966
), both L and M cones form the
input to the surround of the receptive field, and they have the same
sign of surround response, on or "increment excitatory." The
surround is therefore of opposite sign to that of the center. Note
that, therefore, each cone type has a spatial weighting function with a
center/surround or "Mexican hat" shape, resembling the difference
of Gaussians or DOG model (Rodieck, 1965
; Enroth-Cugell and Robson,
1966
). The center/surround organization is particularly evident for the
L-cone response in this example. This is important because it
establishes that, for magnocellular cells, it is possible to measure
center/surround antagonism for a single cone class.
There was no measurable S-cone input to this neuron. Before the
m-sequence runs the neuron was stimulated with a high-contrast S-cone-isolating sine grating, and it was unresponsive.
Magnocellular movies: spatiotemporal weighting functions
The data in Figure 2 give a detailed picture of the spatial
weighting function of the magnocellular cell at one moment in time, but
m-sequence measurements also allow one to reconstruct the entire time
course of the responses to study the dynamics at each point in the
receptive field. Figure 3 shows plots of spatial weighting functions from the same off-center magnocellular cell
at six different time delays between stimulus and response, ranging
from 0 to 89 msec. We refer to this form of data display as a response
movie, because if each column of images were shown in sequence, it
would be an animation of the time evolution of the spatial weighting
function. The scale at the bottom indicates the response magnitude in
units of (spikes/sec)/(unit contrast) (see Materials and Methods).

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Figure 3.
Spatiotemporal weighting functions of the same
magnocellular neuron (Fig. 2) for multiple delays, from the 0 msec bin
(0-15 msec) to the 74 msec bin (74-89
msec). Responses to different stimuli, shown from
left to right: L cone, M cone, and
luminance. Conventions are as in Figure 2. Off-center response starts
in the 0 msec bin, peaks in the 15 msec bin, and reverses sign
(rebounds) at either 30 or 44 msec. On-surround starts at 15, peaks at
30, and reverses at 44 msec. The M-cone response is delayed slightly
relative to the L-cone response. Scale at bottom
indicates response magnitudes in spikes/(sec · C),
where C is the cone contrast of the stimulus.
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First let us consider the luminance movie in the right-hand column of
Figure 3. For the first delay that is illustrated, denoted 0-15 msec,
there is a small but clear off (decrement excitatory) response. This
means that this magnocellular cell had a receptive field center with a
latency of response <15 msec (as did one other cell; these
exceptionally fast cells were fairly peripheral, ~20° from the
fovea). The response of the center peaked in the range 15-30 msec and
then changed sign from 30 up to 89 msec. The on (increment excitatory)
surround is slower to respond than the center. The first significant
surround on response occurs in the 15-30 msec time period. The
surround also has a rebound but later, after 44 msec when the receptive
field inverts its sign completely; compare the images at 15-30 and
44-59 msec.
The L-cone spatiotemporal weighting function has almost exactly the
same time course as that of the luminance signal. The M-cone responses
in the center begin just as rapidly as those of the L cone, at 0-15
msec, but M-cone rebounds, both center and surround, are delayed
compared with those of the L cone. Such a qualitative difference
between L- and M-cone dynamics may be attributable to the retinal
contrast gain control (Shapley and Victor, 1981
; Benardete et al.,
1992
). Because the L-cone stimulus was more effective in driving the
cell than the M-cone stimulus, perhaps it also drove the contrast gain
control mechanism more.
Magnocellular center and surround temporal weighting functions
A quantitative evaluation of the space-time maps can be made by
inspecting the time evolution of center and surround components of the
responses, plotted on the same scale (Fig.
4). Responses of all pixels in the center
and all pixels in the surround regions were summed separately to create
temporal weighting functions (see Materials and Methods). In each panel
of Figure 4 the temporal weighting functions for the center region
(thick line) and for the surround region (thin
line) are plotted as a function of time. Increment excitatory
responses are positive in sign; decrement excitatory responses are
negative. The temporal weighting functions for the magnocellular neuron
(Fig. 4) are quite similar for L and M cones and for luminance
modulation. The peaks of the center responses occur approximately
one-half frame (~7 msec) earlier than the surround peaks
(interpolations not shown; see Materials and Methods). The M-cone
response is ~2-3 times smaller than the L-cone response both in
center and surround.

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Figure 4.
