Department of Visual Science, Institute of Ophthalmology,
University College London, London EC1V 9EL, United Kingdom
 |
INTRODUCTION |
A number of studies have
identified suppressive influences that reduce the responses of neurons
in primate V1 when areas of visual space surrounding the classical
receptive field are stimulated (Born and Tootell 1991
;
Kapadia et al. 1999
; Knierim and Van Essen 1992
; Nothdurft et al. 1999
; Sceniak et
al. 1999
; Sillito et al. 1995
). Some have
reported these surround influences to be restricted to cells in the
upper layers of V1 only (Born and Tootell 1991
), although a recent study of the effect of contrast on spatial summation in V1 neurons (Sceniak et al. 1999
) would suggest that
common mechanisms may apply through all cortical layers. Indeed this latter study suggests that surround effects can be explained in terms
of a difference of Gaussians model with overlapping Gaussians for the
inhibitory and excitatory fields centered on the same point. In this
sense, the mechanism underlying surround suppression would be an
integrated component of the classical receptive field, and terms such
as center and surround mechanisms become rather misleading. However, it
seems likely that several mechanisms would have to underlie both the
excitatory and the inhibitory Gaussians, and their interaction may not
be linear and may depend on the spatial organization of the stimulus.
For example, a layer 4 cell would receive direct thalamic input and
horizontally linked intracortical excitatory connections together with
inputs from cells in the underlying layer 6 (Ahmed et al.
1994
; Callaway 1998
; Ferster and
Lindstrom 1985a
,b
; Peters et al. 1994
). Present
evidence suggests the synaptic efficacy of these different components
of the excitatory input could be quite different (Ferster and
Lindstrom 1985a
,b
; Stratford et al. 1996
).
Likewise a range of inhibitory processes will provide both a direct
influence on individual cells and an indirect effect via their
influence on the cells driving the intra-cortical facilitation. The
potential dynamic complexity of these interactions is underlined by the
work of Kapadia et al. (1995
, 1999
) in primates. Experiments in area MT have also reported suppressive surrounds of
varying degrees of complexity with an organization that may encompass
local to local motion comparisons and the extraction of complex
features of the visual environment (Raiguel et al. 1995
;
Xiao et al. 1995
, 1997a
,b
). This raises
the possibility of a complexity to the organization of surround
mechanisms in V1 that go beyond that predicted from an overlapping
Gaussians model. In particular, the feedback from MT to V1 raises the
possibility of complex motion-dependent effects drawing on the
influence of MT. Thus following from our earlier report of surround
driven suppressive and facilitatory effects in primate V1
(Sillito et al. 1995
), we have utilized drifting stimuli
to make a detailed examination of the strength, spatial organization,
direction dependence, and laminar distribution of surround suppression
in an attempt to further characterize the way in which it is
implemented. The stimuli we have used here were all effective in
driving MT cells (in some of these experiments we made simultaneous
recordings in MT) (H. E. Jones, W. Wang, T. E. Salt, and A. M. Sillito, unpublished data) and also enabled comparison
with a number of other studies in MT and cat and primate V1. Our data
here suggest a much stronger influence of surround suppression through
all laminae than hitherto reported in primate V1, clear dependency on
the relative direction of motion for the surround stimulus and two
distinct patterns of bias to the spatial organization underlying the
suppressive mechanisms. These observations are discussed in the context
of the insight they suggest into the processing mechanisms pertaining in V1.
 |
METHODS |
Subjects
The experiments were carried out on 14 adult Macaca
mulatta monkeys. The animals were treated according to the
published guidelines on the use of animals in research (European
Communities Council Directive 86/609/EEC) and the National Institutes
of Health guidelines for the use of laboratory animals.
Animal preparation
Animals were initially premedicated with atropine sulfate (0.04 mg/kg im) and acepromazine maleate (0.05 mg/kg im). Anesthesia was
induced with intramuscular injection of ketamine (10-15 mg/kg). Surgical procedures were carried out under ketamine anesthesia, and a
solution of bupivicaine hydrochloride (0.75% wt/vol) was applied to
all wound margins. After cannulation of the saphenous veins and
trachea, the animal was transferred to a stereotactic frame. The ear
bars of the stereotactic apparatus were coated with lignocaine
hydrochloride gel. The dura overlying V1 was exposed via a craniotomy.
Anesthesia was maintained throughout the course of the experiment
either with halothane (0.1-0.4%) or sufentanil (4-8 µg · kg
1 · h
1) and a
mixture of 70% N2O and 30%
O2. End-tidal CO2 levels,
the electrocardiogram (ECG) waveform, intersystolic interval, and the
frequency of spindles in the electroencephalogram (EEG) waveform were
monitored at all times through the experiment. The rate and depth of
artificial ventilation was adjusted to maintain end-tidal CO2 at 3.8-4.2%; after completion of all
surgical procedures, the level of anesthetic agent was adjusted to give
a state of light anesthesia. Once a stable state was reached, any
variation in the monitored parameters (change in the frequency of
spindles, fall or fluctuation in intersystolic interval, rise in
end-tidal CO2) commensurate with a change in the
depth of anesthesia was immediately compensated for by an increase in
the level of anesthetic reagent. Following completion of all surgical
procedures and after a stable state of anesthesia had been established,
animals were immobilized with an infusion of vecuronium bromide (0.1 mg · kg
1 · h
1) in glucose-enriched lactated Ringer
solution. Temperature was maintained at 38°C by use of a
thermostatically controlled electric heating blanket. All wound margins
were dusted with topical application of Neomycin sulfate and Noricillin
[procaine penicillin (15 mg/kg) and benzathine penicillin (11.25 mg/kg)im] was administered daily. Dexamethasone (1 mg/kg iv) was
administered daily to reduce cerebral edema.
The pupils were dilated and accommodation paralyzed with topical
application of atropine methonitrate (2% wt/vol). The eyes were
protected with gas permeable contact lenses, and brought to focus on a
semi-opaque tangent screen/front surface mirror at a distance of 0.57 or 1 m, using supplementary lenses and 2-mm diam artificial
pupils. The locations of the blind spot and fovea were located and
plotted using a reversible ophthalmoscope.
