The Journal of Neuroscience, August 20, 2003, 23(20):7690-7701
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Time Course and Time-Distance Relationships for Surround Suppression in Macaque V1 Neurons
Wyeth Bair,1,2
James R. Cavanaugh,2 and
J. Anthony Movshon1,2
1Howard Hughes Medical Institute and
2Center for Neural Science, New York University, New
York, New York 10003
 |
Abstract
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Iso-orientation surround suppression is a powerful form of visual
contextual modulation in which a stimulus of the preferred orientation of a
neuron placed outside the classical receptive field (CRF) of the neuron
suppresses the response to stimuli within the CRF. This suppression is most
often attributed to orientation-tuned signals that propagate laterally across
the cortex, activating local inhibition. By studying the temporal properties
of surround suppression, we have uncovered characteristics that challenge
standard notions of surround suppression. We found that the latency of
suppression depended on its strength. Across cells, strong suppression arrived
on average 30 msec earlier than weak suppression, and suppression sometimes
arrived faster than the excitatory CRF response. We compared the relative
latency of CRF response onset and offset with the relative latency of
suppression onset and offset. Response onset was delayed relative to response
offset in the CRF but not in the surround. This is not the expected result if
neurons targeted by suppression are like those that generate it. We examined
the time course of suppression as a function of distance of the surround
stimulus from the CRF and found that suppression was predominantly sustained
for nearby stimuli and predominantly transient for distant stimuli. By
comparing the latency of suppression for nearby and distant stimuli, we found
that orientation-tuned suppression could effectively propagate across 6 - 8 mm
of cortex at
1 m/sec. This is considerably faster than expected for
horizontal cortical connections previously implicated in surround suppression.
We offer refinements to circuits for surround suppression that account for
these results and describe how feedback from cells with large CRFs can account
for the rapid propagation of suppression within V1.
Key words: macaque monkey; primary visual cortex; surround suppression; contextual modulation; response latency; propagation velocity; cortical feedback
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Introduction
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Receptive fields of neurons in the visual cortex can be decomposed into a
classical receptive field (CRF), in which stimuli directly elicit a neuronal
response, and an area beyond the CRF, in which stimuli elicit no response of
their own but can profoundly modulate a CRF-driven response (for review, see
Allman et al., 1985
;
Gilbert, 1992
;
Fitzpatrick, 2000
;
Albright and Stoner, 2002
).
Understanding the mechanisms underlying contextual modulation from the field
surrounding the CRF is therefore critical to understanding how the visual
system processes arbitrary patterns and natural scenes
(Vinje and Gallant, 2000
).
Most studies of contextual modulation have focused on spatial structure and
stimulus selectivity of the surround field, whereas little attention has been
given to the temporal profile of the modulation. However, the time course of
contextual signals is important because it can constrain both the underlying
circuitry and the functional role of contextual modulation
(Knierim and Van Essen, 1992
;
Lamme, 1995
;
Lee et al., 1998
).
Here we study the time course of orientation-tuned surround suppression
(Blakemore and Tobin, 1972
;
Fries et al., 1977
;
Nelson and Frost, 1978
;
Allman et al., 1985
;
DeAngelis et al., 1994
;
Anderson et al., 2001
), a
prominent form of contextual modulation in the primary visual cortex
(Hubel and Wiesel, 1968
;
De Valois et al., 1985
;
Knierim and Van Essen, 1992
;
Sillito et al., 1995
;
Nothdurft et al., 1999
;
Levitt and Lund, 2002
). It is
widely believed that the extensive horizontal axonal projections within V1,
particularly in layers 2 and 3, offer a conduit for surround suppression
(Gilbert and Wiesel, 1983
;
Allman et al., 1985
;
Gilbert and Wiesel, 1990
;
Born and Tootell, 1991
;
Hirsch and Gilbert, 1991
;
McGuire et al., 1991
;
Gilbert, 1992
;
Knierim and Van Essen, 1992
;
DeAngelis et al., 1994
;
Grinvald et al., 1994
;
Toth et al., 1996
;
Nothdurft et al., 1999
;
Dragoi and Sur, 2000
;
Fitzpatrick, 2000
;
Anderson et al., 2001
;
Hupé et al., 2001b
;
Stettler et al., 2002
).