Temporal weighting functions of the
same magnocellular neuron (Figs. 2, 3) for receptive field center
(thick lines) and surround (thin lines).
Each data point is for a range of times between stimulus and response
(sampled at the stimulus update rate, or 14.8 msec; short tick
marks). The data points marked with carets
correspond to responses during the first bin (in the range 0-14.8
msec). Time labels (long tick marks) are interpolated
with respect to the data points (short tick marks), as
specified in Materials and Methods. Note that the M-cone response is
both weaker and somewhat slower than the L-cone response. All responses
are in spikes/(sec · C), where C is the
cone contrast of the stimulus.
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Parvocellular spatial weighting functions
Parvocellular spatial weighting functions were measured in the
same way as for magnocellular neurons, but the results were qualitatively different. Typical results from one L-on center and one
M-off center neuron are shown in Figures
5-7. The two neurons were recorded from
the same penetration through the LGN: the off-center neuron from the
contralateral eye, near the top of the LGN (presumably layer 6), and
the on-center neuron from the ipsilateral eye, 1.85 mm further ventral
(presumably layer 3).

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Figure 5.
Spatial weighting functions and radial weighing
functions of two parvocellular neurons as measured with
L-cone-isolating, M-cone-isolating, and luminance-modulated stimuli
(conventions are as in Fig. 2). A, L-on/M-off neuron,
9° eccentric. The on-center/off-surround luminance response was used
to define the receptive field center, outlined in white
(see Materials and Methods). Note that neither the center cone type
(L) nor the surround cone type
(M) exhibits center/surround opponency
(Fig. 1, arrow). B, M-off/L-on neuron,
11° eccentric. Although the signatures of the L-cone and M-cone
responses are the same as in A, the M-off response
dominates. Total region shown, 1.0° on a side; pixel size, 7.5 min.
Delay between stimulus and response, 15-44 msec, the sum of the 15-30
and the 30-44 msec bins (see Materials and Methods). Because the
luminance weighting function was much weaker than L-cone and M-cone
weighting functions, it was multiplied by a factor of 2.0 to increase
visibility. Conventions are as in Figure 2.
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The sign of the dominant cone in parvocellular cells was judged from
the luminance response. The luminance responses also were used to
define the center regions (outlined in white; see Materials and
Methods). For instance, the neuron that yielded the data in Figure
5A was an on-center neuron as mapped with white light. The
L-cone response was on in both center and surround, so we concluded
that the L cone was the cone type that caused the on response of the
center. The M-cone input to this neuron was off in both center and surround.
The examples shown are typical in that there were almost always 3-5
pixels in the centers of parvocellular neurons. For the most common
pixel size (7.5 min) this corresponds to ~1-2 times the typical
diameter of receptive field centers, as measured in other studies at
similar eccentricities and through the optics of the eye [for
instance, Lee et al. (1998)
,
c = 2-4 min;
note that, for a difference-of-Gaussians model, the diameter of the center up to the zero crossing is ~4-6 times the commonly quoted parameter for center size, its radius,
c].
These sizes are large compared with the anatomical spreads of the
dendrites of midget bipolar and midget ganglion cells that presumably
constitute the retinal input to these neurons. They are also large
compared with the local inhomogeneities of the cone mosaic measured
recently in macaque and human retina (Roorda et al., 2001
). Possible
reasons for the comparatively large receptive field centers could be
optical spread and/or neuronal coupling. That the macaque's
physiological optics in large part determines the observed center sizes
of parvocellular neurons is consistent with recent measurements of
McMahon et al. (2000)
. They used laser interferometry to bypass the
optics of the macaque's eye and observed higher spatial resolution of
parvo-projecting ganglion cells than was measured through the natural
optics. However, for the purposes of this paper the important issue is,
can we resolve the center and surround through the natural optics? As evidenced in Figure 5, for example, the answer to that is affirmative.
The neuron for the data in Figure 5B was an off-center cell
as mapped with white light; in this case the off input from the M cones
dominated the response of the center. Note that both parvocellular neurons in Figure 5, A and B, received only on
input from the L cones and off input from the M cones; they both were
excited by red light and inhibited by green. The signature of the
luminance response in the center, and also in the surround, was
determined solely by the relative weight of the antagonistic L and M inputs.