Apparatus
Single-unit activity was recorded from area V1 using arrays of
tungsten in glass microelectrodes (Merrill and Ainsworth
1972
). Electrode penetrations were angled to avoid recording
from locations underlying the array entry point. Data were collected
and visual stimuli generated using the Cambridge Electronic Design
(Cambridge, UK) VS system in conjunction with a Picasso Image
Generator (John Daughman, USA), presented on a Tektronix 608 tube. For
further details, refer to Sillito et al. (1993)
. Spikes
were stored with a 0.1-ms interval resolution and could subsequently be
processed with respect to any aspect of the stimulus variables used
during data collection. We first identified and hand mapped receptive fields using an overhead projector and the tangent screen of a plotting
table. Once the receptive fields had been characterized in this way, we
introduced a 45° front-surfaced mirror into the light path,
deflecting the animal's plane of vision to a vertically mounted, 608 Tektronix tube at a distance of 0.57 or 1 m for controlled presentation of visual stimuli. The 608 tube was mounted on a cradle
that could be shifted over a set of floor mounted tracks and tracks
mounted in a slave carrier to roughly center the display on one of the
receptive fields. We utilized the alignment of the receptive field on
the tangent screen and 45° beam splitter to achieve this. We could
fine tune the centering of the receptive field on the 608 tube using
micrometer adjustments on the carrier mechanisms and software
adjustment of the display center. These adjustments were checked with
reference to the magnitude of the responses generated either by small
flashing spots or small patches of an optimally oriented drifting
sinusoidal grating presented in a range of spatial locations forming a
sequential grid over the field. Accurate centering of the display
over the receptive fields studied was critical to our
experiments, and so the fine tuning of the centering was a
standardized procedure for every cell and was checked throughout data
gathering sequences.
Visual stimuli
For the preliminary evaluation of cell response properties, we
used simple visual stimuli comprising flashing spots, drifting bars,
and patches and annuli of drifting sinusoidal gratings. Parameters such
as spatial frequency, temporal frequency, orientation, and bar length
or spot/patch diameter were varied in a randomly interleaved sequence.
A blank stimulus was included in each block for the assessment of
spontaneous activity levels. The contrasts (Lmax
Lmin)/(Lmax + Lmin) routinely used were in the
range 0.1-0.36 with a mean luminance of 14 cd
m
2. To explore the effects of direction
contrast on patch suppression, we used concentric bipartite sinusoidal
gratings centered over the receptive field. We kept the contrast,
spatial frequency, and drift rate constant in both inner and outer
stimuli but varied the direction of drift of the inner and outer
stimuli. The phase of our inner and outer displays were locked together
with reference to the center of the display so that for concentric
stimuli, when the direction of drift of both components was the same,
they appeared as a single grating. Central patch size and inner
diameter of the outer field ranged between 0.3 and 6.0°. Spatial
frequency was in the range 1-4 cycles/° (cpd) and drift rate was
1.0-4.0 Hz. All tests were done with monocular visual stimulation of
the cell's dominant eye.
To examine the spatial location of suppressive zones, we used two
square patches of optimally oriented sinusoidal grating. The gratings
drifted within each patch, and spatial frequency, direction of motion,
and drift rate were kept constant in both patches. One grating patch
(the notional inner stimulus) was centered over the CRF while the
second stimulus patch was presented in randomized sequence at a range
of locations around the field. Central and outer patch sizes ranged
from 0.5 to 2°. For some cells, we also explored the effect of
reversing the direction of drift of the grating in the second patch.
Experimental protocol and analysis
PRELIMINARY EVALUATION OF RECEPTIVE FIELDS.
Isolated single units were classified as simple or complex according to
conventional criteria (Hubel and Wiesel 1962
;
Skottun et al. 1991
). After the receptive field center
had been localized as described in the preceding text, we
quantitatively checked preferred orientation and direction of motion
using a patch of sinusoidal grating localized over the receptive field
center with orientation and direction of drift varied in a randomized
and interleaved sequence.
MAPPING THE CLASSICAL RECEPTIVE FIELD.
Because of the way the mechanisms driving center and surround
mediated influences overlap in primate V1, it is difficult to define
what is precisely meant by the term classical receptive field. It might
be taken to include the spatial borders of the processes driving
surround effects, but these are often difficult to define. Equally the
area of visual space from which excitatory responses can be obtained
may not define the extent of the excitatory mechanism or excitatory
field because the underlying inhibitory mechanism may suppress the
weaker excitatory influences. In this study, we have used the term
classical receptive field, CRF, to indicate the area of visual space
from which excitatory responses, as judged by the spiking activity of
the cell, could be obtained. The precise measurement is influenced by
the procedure used to map the field.
We determined the precise location and spatial extent of the CRF using
four procedures and took the value for the CRF size from the procedure
giving the largest measurement. This avoided the potential danger of
underestimating the size of the CRF (Sengpiel et al.
1997
; Walker et al. 2000
). First, we explored
the spatial distribution of locations from which a contrast modulated
patch or a patch of optimally oriented drifting grating elicited
responses (we termed this the XY patch method). A variety of patch
sizes from 0.2 to1.0° were used for this test. They were presented in a randomized sequence over a set of spatial locations defined in
rectangular coordinates. The location giving the largest response was
used to define the CRF center, and the coordinates of our display were
adjusted to match CRF center and display center. This involved several
iterations with variations of patch size and display coordinates to
optimize both centering and assessment of CRF dimensions. The data from
all the test runs in these procedures were stored. We also assessed the
dimensions of the receptive field with a drifting bar stimulus to
quantify the xy coordinates defining the width and length of
the area from which a bar would drive excitatory responses. Next, we
examined the effect of increasing the diameter of an optimally oriented
patch of grating centered over the receptive field center. This was
followed by a similar test but with an annulus of optimally oriented
grating with its virtual center over the center of the CRF, and the
variable was the diameter of the inner wall of the annulus. This latter
test brought an optimally oriented border in toward the receptive field center. The stimulus variables for all the protocols used to assess RF
size were randomized and interleaved and responses assessed from the
mean computed from 10 to 50 presentations of the stimulus. The data
from the four methods gave similar values, but those from the XY patch
and bars were the smallest. Across the sample (n = 105), the mean value for CRF size derived from the XY patch method was
0.9 ± 0.08° (mean ± SE) compared with 0.75 ± 0.10 from the bars, 1.1 ± 0.14° from the optimal summation diameter
and 1.15 ± 0.17° derived from the annulus paradigm. In all but
two cases, the values used for defining the CRF borders were drawn from
either the optimal summation diameter or annulus paradigm, with the two
exceptions following from cases where the XY patch test revealed the
largest values.
To minimize any effects of adaptation by persistent presentation
of a stimulus at the cell's optimal orientation and to generate control data for subsequent tests, the protocols varying patch diameter
or annulus inner wall diameter also varied the orientation of the
stimulus in a randomized interleaved fashion. The values for the
optimal orientation were then extracted from the data sets and used to
plot the patch tuning curves.
QUANTIFYING RESPONSES.
Responses were computed from the mean firing rate averaged over the
full number of stimulus presentations. Typically we presented three to
five stimulus cycles of each stimulus condition repeated over 5-20
trials. For each cell, we calculated a patch suppression index (PSI)
according to the formula PSI = [1
(Rplat/Ropt)]*100, where Ropt and
Rplat denote the responses elicited by
the optimal and plateau stimuli, respectively. Thus cells showing no
suppression to large diameter stimuli would have a PSI of 0, while
those showing total response suppression would have a PSI of 100. To
explore the effects of direction contrast on patch suppression, we used concentric bipartite sinusoidal gratings centered over the receptive field and varied the direction of drift of the inner and outer stimuli.