Alternatively, studies of surround suppression in the context of texture
pop-out and figure-ground segregation
(Knierim and Van Essen, 1992
;
Lamme, 1995
;
Zipser et al., 1996
) found
that surround modulation was delayed relative to CRF-driven responses and
suggested that the delay was consistent with feedback. However, horizontal
propagation within V1 is probably slow
(Grinvald et al., 1994
;
Nowak and Bullier, 1997
;
Bringuier et al., 1999
;
Girard et al., 2001
;
Slovin et al., 2002
), whereas
connections between V1 and higher cortical areas can be fast
(Movshon and Newsome, 1996
;
Nowak and Bullier, 1997
;
Girard et al., 2001
;
Hupé et al., 2001a
).
Therefore, a delay in the arrival of suppression cannot discriminate feedback
from horizontal propagation.
To further resolve mechanisms of surround suppression, we considered the
implications of a simple circuit (Fig.
1) for the timing of suppression. Here, an orientation-tuned
target neuron (triangle at left) is suppressed by an inhibitory neuron (black
circle) that is driven by similarly tuned neurons displaced laterally in the
cortex (triangles at right). We examined two aspects of timing for this
circuit. First, we compared the timing of response onsets and offsets for CRF
stimuli with that for surround stimuli. We recently reported that response
onset latency was consistently longer than offset latency (in >95% of cells
and by 10-20 msec on average) for cortical neurons driven by dynamic CRF
stimuli (Bair et al., 2002
). If
suppression originates from neurons having an onset delay, the onset of
suppression should be delayed relative to its offset. Second, we examined the
relationship between the onset time of suppression and the distance of the
surround stimulus from the CRF. If suppression travels via slow, horizontal
propagation from similarly tuned cells in other cortical columns, then the
latency of suppression should increase for more distant surround stimuli in a
manner that reflects the propagation speed of the horizontal fibers.

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Figure 1. Putative circuit for iso-orientation surround suppression in V1. The target
neuron (left triangle) receives inhibition from a nearby neuron (large filled
circle) that is driven by excitatory neurons displaced laterally in cortex (3
triangles at right) that have orientation tuning similar to the target cell.
Preferred stimuli confined to the CRFs for three excitatory neurons are
indicated by the circular patches of sinusoidal grating shown on the tilted
plane that represents a two-dimensional visual field. Arrows emanating from
the stimuli indicate localized feedforward inputs to the excitatory neurons.
We find that this circuit is insufficient to account for some temporal
features of surround suppression.
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Materials and Methods
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Electrophysiology. We recorded extracellularly from primary visual
cortex of anesthetized, paralyzed macaque monkeys (two Macaca
nemestrina and eight M. fascicularis). Detailed methods for this
type of recording are available in an article by Levitt et al.
(1994
). Experiments typically
lasted 4-5 d, during which anesthesia and paralysis were maintained with
sufentanil citrate (4-6 µg · kg -1 · hr
-1) and vecuronium bromide (Norcuron, 0.1 mg · kg
-1 · hr -1), respectively,
administered in lactated Ringer's solution (8 ml · kg
-1 · hr -1) containing
dextrose (2.5%). Artificial respiration with a mixture of O2,
N2O, and CO2 was maintained with rate adjustments to
keep expired CO2 between 3.8 and 4.0%. Body temperature was
maintained near 37°C with a heating pad. Electroencephalograms and
electrocardiograms were monitored to ensure proper depth of anesthesia. All
procedures conformed to guidelines of the New York University Animal Welfare
Committee.