It is remarkable that in these data we see no evidence for
center/surround antagonism within a single cone type, although center/surround antagonism is observed in the luminance responses. This
bears on the debate concerning mixed versus cone-specific surrounds
(Wiesel and Hubel, 1966
; Shapley and Perry, 1986
; Lennie et al., 1991
;
Reid and Shapley, 1992
; Lee et al., 1998
). In Figure 1, it is shown
that center/surround antagonism within a single cone type is the key
test for distinguishing cone-specific versus mixed input to the
receptive field surround. Let us consider for the neuron in Figure
5A how center/surround antagonism arises in the luminance
responses although there is none in its L- or M-cone-isolated
responses. The biggest response from either L or M cones is
concentrated in a small number of pixels (outlined in white
in the Fig. 5) in the center of the receptive field. The L-cone
response is somewhat stronger in driving the center of this neuron, so
when white light is used and drives the L and M cones equally, the
L-cone on response predominates and the neuron is on-center. However,
the L-cone spatial weighting function declines more steeply with
position than does that of the M cone; thus the off response of the M
cone predominates in the surround region when luminance stimuli are
used. The data for the neuron in Figure 5B are similar
except that for this neuron the stronger signals in the center came
from the M cone, and the stronger signals in the surround came from the
L cone. Data like those in Figure 5, A and B,
suggest a high degree of specificity of cone functional connections to
parvocellular neurons. They also confirm directly, for parvocellular
neurons, the DOG model (Rodieck, 1965
; Enroth-Cugell and Robson, 1966
)
of center/surround antagonism. In this model the center/surround
receptive field is a result of the summation of two opposed spatial
mechanisms that both have peak sensitivity in the center of the
receptive field but that have different spatial spreads.
Parvocellular movies: spatiotemporal weighting functions
The nature of cone-cone interaction is such a central issue for
understanding primate color vision that we studied it further by using
dynamic measurements in parvocellular neurons. Representative response
movies of parvocellular neurons are shown in Figure
6, A and B, from
the same neurons that yielded the data snapshots in Figure 5,
A and B. Each row is from a given time offset as marked in the figure. As in the peak responses illustrated in Figure 5,
A and B, the cone responses in these
parvocellular neurons are of one sign at each particular time. For
instance, in Figure 6A at both 15-30 msec and also
from 30-44 msec, the L cone responses are all on, and the M cone
responses are all off. The on-center/off-surround structure of the
luminance response arises because L-cone excitation predominates in the
center, whereas the M-cone input is slightly stronger in the surround.
Later in time there is a zero crossing and change in sign of response
(the rebound), as can be seen for both cells (Fig.
6A,B). The peaks, zero crossings, and rebounds of the
center responses lead those of the surround. It is worth noting that
the zero crossings and rebounds occur later in time for
parvocellular compared with magnocellular neurons; this probably reflects differences in retinal postreceptoral processing in the two
parallel pathways.

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Figure 6.
Spatiotemporal weighting functions of the same two
parvocellular neurons (Fig. 5). A, L-on/M-off neuron.
B, M-off/L-on neuron. Conventions are as in Figure
3.
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Parvocellular center and surround temporal weighting functions
A second way to evaluate the degree of cone specificity in the
parvocellular pathway is to examine the temporal weighting functions of
the separate cone inputs to center and surround, as done earlier for
the magnocellular neurons. The temporal weighting functions in Figure
7 represent the dynamics of the responses of the parvocellular neurons from Figures 5 and 6. Each row is for a
single neuron: the upper row is for the L-on/M-off neuron of Figures
5A and 6A, whereas the lower row is for
the M-off/L-on neuron of Figures 5B and
6B. Note the opposite sign of cone-specific signals
(L, positive; M, negative) in both the center (thick lines) and in the surround (thin lines). Also, the relative
strength of center and surround cone-specific responses can be
appreciated. It is most important that the center cone type (the L cone
in Fig. 7A; the M cone in Fig. 7B) has a stronger
response in the center and a weaker but same-sign response in the
surround. The surround cone type (the M cone in Fig. 7A; the
L cone in Fig. 7B) has peak sensitivity in the center but is
relatively stronger in the surround and also does not change sign
between center and surround. The antagonistic surrounds, which might
appear noisy at any given pixel in the spatial or spatiotemporal plots
(Figs. 5, 6), are quite robust in the temporal weighting functions in Figure 7, which are averaged over many pixels.