Cells were regarded as showing no direction contrast if the response to
the inner stimulus drifting in the preferred direction in the presence
of an outer stimulus drifting in the reverse direction was not
significantly different to the response observed when the inner and
outer stimuli both drifted in the same direction (P = >0.05, paired t-test). Cells were regarded as showing
direction contrast modulation if the response to the reverse direction
configuration was significantly larger (P < 0.05) than
the response observed when the inner and outer stimuli both drifted in
the preferred direction [thus "direction contrast modulation" is
analogous to the term "orientation contrast" (Knierim and
Van Essen 1992
)]. In some cases, the response to the direction contrast stimulus configuration exceeded the response to the inner stimulus presented alone ("direction contrast facilitation"). To
quantify this, we calculated the percentage response increase elicited
by the reverse direction configuration with respect to the response
level elicited by the inner patch of grating presented alone. Cells
were only regarded as showing direction contrast facilitation if the
response to the reverse direction configuration was significantly
larger (P < 0.05) than the responses to the same
direction configuration and the inner stimulus alone and exceeded that
to the inner alone by 10% or more. (We observed one example where the
response to the reverse direction configuration was significantly
smaller than the response to the same direction configuration. For
simplicity, this cell was included in the no direction contrast
grouping.)
Contour maps of the CRF were plotted as a function of stimulus position
on a ten level iso-response contour plot [where the distance between
contours was defined by the equation
(Rmax
Rmin)/1 + number of levels,
and the first level was defined by Rmin], using a spline fitting
algorithm for interpolation between recorded positions.
To examine the spatial location of suppressive zones, we used two
square patches of optimally oriented sinusoidal grating. One grating
patch was centered over the CRF while the second stimulus patch was
presented in randomized sequence at a range of locations around the
field. For graphical representation of this data, we constructed
three-dimensional surface maps documenting the modulatory effect of the
second stimulus on the response to the simultaneously presented central
stimulus at a range of xy locations. The data were
represented as iso-response surface plots, using a spline fitting
algorithm for interpolation between recorded locations. The central
point in these surfaces always represented the response to the central
stimulus presented alone. The data were also represented as
two-dimensional iso-response contour maps (shown beneath each surface
plot). We adopted the procedures and criteria used in area MT by
Xiao et al. (1997b)
to quantify the angular distribution of the suppressive zones. First, we computed the strength of
suppression (expressed as a percentage of the response to the center
stimulus alone) for each surround stimulus location, according to the
formula S = [1
(Rcs/Rc)]*100,
where S is the strength of the antagonistic surround
elicited by a particular surround stimulus location, Rcs is the response to the combination
of the center and surround stimulus, and
Rc is the response to the center
stimulus presented alone. We then computed two selectivity indices
(SIs) from the level of surround antagonism generated by each of the
surround stimulus positions using a formula, based on circular
statistics, for calculating the length of the mean vector
where Si is the magnitude of the surround suppression
at each surround location,
i. Following Xiao et
al. (1997b)
, we termed the first of the two SIs the unimodal
selectivity index (USI), which was calculated from the actual
i values. The USI is a measure of the degree of
unimodality of the surround antagonism, i.e., the tendency for the
surround antagonism to be concentrated in one location. A USI value of
1.0 indicates that only a single surround position was effective in
modulating activity, whereas a value of 0.0 denotes a uniform angular
distribution of surround antagonism. The second SI, the bimodal
selectivity index (BSI), was calculated with each
i value
doubled and reflects the degree of bimodal distribution, or the
tendency for surround antagonism to be concentrated along an axis, on
opposite sides of the CRF. A BSI value of 1.0 indicates that all
suppression originates along a single axis, whereas a values of 0.0 denotes that the suppression along each axis is equal.
The Rayleigh test (Batschelet 1981
), which tests the
hypothesis that the data are uniformly distributed, and the USI and BSI values were employed for classifying the angular distribution of the
antagonistic surround into three classes: uniform or circularly symmetric surround suppression (Rayleigh test P
0.05), asymmetric surround suppression (Rayleigh test P < 0.05 and USI > BSI) and bilaterally symmetric suppression
(Rayleigh test P < 0.05 and BSI > USI).
To quantify the surround location showing most suppression, we computed
the optimal angle (OPA) for each cell using the formula for calculating
the mean vector angle (Batschelet 1981
)
For cells with a bilaterally symmetric surround, the OPA
represents the angle of the axis through the two optimal surround locations.
RECONSTRUCTION OF RECORDING SITES.
At the end of each electrode penetration, key recording sites were
marked by electrolytic lesions (3-5 µA for 3-5 s, electrode negative). At the conclusion of the experiment, animals were overdosed with pentobarbital sodium, desanguinated with phosphate-buffered saline
(PBS), and perfused with paraformaldehyde followed by sucrose in PBS.
Frozen sections were cut at 40 µ, and alternate sections were stained
by the Nissl method and an enhanced cytochrome oxidase method,
respectively. Sections containing electrolytic lesions were drawn at
low power. Adjacent sections were aligned precisely using blood vessels
and section outlines as reference points.
 |
RESULTS |
The results reported here derive from 105 cells recorded in layers
2-6 of primate V1 at eccentricities from 2-6°. Our sample comprised
61 S type cells and 44 C type cells. All the effects reported applied
equally to both S and C types.
Spatial summation curves and suppression
For all the cells in our sample (105), we determined the change in
response as the diameter of a patch of optimally oriented drifting
grating was varied. The core procedures we used to center on the CRF,
map its size, and examine its spatial summation characteristics are
illustrated in Fig. 1 for a layer 5 cell.
The histogram (Fig. 1A) shows the response of the cell to an
optimally oriented 0.3° square of drifting grating presented in a
randomized sequence at a range of locations over and around the
receptive field. The responsive regions are clearly defined. The
contour plot (Fig. 1B) provides an overview of the shape of
the field as determined by this method. The spatial summation curve
(Fig. 1C) shows the response of the cell to varying the
diameter of an optimally oriented patch of drifting grating. The
response rose and then fell as the stimulus reached and then exceeded
0.75° in diameter, suggesting a potent suppressive or disfacilitatory
influence beyond this point. This spatial summation curve was typical
of the majority of cells we saw in primate V1. In addition to
quantifying the response to varying the diameter of a circular patch,
we also plotted the response to varying the diameter of the inner wall of an annulus of drifting grating. This provided a mirror image probe
to the sequence of patch diameters and enabled us to assess the response of the cell to stimulation of outer regions of the receptive field in the absence of stimulation of the central region. The bottom right curve shows the response to varying the
diameter of the inner wall of an optimally oriented annulus of drifting grating. This started to exert a small excitatory effect at 0.75°. For the sake of simplicity, we have used the term CRF here to indicate
the area of visual space from which the cell showed clear excitatory
responses with the tests used. In the case of the example shown in Fig.
1, we defined this as 0.75°.