Tungsten-in-glass microelectrodes
(Merrill and Ainsworth, 1972
)
were advanced with a hydraulic microdrive downward through a craniotomy of
9-10 mm in diameter centered typically 4 mm posterior to the lunate sulcus and
10 mm lateral to the midline. In some experiments, we used a mechanical
microdrive system with quartz-platinum/tungsten microelectrodes (Thomas
Recordings, Marburg, Germany). Action potentials were discriminated using a
hardware dual-window time-amplitude discriminator (Bak) and time-stamped at a
resolution of 0.25 msec. Electrolytic lesions 2 µA for 2-5 sec were made
for histological verification and estimation of the cortical layer. Neurons
were recorded both on the operculum and in the calcarine sulcus [typical
receptive field (RF) eccentricities were 1-6 and 8-20°, respectively].
At the end of experiments, animals were perfused with 4% paraformaldehyde
in saline. Cortical sections of 40 µm were mounted on slides and stained
for Nissl substance with cresyl violet. We reconstructed electrode tracks by
locating the electrolytic lesions and by visualizing tissue damage from the
passage of the electrode. We determined the laminar location of each cell on
the basis of visual inspection of landmarks in the stained sections, as
described by Cavanaugh et al.
(2002
).
Visual stimuli. Visual stimuli were generated by custom software
on a Cambridge Research Systems (Kent, UK) 2/2 board and presented on a
standard cathode ray tube (CRT) at 100 Hz vertical refresh with mean luminance
of 33 cd/m 2. The CRT was placed farther from the monkey's eye for
smaller RFs and closer for larger RFs (range, 80-180 cm). For each cell whose
action potential waveform was well isolated from the noise, we systematically
optimized the orientation, spatial period, and temporal frequency of a sine
wave grating at 100% contrast that drifted for 2-4 sec behind a circular
aperture chosen to approximate the CRF. We then used the smallest patch of
optimal grating that provided a reliable response to find the center of the
RF. Next, we presented stimuli in an interleaved manner consisting of either a
single circular patch of variable diameter or a single annular patch of
variable inner diameter For annuli, the outer diameter was set to the maximum
extent of our screen, which ranged from 10 to 20° of visual angle,
depending on the screen placement. We defined the CRF region to be the
smallest circular patch that produced at least 95% of the maximum response
(for a detailed description, see Cavanaugh
et al., 2002
, where this region is referred to as the
"grating summation field"). We defined the surround region to be
the annulus with the minimum inner diameter that evoked no response above the
spontaneous level. Across the database, the ratio of surround inner diameter
to CRF size had a mean of 0.19, a median of 0.16, and a mode of 0.15
(n = 92).
Our dynamic center-surround stimulus consisted of two patches of drifting
grating that were presented in the CRF and surround apertures defined above.
The stimulus consisted of a random sequence of states
(Fig. 2C) in which
each grating drifted in either the preferred direction or in an orthogonal
direction for one full cycle of sinusoidal modulation. At the end of each
state, each grating was randomly and independently assigned to have either the
preferred or orthogonal direction for the next state. Thus, at each state
boundary (i.e., after each full cycle of drift), each grating either drifted
seamlessly or made a 90° change in orientation and direction.
Opportunities for state transitions occurred simultaneously for the CRF and
surround. The two possible directions of motion for the CRF and surround
created four possible states and 16 state transitions, which occurred at
random. The state transitions of interest for this study are labeled above the
icons in Figure 2C.
When describing states and state transitions, we will refer to orientation and
direction as "preferred" when they are the same as those preferred
by the CRF, even when referring to stimuli that are located in the surround.
Likewise, "orthogonal" always means at 90° to preferred. Thus,
a stimulus in the surround that has the orientation preferred by the CRF is
called preferred even though it is a suppressive stimulus.