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Figure 7.
Temporal weighting functions of the same two
parvocellular neurons (Figs. 5, 6). A, L-on/M-off
neuron. Note that the L-cone response is on in both the center
(thick line) and in the surround (thin
line), but the center response is stronger. The M-cone response
is off in both regions, but the surround is stronger. The opposite
relationships between center and surround hold for the M-off/L-on
neuron (B). Conventions are as in Figure 4.
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Blue-yellow opponent receptive field
Four neurons in our sample responded robustly to an
S-cone-isolating stimulus. Three of these were blue-on cells; they had S-on responses that were antagonized primarily by L-off responses, whereas responses to the M-cone stimulus were weak or negligible. In
each of these cells the spatial extent of the L-off response was
smaller than that of the S-on response. We nonetheless call these
neurons S-on/L-off (rather than L-off/S-on) for consistency with the
usual nomenclature: blue-on/yellow-off. In Figure 8, we show the
spatial weighting functions of one such neuron, as measured with L-,
M-, and S-cone stimuli, as well as a 100% contrast luminance stimulus.
The L-off response for this cell spans a region of ~0.38° (3 pixels). The S-on responses are distributed over a considerably larger
region, almost 1°. Consequently, the measured luminance responses
appear off-center/on-surround. The receptive field structure attributable to the M cones is perhaps on-center (at only 1 pixel) but
predominantly off in the surround, but the responses are much weaker
than those attributable to the other two cone types. The large area of
S-cone input was noted in studies of S-on cells in the retina (small
bistratified cells) (Zrenner and Gouras, 1981
; Dacey and Lee, 1994
;
Chichilnisky and Baylor, 1999
), although most studies report that the
antagonistic inputs from L and M cones are equal in size. Although we
find differently, our small sample does not permit us to draw strong
conclusions from this difference. Further, chromatic aberration in the
optics of the eye could play a role in these measurements (Flitcroft,
1989
). We focused the eyes to maximize the responses of red-green
opponent parvocellular cells to achromatic gratings, so the stimuli
that drive S cones may have been defocused.
The S-on neuron illustrated here (Figs.
8, 9) was
recorded 135 µm below the parvocellular neuron for which the
responses are illustrated in Figures 5A-7A,
which was in the second layer that was encountered driven by the
ipsilateral eye. It was therefore probably near the bottom of
parvocellular layer 3. Although histological analysis was not
performed, this location is consistent with other work in which neurons
with S-cone input were found in the middle two intercalated layers,
located between the two ventral parvocellular layers (4 and 3) and
between the parvocellular and magnocellular divisions (layers 3 and 2)
(Hendry and Reid, 2000
) (also see Schiller and Malpeli, 1978
; Martin et
al., 1997
). A second S-on neuron was found 300 µm below this one.

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Figure 8.
Spatial weighting functions and radial weighing
functions of an S-on/L-off neuron (12° eccentric, recorded at the
bottom of the parvocellular layers), as measured with L-, M-, and
S-cone-isolating and luminance-modulated stimuli. Total region shown,
1.25° on a side; pixel size, 7.5 min. Delay between stimulus and
response, 15-44 msec, the sum of the 15-30 and the 30-44 msec bins
(see Materials and Methods). The luminance weighting function was
multiplied by 2.0 to increase visibility. Conventions are as in Figure
2.
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Figure 9.
Spatiotemporal weighting functions of the same
S-on/L-off neuron (Fig. 8). Conventions are as in Figure
3.
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The spatiotemporal weighting functions for this S-on/L-off neuron
illustrate a feature that was characteristic of the three blue-on cells
we recorded. In both the magnocellular and the red-green opponent
parvocellular neurons, the center mechanism is significantly faster
than the surround. In the cells with S-on input the S-cone input spans
a larger region (so we have called it the surround), but its time
course is faster than the L-off input to the center. At delay of 15-30
msec the S-on response is robust, but the L-off response is barely out
of the noise. Note that this initial phase of the S-cone response is as
fast as the center responses in the red-green opponent parvocellular
neurons (Fig. 6). The S-on response has a weak rebound (see Zrenner and
Gouras, 1981
) that begins at a delay of between 59 and 74 msec. By
contrast, the L-cone rebound begins at 89 msec and is weaker yet. These
differences in the dynamics of S-cone and L-cone inputs lead to the
unusually prolonged off response of this neuron to a luminance
stimulus. At short delays (30-59 msec) the luminance-off response is
caused by the L-off response; at later delays (59-74 msec) it is
caused by the rebound from the S-on response. These qualitative
features of the dynamics of the blue-on cell are best appreciated in
the temporal weighting functions (Fig.