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Fig. 1.
Classical receptive field and spatial summation properties.
A: the 3-dimensional (3-D) histogram documents the
response to a small patch of an optimally oriented, drifting sinusoidal
grating presented at a range of spatial locations spanning a 3 × 3°
area of visual space encompassing the cell's receptive field location.
Responses (computed from the mean response rate averaged from the full
stimulus cycle over 15 stimulus repeats) were elicited only from a very
circumscribed area of visual space. [Patch diameter, 0.3°. Spatial
frequency (SF), 2 cycles/degree (cpd). Temporal frequency (TF), 3 Hz.
Contrast 0.36. Vertical scale denotes response in imp/s. C type layer 5 cell.] B: contour plot delineating the shape of the
receptive field shown in A. The magnitude of the cell's
response is shown by the shading of the contours as denoted by the
color scale to the left. The scale bar shown in red
denotes 0.5°. See METHODS for further details.
C: the tuning curve plots the variation in response
magnitude for increasing diameters of an optimally oriented patch of
grating centered over the receptive field center. Responses were
normalized to the response value elicited by the optimal diameter patch
(9 imp/s). Error bars indicate ±1 SE. Black line to the right denotes
spontaneous activity level. The patch suppression index for this cell
(see METHODS) was 43%. Stimulus details as in
A but 50 stimulus repeats. D: the tuning
curve documents the response to varying the inner diameter of an
annulus of optimally oriented grating. Responses were normalized to the
maximal response seen in the patch tuning curve (C).
Stimulus details as in C.
|
|
We show two further examples of spatial summation curves for a circular
patch of drifting grating in Fig. 2,
A and B. The variation in patch suppression over
our cell sample is shown by the histogram in Fig. 2C. Here
we have quantified the degree of suppression in terms of the percentage
reduction in the response observed at the plateau of the spatial
summation curve elicited by larger diameter stimuli in comparison to
the response seen to an optimal diameter patch (see
METHODS). The percentage reduction in response is
represented in steps along the abscissa and number of cells in each
category on the ordinate. The majority of the cells (99/105, 94%)
exhibited response suppression to large diameter stimuli with a mean
suppression of 67% (±2.07%; mean ± SE). This decrement in
response with increasing stimulus diameter was highly significant
across the population (P < 0.001 Wilcoxon test) and reflected a potent reduction in the output of V1 cells for optimally oriented stimuli extending beyond the CRF. Indeed it is worth underlining the fact that 80% of the sample exhibited a more than 50%
suppression and 43% a more than 70% suppression in response. We
recognize two possible sources of error in these observations. The
first was that in a few cases, we were unable to generate stimuli large
enough to be sure that we had accessed the full extent of the surround
suppression and the second that in a few cases, we were unable to
generate stimuli small enough to be sure we had accessed the cell's
optimal response. However, both these would cause us to underestimate
the degree of surround suppression and so would emphasize rather than
diminish the finding that the majority of primate V1 cells are strongly
suppressed by stimuli extending beyond their CRF.

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Fig. 2.
Patch suppression across our V1 cell sample. A and
B: 2 further examples of spatial summation curves.
Conventions as for Fig. 1C. For A, the
patch suppression index was 69% and the optimal response 167 imp/s.
(30 stimulus repeats. SF, 2cpd; TF, 3 Hz; contrast, 0.36. C type layer
4B cell.) For B, PSI was 64% and optimal response 33 imp/s. (Further details as in A. S type layer 4C
cell.) C: block histogram plotting the distribution of
patch suppression across the V1 cell population (n = 105). Cells were subdivided into 10 categories of patch tuning,
binned in 10% epochs. Thus cells in category 0-9% had little or no
patch tuning, cells in category >90% showed little or no response to
large diameter patches (see METHODS for details of
quantification).
|
|
These observations might follow from a sample restricted to the
superficial layers (cf. Born and Tootell 1991
), or they
might encompass a substantial laminar variation in the degree of patch suppression. Given the variation in connectivity of the different layers, it might be expected that cells in the different layers would
show large variations in the degree of patch suppression. Interestingly, as shown in Figs. 3 and
4, we were unable to
demonstrate a laminar variation in the distribution of cells showing
surround suppression. The range of the indices of patch suppression was similar through all laminae. Figure 3, A-C, shows the
laminar distribution of cells showing a more than 25, 50, and 70%
reduction in response with stimulus diameter while Fig. 4 shows the
number of cells in each lamina falling in the groups summarized in Fig. 2C. We also compared the distribution of optimal summation
diameters and the distribution of stimulus diameters eliciting maximal
suppressive effects across cortical layers. The scatter diagrams in
Fig. 5 plot, for each lamina, the
magnitude of patch suppression versus optimal summation diameter
(top) and versus maximal suppression diameter
(bottom). Again, there is little evidence to support any
obvious differences across layers. In Table
1, we summarize, for each layer, the mean
(±SE) values observed for patch suppression, optimal summation
diameter, maximal suppressive diameter and spatial frequency used. Once
more, there appears to be little laminar variation in the mean values
observed for any of these parameters, although, interestingly, the
optimal summation diameter for layer 5 and 6 cells was nearly double
that seen for the other cortical layers. In general, the mechanism
underlying patch suppression would appear to be common to all
processing steps within V1 and possibly represents a general algorithm
pertaining at this level in the system. The distribution of surround
suppression through all layers of V1, plus the numbers of cells showing
high levels of suppression, underlines the fact that extensive stimuli
(4-9° diameter) will tend to minimize the output of a column.
Furthermore, for eccentricities in the region of 5° as explored in
the present work, even a 2° stimulus will result in substantive
attenuation of the output of many cells in a column.

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Fig. 3.
Laminar distribution of patch-suppressed cells. Cortical layers were
assigned according to the criteria of Lund (1988) . The 3 block histograms show the percentage of patch suppressed cells in each
lamina. For the histogram in A, any cell showing 25% or
more suppression was regarded as patch suppressed. B:
only cells showing 50% or more suppression were regarded as patch
suppressed. C: cells were classed as patch suppressed
only if the suppression with large diameter patches exceeded 70%.
Regardless of the cutoff value chosen, patch suppressed cells were
distributed across all laminae.
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Fig. 4.
Block histograms plot the distribution of patch suppression for
different cortical layers (noted above each histogram).
Cells were subdivided into ten categories of patch tuning, binned in
10% epochs as described in the legend to Fig. 2C.
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Fig. 5.
The scatter diagrams plot the magnitude of patch suppression (%) vs.
optimal summation diameter (top row) and vs. maximal
suppression diameter (bottom row) for different cortical
layers (noted above each plot).
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Dissection of the spatial organization of suppressive mechanisms
Generally, suppression in the receptive fields of cat V1 cells has
been associated with either suppressive end zones, suppressive side
bands, or both (DeAngelis et al. 1994
; Hubel and
Wiesel 1965
; Kato et al. 1978
; Orban et
al. 1979a
,b
; Walker et al. 1999
). It is
important to know how the suppression we examined here with patches of
varying diameter links to discretely identifiable end zones or side
bands. Hence we included in our tests a protocol examining the
influence of a second discrete patch of grating introduced at a stepped
series of locations around a patch of rectangular drifting grating
overlying the CRF. Examples of the data obtained from this are shown in
Fig. 6, A-J. These surface plots show the variation in response magnitude to the stimulus overlying the CRF induced by the presentation of the second stimulus at
any of the locations around the CRF (in a randomized interleaved sequence) as indicated by the matrix of points in the icon diagram above the records. The plots are all oriented so that the axis of the
optimal orientation of the cell lies along the plane indicated in the
icon diagram. In each case the center point of the records and the
color, dark green, indicates the response level associated with the
inner stimulus alone. All the cells in the examples A-J in
Fig. 6 exhibited strong surround suppression with increase in the
diameter of a circular patch of drifting grating. However, the detailed
dissection of the zones around the CRF revealed patterns of influence
that bore no relation to the degree of suppression following from an
increase in the diameter of a circular patch of grating. The cell in
Fig. 6A was not suppressed by the second stimulus at any
location around the CRF and that in Fig. 6B showed a slight
suppression at one location only, while the cells in Fig. 6,
I and J, were suppressed at all locations around
the CRF. The other examples encompass patterns that show clear end
zones and side bands (Fig. 6C) and those where suppressive
effects partially surrounded the field or sat at either corner of the
receptive field. The scatter diagram in Fig.
7 compares the amount of suppression observed at the plateau level of the patch summation curve to that
observed using a discrete patch of grating positioned at the most
effective surround location. As is clear, there was little correlation
between the plateau level large diameter patch suppression and the most
effective suppression elicited by a discrete patch. Indeed, for more
than half the sample (58%), we were unable to detect any significant
influence from side bands, end zones or corner zones (ANOVA) in cells
showing significant patch suppression (P < 0.05 Wilcoxon test and ANOVA). Thus for these cells, a stimulus uniformly
surrounding the CRF appeared to recruit otherwise subthreshold effects
to exert a potent suppressive influence. Where there were clearly
defined suppressive foci around the CRF, our data suggest a wide
variety of configurations for their spatial organization. To quantify
the degree of heterogeneity in these cells, we have used circular
statistics (Batschelet 1981
; Xiao et al. 1995
,
1997b
) to analyze the data. We used the criteria described by
Xiao et al. (1997b)
(see METHODS) to
subdivide the cells into three groups, those exhibiting spatially
uniform surround suppression, spatially asymmetric surround
suppression, and bilaterally symmetric surround suppression. The
majority of the cells analyzed in this way (81%) exhibited spatial
heterogeneity of surround locations, although 19% showed spatially
uniform surround suppression (an example is shown in Fig.
6J). Cells exhibiting heterogenous surrounds were divided approximately equally into spatially asymmetric
cells (44%) where the surround suppression was biased toward one
location (e.g., Fig. 6B) and bilaterally symmetric cells
(37%) where the surround effect was localized to two opposing regions
along a single axis (e.g., Fig. 6F). For cells that
exhibited spatially heterogenous surrounds, we asked whether the
suppressive effects were localized to the ends, sides, or corners of
the field. Interestingly, suppressive effects were nearly equally
distributed in all directions round the CRF; there was no evidence to
suggest that suppressive effects were concentrated in end-zone or
side-band regions. As previously described, for 58% of cells showing
significant patch suppression to a large grating patch, we were unable
to detect any significant suppressive influence from a discrete second
stimulus presented at any location around the CRF. Nonetheless, we also checked the degree of heterogeneity in the spatial organization of the
surround for this subgroup of cells using the circular statistics
method described in the preceding text. The results were essentially in
accord with those for the 42% of cells that did show significant
suppressive influences to a discrete second stimulus located at some
position around the CRF. Thus the majority of cells showed heterogenous
surrounds, and these were again divided approximately equally into
spatially asymmetric and bilaterally symmetric types.

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Fig. 6.
Spatial organization of suppressive effects. The surface plots depict
the modulatory effect of a 2nd stimulus presented at a range of spatial
locations on the response to a central stimulus for 10 patch suppressed
cells recorded in primate V1. The stimulus configuration comprised an
inner stimulus (a square patch centered over the CRF containing an
optimally oriented grating drifting in the cell's preferred direction
of motion) and a 2nd stimulus (another square patch of optimally
oriented grating drifting in the same direction of motion) that was
positioned at a range of xy locations around the central
stimulus (as depicted by the schematic diagram above).
In each plot, the responses are normalized with respect to the response
elicited by the center patch alone (100% in each case, dark green).
Suppressive effects are denoted by blue colors, facilitatory effects by
light green to yellow colors (see color scale bar top
right). Center patch diameter ranged from 1 to 2° depending
on each cell's CRF size. Spatial frequency ranged from 2 to 3 cpd.
Temporal frequency, 3 Hz; contrast, 0.36.
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Fig. 7.
Comparison of the amount of suppression observed at the plateau level
of the patch summation curve to that observed using a discrete patch of
grating positioned at the most effective surround location. The scatter
diagram plots the degree of suppression (%) elicited by a large
diameter patch along the x axis vs. the degree of
suppression (%) elicited by the most effectively located discrete
patch of grating along the y axis.
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Dissection of surround effects with annuli
The spatial summation curves constructed from a circular patch of
varying diameter reflect a situation where the receptive field center
mechanism is always part of the integration driven by the stimulus. For
this reason, we examined the effect of varying the diameter of
the inner wall of an annulus of drifting grating so that we could
explore the effect of a stimulus encroaching on the field from the
surround without optimally activating the center mechanism. The data
obtained revealed some interesting variances in the pattern of
integration of surround influences and the mechanisms driving responses
from the center of the CRF.
We explored these effects in detail for 54 cells in our sample by
comparing the responses obtained in the patch tuning curves to effects
elicited by annuli encroaching into the CRF but excluding the very
center of the field. We grouped the data obtained with the annuli into
three categories, those obtained with the inner border of the annulus
in the outer 25% of the diameter of the CRF, those obtained with the
annulus border in the middle 50%, and those obtained with the annulus
border in the inner 25%. For the general comparisons, we have taken
the category giving the largest response. Essentially these data
highlighted the presence of cells with contrasting patterns of
responses to the annuli. On the basis that an annulus by definition
excludes the receptive field center, but encompasses all the surround,
it is logical to expect that the best response to an annulus would be
less than the plateau in the area summation curve. This indeed was the
case for many cells (20/54, 37%). We separated out those cells showing responses lower than the plateau in the area summation curve using the
criterion that the responses to the most effective annulus had to be
significantly smaller than the plateau of the area summation curve
(P < 0.05 level, t-test). For these cells,
the mean response to the annulus was 61 ± 6.55% smaller than the
value of the plateau in the patch tuning curve. Taking each category of
the annulus encroachment within the CRF in turn the responses were
76 ± 6.41% smaller for the outer 25%, 64 ± 7.95% smaller
for the middle category, and 68 ± 13.89% smaller for the inner
category. Examples of the pattern of effect we saw are shown in Fig.