10E).

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Figure 10.
Temporal weighting functions for all red-green
opponent parvocellular neurons (A-D) and
S-cone-dominated neurons (E, F). For each cell
type three or four sets of temporal weighting functions are plotted
separately for both center (top) and surround
(bottom); L-cone, M-cone, luminance, and, for some
cells, S-cone responses are shown. For each cell all weighting
functions are normalized by the same value. Red-green responses are
normalized by the peak of the center response for the center cone type
(L cone in A, B; M cone in C, D).
S-on/L-off responses (E) are normalized by the
S-cone surround peak (which was stronger than the S center). S-off
responses (F) are normalized by the S-cone
center. Data from four neurons that gave the weakest responses
[normalization value <3.0 (spikes/sec)/(unit contrast)] are plotted
in gray. Note that for red-green neurons the center
cone types (L cone, A, B; M cone,
C, D) have the same sign responses in the
center and surround (with only two clear exceptions, shown by
arrows). The luminance responses, however, have opposite
signs in the center and surround.
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Population studies: temporal weighting functions for receptive
field center and surround
The spatial and temporal weighting functions for receptive field
center and surround presented above are for typical examples of
magnocellular and parvocellular neurons. We now present several figures
that display quantitative features of the cone maps in the population
of LGN cells that were studied. First we display the temporal weighting
functions of center and surround, introduced in Figures 4 and 7.
The temporal weighting functions illustrate the relative
magnitudes of cone inputs and also their dynamics. Because of the
controversy concerning the composition of the parvocellular surround,
the temporal weighting functions of the four classes of red-green
opponent neurons are presented first.
L-on/M-off cells
The temporal weighting functions of all nine L-on/M-off cells
(Fig. 10A) were quite consistent; with only one exception, the cone-isolated responses had the same sign in center and surround. That
is, L-cone responses were on everywhere and M-cone responses were off
everywhere. For one cell of nine (Fig. 10A,
arrow) the L-cone response changed sign in the surround and
so showed a pronounced off response. This is one of only two examples
we found of spatial antagonism for a cone-isolated response: the
hallmark of a mixed surround. For all other cells the magnitudes of the
L-cone responses in the center were stronger than in the surrounds, but
the M-cone responses were similar in both center and surround. This
resulted in the dominance of the L-on responses in the center and the
M-off responses in the surround.
L-off/M-on
The temporal weighting functions of the eight L-off/M-on neurons
(Fig. 10B) were also quite consistent, again with only one outlier. As a rule, cone-isolated responses had the same sign throughout the receptive field, and L-cone signals were opposite in
sign to M. In the center the L-off responses were stronger than the
M-on. In the surround the M-on response was stronger than the L-off.
The only exception (marked with an arrow, Fig. 10B) showed spatially antagonistic input from the L
cone. This cell was encountered in the same penetration as the
exceptional, mixed surround cell in the L-on/M-off group (above), but
in a different parvocellular lamina 1.3 mm ventral.
For the other seven L-off/M-on neurons (Fig. 10B) the
dynamics of the L-off responses should be noted. Although the initial response was L-off in the surround (Fig. 10B,
bottom), this L-off response was less sustained than in the
center (Fig. 10B, top). This effect is
hard to discern when the responses of all cells are superimposed on
separate plots of center and surround (as in Fig.
10B), but it is quite evident when center and
surround for each cell are plotted on a single axis (as seen in Fig. 7; analysis not shown). It is possible that this relative transience could
have been attributable to an L-off center partially superimposed with a
weak L-on surround in many of these cells, which would mean they had a
mixed surround. To test this possibility, we examined the temporal
weighting functions of annuli, starting at different distances from the
center. At no distance from the center were the transient L-off
responses converted to L-on responses. In other words, at no distance
from the center were responses elicited from the L cones that were
opposite in sign to the L-off responses in the center. Therefore, the
hypothesis of a mixed surround was not supported by these data.