8. It is clear in Fig. 8, A
and B, that the annulus exerted a small but increasing
excitatory effect as it encroached into the CRF, but one that was
smaller than the plateau in the patch tuning curve (marked by the
dashed line). These observations would be consistent with the
predictions either for a suppressive field that surrounded the
excitatory CRF or for those following from the difference of Gaussians
model with overlapping inhibitory and excitatory fields.

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Fig. 8.
Block histograms comparing the responses elicited by patches of varying
diameter to those to annuli of a fixed outer diameter and a varying
inner wall diameter. A: patch responses are denoted by
the dark gray stippled bars to the left of the figure,
annulus responses by the light gray stippled bars on the
right. Stimulus configuration is denoted schematically
above each bar. Patch and annulus inner wall diameters
are indicated below each bar. The best response to an
annulus (for an annulus with an inner wall diameter of 0.5°) was
considerably smaller than the response elicited by the largest patch
(response level denoted by dashed line). (50 stimulus repeats, SF, 2 c/d; TF, 3 Hz; contrast, 0.36. C type layer 4B cell.) B:
stimulus conventions as in A. (Details as for
A, but patch/annulus inner wall diameters are 1, 2, 3, and 9°. TF, 4 Hz; C type layer 3 cell.)
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However, for the majority of the cells in our sample (34/54, 63%), the
largest response to an annulus was either not significantly different
to (7/34 cells) or was significantly more than (27/34 cells) the
plateau in the area summation curve (P < 0.05). Two examples are shown in Fig. 9. In both
cases, the response to an annulus within the CRF substantially exceeded
that to the plateau in the patch tuning curve (picked up by the dashed
line) and indeed the response to the optimal patch diameter (picked up
by the dotted line). Thus for both these cells, including the very
center of the CRF in a stimulus that extended beyond the CRF reduced
the response rather than enhanced it suggesting an increase in the magnitude of the "suppressive effect." Interestingly, the example in Fig. 9A shows that the response to the annulus decreased
as it encroached further into the central region of the CRF. For these
two examples, one could argue that the optimal stimulus was an annulus
excluding the very center of the CRF. For the group as a whole, the
mean best response to an annulus driving the CRF was 195 ± 68.10% larger than the response level for the plateau in the patch
tuning curve. Taking each category of annulus encroachment into the CRF
in turn, the responses for the outer 25% were 100 ± 82.53%
larger, middle category 83 ± 25.21% larger, and inner category
85 ± 35.63% larger. It is clear for these cells that including
the very center of the CRF in a stimulus extending beyond the borders
of the CRF reduced the response rather than enhanced it.
Thus for these cells, the surround suppressive mechanism appeared to be
enhanced by, and in some cases require (as in Fig. 9), activation of
the CRF center. This pattern of effect is neither simply predicted by
the differences of Gaussians model or a surrounding inhibitory field.

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Fig. 9.
Block histograms showing that excitatory response to an annulus falling
within the CRF can exceed the responses to the plateau in the patch
tuning curve. A: patch responses are denoted by the dark
gray stippled bars to the left of the figure, annulus
responses by the light gray stippled bars on the right.
Stimulus configuration is denoted schematically above
each bar. Patch and annulus inner wall diameters are indicated
below each bar (0.3, 0.5, and 4°, respectively). The
best response to an annulus exceeded the response seen in the patch
tuning curve at the plateau (response level denoted by dashed line) and
the optimal response in the patch tuning curve (dotted line). (24 stimulus repeats, SF, 2 c/d; TF, 3 Hz; contrast, 0.36. layer 4C
cell.) B: stimulus convention as for A.
(Details as for A, but patch/annulus inner wall
diameters are 0.5, 1, 6, and 9°. 50 stimulus repeats, SF, 1 cpd;
Layer 6 cell.)
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To simplify the description, we refer to those cells showing annulus
responses that were significantly below the plateau in the patch tuning
curve as classical surround suppression (CSS) cells and the others as
center gated surround suppression (CGSS) cells. The block histogram in
Fig. 10A summarizes the
differences in the mean relative response levels of the CSS and CGSS
category cells to annuli in comparison to the plateau response from the patch tuning curve. The distinction between the two groups is further
highlighted if one considers the response magnitudes with respect to
the optimal. For the CSS category, the best annulus responses were
84 ± 3.22% smaller than the optimal while for the CGSS group the
best annulus responses were only 34 ± 7.65% smaller than the
optimal, as shown in Fig. 10B. We highlight the CSS and CGSS
behavior because it underlines patterns of response that are
sufficiently different to suggest distinct roles in the processing of
the visual input. This point is underlined by the scatter diagram in
Fig. 10C that plots the response to a large patch driving
plateau-level response against the response to an annulus with the
inner wall set at the diameter eliciting the best response. Cells with
CSS properties are denoted by circles in the plot and those with CGSS properties by triangles. The dashed line identifies the diagonal denoting equal responses to annuli and large patches driving
plateau-level responses. The broad distinction between the two
categories is clear, although it remains open to question as to whether
they reflect distinct groupings or two ends of a continuum deriving from a varying level implementation of the process generating the
deviation of CGSS cell response from that which might be predicted from
simpler mechanisms. The essential point though is that the two extremes
encompass cells that, on the one hand, respond better to an annulus of
drifting grating that excludes the center and, on the other, respond
better to a patch of drifting grating that excludes the surround.

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Fig. 10.
A and B: block histograms summarizing the
mean relative responses of our population of classical surround
suppression (CSS) and center-gated surround suppression (CGSS) cells to
annuli in comparison to the plateau response from the patch tuning
curve (A) or the optimal response from the patch tuning
curve (B). In A, the histogram plots the
mean difference in response for the most effective annulus tested in
comparison to the response level seen for the plateau of the patch
tuning curve. The response at the plateau of the patch tuning curve
(marked by the arrow head) is set to 0 so that negative values indicate
that the response to the annulus was smaller than that at the plateau
of the patch tuning curve, whereas positive values indicate that the
responses were larger. CSS cells are denoted by the gray bar, CGSS
cells by the black bar. Error bars indicate 1 SE. In B,
the histogram plots the difference in response for the most effective
annulus tested in comparison to the optimal inner patch response. The
optimal patch response (marked by the arrow) is set to 0 so that
negative values indicate that the response to the annulus was smaller
than the optimal patch response. Bar conventions as in A.
C: distribution of plateau vs. annulus responses for CSS and
CGSS cell groups. The graph plots the response (in imp/s) to a large
diameter patch along the x axis vs. the best response
observed to an annulus along the y axis. CSS cells are
denoted by circles and CGSS cells by triangles.
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We were interested to ascertain whether we could isolate another
measure of the distinction between these two groups. If the suppression
derived from the surround, then the annulus response would be a mirror
reflected image of the patch response. Assuming this to be the case,
one can compute the number of excess spikes (if any) that an annulus
produced over the prediction. We have thus computed the number of
excess spikes produced by an annulus over the prediction based on the
shape of the mirror-image patch-tuning curve (but resetting the
prediction to 0 if the prediction was negative). This produced figures
of 3.6 ± 0.69 (SE) imp/s for CSS cells and 11.7 ± 1.60 imp/s for CGSS cells. These values were statistically significantly
different at the P < 0.001 level (Mann-Whitney U test). The difference was not because CGSS cells had a
higher overall firing rate than CSS cells because the mean optimal
firing rate for CSS cells was if anything slightly higher at 29 ± 5.00 imp/s than that for CGSS cells (25 ± 3.56 imp/s), although
the differences were not statistically significant. We also quantified the number of excess spikes as a percentage of the optimal patch response. The mean value for CSS cells was 13.6 ± 2.48% and that for CGSS cells was 59.4 ± 6.56%. These values were statistically significantly different at the P < 0.001 level
(Mann-Whitney U test). These figures show that both the CSS
and CGSS cells drive extra spikes, but there seems to be a very robust
enhancement of the effect in the transition to CGSS cells. Overall this
supports the concept of a mechanism, potentially present across all
cells in the sample but implemented with varying strength, to form two extrema in the pattern of responses to annuli.
Influence of direction of stimulus motion on surround suppression
It is clear from previous and current work in our laboratory
(Sillito et al. 1995
) and that of others (Born
and Tootell 1991
; Knierim and Van Essen 1992
;
Nothdurft et al. 1999
) that surround suppression in
primate V1 is generally tuned to the same orientation as a cell's
excitatory response. Thus it is likely that the connections between
cortical columns tuned to the same orientation (Bringuier et al.
1999
; Gilbert and Wiesel 1989
;
Kisvárday and Eysel 1992
; Malach et al.
1993
; Ts'o and Gilbert 1988
; Ts'o et
al. 1986
) must provide a significant contribution to
the degree of surround suppression. However, this could be either via
direct facilitatory inputs that might tend to decrease the degree of
suppression or indirect connections via inhibitory interneurons that
would enhance it. Additionally it is not clear whether the pattern of
influence would be the same when the direction of the surround stimulus
is reversed. Although effects have been described for a range of
stimulus configurations involving motion contrast (Lamme
1995
; Orban 1994
; Orban et al. 1989
), this has not been systematically examined in the context of the mechanisms underlying surround suppression in the primate. At
least one reason for this is that the incidence and strength of
surround suppression in primate V1 has not previously been appreciated.
We thus examined the effect of reversing the direction of motion of the
surround stimulus. These observations were made on 51 cells of our
sample. All cells included in the analysis exhibited a PSI more than
20%. We examined the effect of reversing the direction of motion of
the surround stimulus at range of different interface diameters for the
center surround border. This was to enable us to examine the effect of
reversing the direction of motion on surround suppression for a border
within, on the edge of, and outside the CRF. We observed different
types of effect from the reverse direction configuration. In the first
instance, we have summarized these for the interface diameter
generating the largest effect (where there was an effect of reversing
the direction), and then we examine the influence of the location of
the interface border with respect to the CRF.
For 22% of the cells tested (11/51), reversing the direction of drift
of the surround had no effect on the magnitude of suppression at any
interface diameter tested. For this subgroup, the mean suppression
(with respect to the response to the inner stimulus alone) for the
iso-direction surround was 45 ± 9.31% compared with a value of
49 ± 8.24% for the reverse direction surround. An example of the
tests carried out on one of these cells is illustrated in Fig.
11A. The icons above the bar
chart indicate the stimulus configurations. The cell exhibited
directional selectivity to the inner stimulus alone but for either
direction introducing an outer stimulus drifting in either the same or
opposite direction reduced the response. For these cells, the mechanism
driving the surround suppression would appear to integrate both
directions of motion equally, even where, as for the example in Fig.
11A, the excitatory response driven from the field center
was directionally selective. We should qualify our comments for this
group with the comment that one of the cells showed a small, but just
significant, increase in suppression when the direction of motion of
the outer stimulus was reversed. This shift is included in the average
change for the group quoted in the preceding text. These cells were
thus not sensitive to direction contrast but were sensitive to the size
of the stimulus.

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Fig. 11.
These histograms document the responses of 2 V1 cells to a direction
contrast stimulus. A: the 4 columns on the left
plot, respectively, the response (in imp/s) to an inner patch
of grating drifting in the cell's preferred direction of motion
(column 1), the response to an annulus of grating
drifting in the preferred direction (column 2) and then
the response to the inner patch of grating drifting in the preferred
direction presented simultaneously with the annulus of grating drifting
in the same (column 3) or opposite (column
4) direction. The 4 columns to the right plot
the response for the opposite direction of drift of the inner stimulus.
Stimulus conditions are summarized schematically above each record.
Error bars denote +1 SE. (Patch/interface diameter 1°. TF, 3 Hz; SF,
2 cpd; contrast, 0.36. 25 stimulus repeats. S type layer 4A cell.)
B: convention as in A. (Patch/interface
diameter, 0.75°. Further stimulus details as in A, but
SF, 3 cpd; S type layer 4 B cell.)
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The remaining cells were all sensitive to direction contrast, showing
significant changes in surround suppression when the direction of drift
of the outer was opposite to that of the inner. These cells fell into
two groups, one showing a direction-contrast-dependent modulation of
the strength of surround suppression and the other a
direction-contrast-driven facilitation of responses. The group exhibiting direction-contrast modulation constituted 41% (21/51) of
our sample and showed a reduction from a mean suppression of 70 ± 4.11% for the iso-direction surround to 22 ± 5.31% for the reverse direction surround, thus reflecting a partial but not total
reduction in the strength of the surround suppression. An example of
the responses of one of these cells is shown in Fig. 11B.
The cell showed no directional selectivity to the inner stimulus, suppression when the outer stimulus moved in the same direction, and a
reduction in surround suppression when the direction of the outer
stimulus was reversed. This would seem to indicate that the mechanism
integrating the suppression in these cells was only fully enabled when
the surrounding and central area of visual space were engaged by the
same direction of motion. Equally, a significant component of
suppression (22%) remained in the reverse direction configuration,
suggesting the possibility of two groups of lateral interactions
driving the surround suppression.
Some of the complexities in the process generating suppression are
underlined by the responses of the cells showing direction contrast
facilitation. These constituted 37% (19/51) of our sample, and when
the direction of the outer stimulus was opposite to that of the inner,
their responses exceeded that to the inner alone. For these cells, the
iso-direction surround stimulus elicited a suppression of 28 ± 5.79% of the response to the inner alone at the interface diameter
used for the test, while the response in the presence of the reverse
direction surround was a mean facilitation of 74 ± 15.69%.