M-on/L-off and
M-off/L-on
The temporal weighting functions of all 10 M-cone-dominated cells
(Fig. 10C,D) showed no positive evidence of a mixed surround. Specifically, center/surround opponency was not seen in their M-cone
responses. Of the four classes of red-green opponent neurons, M-on/L-off cells (Fig. 10C) received the most balanced
input from the L and M cones to the center. The luminance responses
(with one exception) were therefore weak. In three cases an
antagonistic surround could not be demonstrated in the luminance
responses (Fig. 10C, bottom right); therefore,
strong arguments cannot be made for the cone composition of the
surround in these cells (if indeed there was one; see Fig.
15D). In the M-off/L-on cells (Fig. 10D),
however, overt spatial opponency was seen clearly in the luminance
responses, but never in the M-cone responses.
S-on and S-off
The temporal weighting functions of the three cells that received
S-on input (Fig. 10E) were all quite similar. As noted for Figure
9, the responses of the S-on neurons had particularly weak rebounds.
Further, as was the case for the cell illustrated in Figures 8 and 9,
the region of S input was always larger than the region of antagonistic
off input, which was dominated by the L cone. Their receptive fields as
mapped with luminance stimuli (far right column here
and in Figs. 8, 9) therefore all appeared off-center/on-surround. The
only cell we found that received S-off input (Fig.
10F) was quite different in character. The responses were quite weak, on the order of 2 (spikes/sec)/(unit contrast), and
were dominated almost entirely by the S cone, both in the center and in
the nonantagonistic surround.
Magnocellular
Finally, the temporal weighting functions for the on-center (Fig.
11A) and off-center
magnocellular neurons (Fig. 11B) were very consistent
within each class but quite different from those of parvocellular
neurons. In the centers the M and L-cone responses were both of the
same sign (although the L-cone responses were stronger); in other
words, there was no red-green opponency. In most cases, however, the
single-cone inputs (both L and M) as well as the luminance responses
were spatially opponent. Contrary to what we found for parvocellular
neurons, single-cone maps were usually center/surround antagonistic.
The exceptions were three on-center cells that were predominantly M-on
in both the center and surround. Because the surrounds of these cells
were also L-off, the surrounds were color-opponent (see Figs.
14B, 16B).

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Figure 11.
Temporal weighting functions for all
magnocellular neurons. For each cell type three or four sets of
temporal weighting functions are plotted separately for both center
(top) and surround (bottom); L-cone,
M-cone, luminance, and, for some cells, S-cone responses are shown. For
each cell all weighting functions are normalized by the same value, the
peak of the luminance response.
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Sustained and transient dynamics
The dynamics of the parvocellular temporal weighting functions in
Figure 10 are interesting because they differ from magnocellular temporal weighting functions in having a smaller rebound compared with
the peak response. This is important because the relative strength of
the rebound is related directly to the transience of the response to a
step stimulus (Gielen et al., 1982
; Usrey et al., 1999
; De Valois et
al., 2000
; Usrey and Reid, 2000
). The integral of a temporal weighting
function should be approximately equal to the sustained component of
the step response. For magnocellular neurons the integrals of the
temporal weighting functions are near zero, but for parvocellular
neurons they are not. By comparing the data for parvocellular and
magnocellular neurons in Figures 10 and 11, one observes that the
different dynamics are present in the cone-isolated responses as well
as in the responses to achromatic stimuli. To make this observation
more quantitative, we devised a measure of sustained-ness intended to
approximate the sustained firing rate of the step response divided by
its peak firing rate. The sustained component is the ratio of the area
under the temporal weighting function integrated over its entire
duration (0-222 msec, or 15 stimulus frames) divided by the area under
the waveform up to the first zero crossing. For temporal weighting
functions that are monophasic with no undershoot, the sustained
component is 1. For temporal weighting functions that are biphasic and
for which the rebound exactly cancels the initial peak, the sustained
component is 0. Figure
12A is a histogram of
the distribution of the sustained component across our population of
macaque LGN units in response to luminance m-sequences, and it is
consistent with the well known distinction between parvocellular and
magnocellular neurons as sustained and transient, respectively (Dreher
et al., 1976
; De Valois et al., 2000
). The distribution falls into
three distinct clusters: magnocellular neurons with sustained component
near 0, red-green opponent parvocellular neurons with sustained
component near 0.5-0.6, and S-cone-driven neurons (although few in
number) with sustained component near 0.9 (see Zrenner and Gouras,
1981
). Figure 12B displays the novel result that the
same tripartite distribution of sustained-ness is observed in responses
to cone-isolating m-sequences for the dominant cone type (L cone for
magnocellular; the center cone type, L or M, for red-green opponent
parvocellular; and the S cone for blue-on cells). This implies that the
degree of sustained-ness or transient-ness is not caused by subtraction
of the signals of the cones in response to achromatic patterns but,
rather, must be a result of different temporal filtering in the retinal
circuitry that drives the parvocellular and magnocellular neurons in
parallel.