Examples of this pattern of response are given in Fig.
12, A-C. Note that in Fig.
12, A-C, the diameter of the central patch used for the
tests was larger than the optimal diameter for a single patch. For each
of these cells, although the reverse direction configuration evoked a
response level higher than that to the inner stimulus used in the test,
the responses did not exceed the response elicited by the optimal
single stimulus. Thus the reverse direction enhancement may reflect a
disinhibitory mechanism serving to reset the lower firing level
associated with the particular inner stimulus toward the cell's
optimal (see DISCUSSION and following text). In some cases,
as in Fig. 12D, the response to the direction contrast
configuration exceeded that evoked by the optimal single patch diameter
stimulus. Of the cells showing direction-contrast facilitation, 26%
(5/19) showed this "supra-optimal" facilitation. For this group in
isolation, the mean response reduction associated with the
iso-direction surround was 23 ± 14.67% at the interface diameter
used for the test, while the mean response increase for the reverse
direction configuration was 133 ± 45.87%. This translated into a
mean increase of 95% above the value for the optimal diameter stimulus
alone. The lower degree of iso-direction suppression reported here for
the examples showing reverse direction facilitation and supra-optimal
facilitation merely reflects the fact that many of these effects were
only observed with interface diameters where the inner stimulus
exceeded the CRF size (and was hence already driving a component of
surround suppression, see following text). There was no significant
difference (P > 0.05, Mann-Whitney U test)
in the absolute degree of surround suppression derived from the area
summation curves for the group of cells showing direction contrast
facilitation and those that did not.

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Fig. 12.
Further examples of the effects of direction contrast between
iso-oriented stimulus components. Conventions as for Fig. 11.
A: patch/interface diameter 1°. TF, 3 Hz; SF, 2 cpd;
contrast, 0.36. 15 stimulus repeats. C type layer 4B cell.
B: further details as for Fig. 12A. S
type layer 4B cell. C: further details as for Fig.
12A but patch/interface diameter 1.5°. S type layer
4C cell. D: further details as for Fig.
12A but 20 stimulus repeats. Patch/interface diameter
was 1°. The 1° patch was the optimal single stimulus for this cell.
C type layer 4B cell.
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For the cells showing direction contrast facilitation, changing the
interface diameter could change the response. An example is given in
Fig. 13, A and B,
where it is clear that adding a surround stimulus to a 1° inner
stimulus (the optimal diameter for this cell) caused a strong
suppression when it drifted in the same direction and a still clear but
weaker suppression in the other direction. However, when the stimulus
diameter was increased to 2°, although adding a surround drifting in
the same direction again strongly suppressed the cell's response to
the inner alone, reversing the direction of drift of the outer resulted
in a response level exceeding that to the 2° inner alone. It is to be
noted that the response level associated with the reverse direction configuration at 2° did not exceed that to the 1° inner (optimal diameter) alone, but the reverse direction configuration at 2° resulted in a response that was substantially larger than that to the
reverse direction configuration at 1°. It is important to emphasize
that none of the cells placed in the category exhibiting equal
suppression to either direction of drift of the outer stimulus showed
any other effect at any other diameter. Similarly none of the cells
placed in the category showing direction contrast modulation of the
level of surround suppression with direction of drift exhibited
direction contrast facilitation at any stimulus interface diameter
[and the majority exhibited similar effects at diameters smaller
(57%) or larger (83%) than that showing the largest directionally
dependent modulation]. For the cells showing direction contrast
facilitation, 80% exhibited either equal effects or simple modulation
of surround strength for the reverse direction configuration at smaller
interface diameters than those revealing the largest facilitation and
89% at larger diameters.

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Fig. 13.
Histograms show the effect of changing the patch/interface diameter on
direction contrast effects for an S type cell recorded in layer 3. Conventions as for Fig. 11. Top row: the responses
obtained with a patch/interface diameter of 1°; bottom
row: the response of the cell to the same stimulus
configuration but with the patch/interface diameter held at 2°.
(Patch/interface diameter 1°. TF, 3 Hz; SF, 2 cpd; contrast, 0.36. 35 stimulus repeats.)
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The distribution of effects observed across our sample is summarized in
the scatter diagram in Fig.
14A that compares the
modulatory effect of a surround stimulus drifting in the same direction
as the center stimulus (x axis) to that of a surround
stimulus drifting in the opposite direction (y axis),
on the response elicited by the center stimulus alone. Suppressive
effects are denoted by negative values, response enhancements by
positive values. In nearly all cases, the iso-direction surround
stimulus reduced the response to the center stimulus alone so that
virtually all points fall in the left two quadrants of the plot. Cells
where both directions of the surround elicited equal suppressive
effects, as shown in Fig. 11A, lie along the diagonal (
).
We have termed this group "no direction contrast effects." Less
than a quarter of the cells tested showed this pattern of effect. The
remaining cells all lie above the diagonal, indicating that an
iso-direction surround elicited more suppression than a reverse
direction surround. Cells such as that shown in Fig. 11B,
where both drift directions of the surround stimulus suppress the
center response, but where the suppressive effect elicited by the
reverse direction surround is weaker, fall in the lower left quadrant,
above the diagonal (
). We have termed this pattern of effect
"direction contrast modulation." Cells such as those shown in Fig.
12, where the reverse direction stimulus enhances the response to the
center stimulus lie in the upper left quadrant (
). We termed this
pattern of effect "direction contrast facilitation." For five
cells, the magnitude of the response observed exceeded the response
elicited by the optimal single stimulus (
) as illustrated in Fig.
12D. We have termed this effect "supra-optimal direction
contrast facilitation."

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Fig. 14.
A: comparison of the modulatory effects elicited by
surround stimuli drifting in the same direction and in the opposite
direction to the center stimulus on the response elicited by the center
stimulus alone. The modulatory effect of the iso-direction surround
stimulus is plotted along the x axis and that of the
reverse-direction surround stimulus along the y axis.
Suppressive effects are denoted by negative values, response
enhancements by positive values. Cells where both directions of the
surround elicited equal suppressive effects, as shown in Fig.
11A, lie along the diagonal ( , no
direction contrast cells). Cells where both drift directions of the
surround stimulus suppress the center response but where the
suppressive effect elicited by the reverse direction surround is
weaker, fall in the lower left quadrant, above the diagonal
( , direction contrast modulation cells). Cells where
the reverse direction stimulus enhances the response to the center
stimulus lie in the upper left quadrant ( , direction
contrast facilitation). Cells where the magnitude of the response
observed to the reverse direction configuration exceeded the response
elicited by the optimal single stimulus are marked by the (supra-optimal direction contrast facilitation). B:
summary histograms documenting the prevalence of the various patterns
of direction contrast effects with respect to whether the interface
border between the inner and outer stimulus components was within, on
the edge of, or out |
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