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Figure 12.
Histogram of the sustained component (see
Results) of all magnocellular neurons, red-green opponent
parvocellular neurons, and blue-on cells. A, Responses
to luminance stimuli. B, Responses to cone-isolating
stimuli for the dominant cone type (L cone for magnocellular, center
cone for red-green parvocellular, S cone for blue-on). The three
populations were nonoverlapping, whatever the stimulus type.
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Relative weights of cone mechanisms in the center and surround
across the population of LGN cells
To compare the amplitude of the single-cone responses across the
population of LGN cells, we compressed the temporal weighting functions
of center and surround to a single number: the strength of response
attributable to each of the cone classes (or to the achromatic
stimuli). These strengths were calculated by integrating the initial
portions of the temporal weighting functions up to the first zero
crossing that followed the peak. Because surround responses were
generally slower than center responses, integrating the center and
surround separately provides a more valid measurement of their relative
strength than would be obtained by considering static spatial weighting
functions (as seen in Fig. 5). Six different cone strengths were
determined: the strengths of L, M, and S both for the center
(cl, cm,
cs) and for the surround
(sl, sm,
ss). Also, the data allowed us to calculate the
total strength of the achromatic (luminance) responses to center and
surround, ca and sa.
Finally, we defined the total strength t as the sum of the center and surround strengths, for instance:
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To compare the relative contribution of the three cone classes on
a single plot, we normalized each response strength by the sum of the
absolute values of all three, following Derrington et al. (1984)
. We
refer to these normalized cone strengths as cone weights. For instance,
the L-cone weight to the center is given by:
By definition, the sum of the absolute values of the weights
( Cl, Cm, and
Cs) is 1.0. If two of the three are plotted
against each other, the absolute value of the third can be inferred. As in Derrington et al. (1984)
, Cm has been plotted
versus Cl in Figure
13. The distance from each point to the
diagonal borders of the figure gives the absolute value of the S-cone
weight (points outside the borders indicate cells for which no S-cone
measurements were made).

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Figure 13.
Scatter plots of normalized cone weights,
following Derrington et al. (1984) , plotted for all neurons recorded in
parvocellular layers. Shown are M-cone weights plotted versus L-cone
weights, in which magnitudes of S-cone weights are determined by the
distance from diagonal lines. Points near
the diagonal lines are from cells that received
negligible S-cone input. Points for which no S-cone
measurements were performed are plotted outside the diagonal
lines. Symbols signify the eight classes of
cells. Antagonistic L-cone versus M-cone responses are in the second
(II) and fourth (IV)
quadrants. Nonantagonistic (mixed) responses are in the first
(I) and third (III)
quadrants. Each class clusters distinctly in the plot of
Center weights (A), but less so in
plots of Surround (B) and
Total (C) weights. The two cells
that had clear mixed surrounds (Fig. 10A,B) are
indicated with arrows (B).
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Note that the cone weights of the centers of the four types of
red-green opponent parvocellular neurons clearly are clustered (Fig.
13A). The neurons excited by green (M-on/L-off and
L-off/M-on) are found on the border in the second quadrant. The tick
mark on this border indicates the position at which the L and M cone weights are equal and opposite: Cm = 0.5;
Cl =
0.5. Points for the M-on/L-off neurons
cluster above the tick mark; those for the L-off/M-on neurons cluster
below the tick mark. Neurons that were excited by red (L-on/M-off and
M-off/L-on) cluster on the border in the fourth quadrant. Again, the
tick mark segregates the on-center from the off-center neurons.
Finally, points for the three S-on neurons all fall near the
x-axis. This indicates that the M-cone input to the
antagonistic mechanism was quite weak.
The plot of cone weights for the receptive field surrounds (Fig.
13B) addresses the question of whether the surround is
cone-specific or mixed. Most points for the red-green parvocellular
neurons (circles and squares; see legend) fall in
the second and fourth (cone-opponent) quadrants. This is evidence in
favor of a cone-specific surround, because if the surround were mixed,
one would expect the cone weights of the surround to be the same sign
(first and third quadrants). The only two clear exceptions are marked
with arrows, as they are in Figure 10, A and B.
Three other points for L-center cells fall in the "nonopponent"
first and third quadrants of Figure 13B, but near the
y-axis, where the L-cone weight is almost zero. We think
that these data points are not positive evidence for the mixed surround
hypothesis, however, because they correspond to cases in which the
L-cone surround responses were simply weak and noisy (see Fig.
15A, specifically the three points near the
x-axis).
Figure 13C shows the plot of M-cone versus L-cone weights
integrated over the entire receptive field. It represents the predicted cone weights that would be obtained with stimuli larger than the receptive field. This is equivalent to the similar plot in Derrington et al. [(1984
), their Fig. 6] and shows a similar result: red-green opponent neurons cluster in the second and fourth quadrants with approximately equal and opposite weights.
Plots of the L and M cone weights for the magnocellular neurons in our
sample (Fig. 14) demonstrate that the
receptive field center receives mixed, synergistic L- and M-cone input
(Fig. 14A), as does the surround in most cases (Fig.
14B). In three cases, however, the surround in fact
received antagonistic L- and M-cone input (Fig. 14B),
as indicated by points in the second quadrant. These exceptions, all
on-center neurons [perhaps the type IV cells of Wiesel and Hubel
(1966)
], in fact received antagonistic L-off and M-on inputs in the
surround. Weakly opponent cone weights (points in the second and fourth
quadrants near one of the axes) were yet more common for the total
responses (the sum of the center and surround; Fig. 14C).
These results are consistent with the findings of Smith et al. (1992)
(see also Schiller and Colby, 1983
; Derrington et al., 1984
; Lee et
al., 1989
), who demonstrated cone-opponent responses in the surrounds
of magnocellular cells.

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Figure 14.
Scatter plots of normalized cone weights for
magnocellular neurons, as in Figure 13. On-center cells are indicated
by symbols with light centers; off-center
cells are indicated by symbols with dark
centers.
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Strengths of cone inputs to center and surround across
the population
Because center and surround are considered separately in the cone
weight plots, Figures 13 and 14, it is impossible to compare them for
any given cell. Furthermore, all magnitudes in Figures 13 and 14 are
relative, so response strengths cannot be appreciated. Therefore, in
Figure 15 we plot the strengths of the
surround versus the center responses for the entire population of
parvocellular neurons that we studied. In this figure, points in the
second and fourth quadrants indicate opponent center/surround
interactions: on-center/off-surround in the fourth quadrant;
off-center/on-surround in the second quadrant. Points plotted in the
first and third quadrants indicate that the center and surround had the
same sign of response. These plots illustrate that red-green
parvocellular neurons generally had spatially opponent receptive fields
when mapped with luminance stimuli (Fig. 15D), but the
centers and surrounds had the same sign of response when the cells were
driven with L-cone- and M-cone-isolating stimuli (Fig.
15A,B, with two exceptions shown by arrows).

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Figure 15.
Scatter plots of response strengths (not
normalized) in the surrounds versus the centers for L-cone
(A), M-cone (B), S-cone
(C), and luminance responses
(D) in units of spikes/(sec · C), where C is the cone contrast of the
stimulus. Data are shown for all neurons recorded in parvocellular
layers; the symbols are as in Figure 13. Antagonistic
center/surround responses fall in the second and fourth quadrants;
nonantagonistic responses fall in the first and third quadrants (see
insets). With few exceptions, all luminance responses
(D) had antagonistic centers and surrounds. Most
L-cone responses (A) and all M-cone responses
(B) had nonantagonistic centers and surrounds
(exceptions are indicated with arrows in A,
as in Figs. 10, 13).
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In a past report with an overlapping data set, we reported that more
than one-third of parvocellular neurons were spatially nonopponent
(type II cells) when measured with luminance stimuli (Reid and Shapley,
1992
); here we instead found center/surround opponency (type I cells)
in 23 of 27 cases (Fig. 15D). The difference is that here we
considered independently the temporal weighting functions of center and
sur