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Figure 2. Tuning curves for orientation and size were used to configure our dynamic
center-surround stimulus. A, The mean firing rate of an example
neuron (3 trials, 4 sec/trial) is plotted against the drift direction (in
degrees, relative to preferred) of a sinusoidal grating. Motion was always
orthogonal to the orientation of the grating; therefore, we refer to this as
an orientation tuning curve. Error bars indicate SEM. The stimulus of
preferred orientation is shown by the icon above the peak at zero. The
spontaneous rate for this neuron was zero. B, A size tuning curve
(filled circles) shows mean response versus stimulus diameter for the same
neuron. The optimal size (small icon) was smaller than that in A,
which accounts for larger responses here. The annulus tuning curve (open
circles) shows the response to gratings presented in an annular window versus
the inner diameter of the annulus. The outer diameter was set to fill our
screen. The CRF region (small icon) was the disk that optimized the size
tuning curve. The surround region (large icon) was the annulus with the
smallest inner diameter that did not elicit a response above the spontaneous
firing rate. The arrow marks the inner diameter for the surround region. Icons
here and in A are drawn to scale. C, The icons depict a
succession of six states of the dynamic center-surround stimulus (see
Materials and Methods). The gratings in the CRF (center disk) and surround
(annulus) drifted in either the preferred direction (shown as vertical) or in
an orthogonal direction (horizontal). For clarity, the surround annulus outer
diameter is shown here at 50% of the size determined in B. Below the
icons, orientation is plotted versus time for the CRF (black line) and
surround (gray line). The state transitions of interest here are labeled above
the bent arrows. This sequence was chosen for convenient demonstration; the
actual sequence of transitions was random.
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The dynamic stimulus was presented in trials lasting 30 sec and was
interleaved with a center-alone and a surround-alone control in which the
contrast of the grating in the other aperture was set to zero. There were 4
sec of mean gray between trials. If the surround-alone stimulus yielded a
substantial response to the transition from orthogonal to preferred, the inner
diameter of the annulus was increased to eliminate the response. The temporal
frequency of the grating was sometimes increased from the optimum (if the
optimum was <4 Hz and if doing so did not cause the firing rate to drop to
<90% of optimal) because this increased the number of times that each state
transition was tested. We used temporal frequencies ranging from 3.1 to 25 Hz,
but most cells were tested at either 6.25 or 12.5 Hz. The spatial phase of the
surround grating was set to match that of the center grating. In two cells, we
varied the phase of the surround grating and found that it did not affect our
results. This is consistent with reports that surround suppression is
primarily phase-insensitive (Nelson and
Frost, 1978
; DeAngelis et al.,
1994
).
To test the dependence of surround suppression on the distance of the
surround stimulus from the CRF, we designed a second, simpler experiment that
allowed us to focus on the timing of the onset of suppression. In this
experiment, the optimal drifting grating for the CRF appeared on a mean gray
background for 1 sec, and a surround stimulus appeared 400 msec later and
lasted for 300 msec. Six stimuli were interleaved in a block-wise random
manner with 2 sec of mean gray between stimuli. Five of the six stimuli had
surrounds, which extended from the outer border of our screen to an inner
diameter that varied across stimuli, and the sixth stimulus had no surround.
This allowed us to study the time course of suppression for stimuli at various
distances from the CRF with reference to the time course of the response to
the CRF stimulus when no surround stimulus was imposed.
Data analysis. The response to a particular transition of the
dynamic stimulus was computed by averaging together segments of spike trains
(1 msec resolution) shortly before and after each occurrence of the
transition. The spike trains were aligned to the time of the state transition
before averaging, and the resulting average is referred to as a peristimulus
time histogram (PSTH). PSTHs were filtered in time with a Gaussian of an SD of
2 msec and plotted in units of spikes per second. Responses to the stimuli in
which a surround was flashed on were computed in a similar manner, with the
onset of the stimulus taken as the temporal reference.
We computed the latency of response to a change in the visual stimulus
(e.g., a state transition or the appearance of a surround stimulus) by first
subtracting the reference response (the PSTH in response to no change in the
stimulus) from the response PSTH for the change. We then identified the
maximum of the absolute value of this response difference, and we searched
backward in time from the maximum to the point at which the difference was
equal to 5% of the maximum. The time of this point was defined as the response
latency. Thus, latencies were the times of 5% rise to the peak response
difference. This is the same method that we used previously
(Bair et al., 2002
).
We compared our method with one that chooses the latency to be the point at
which the response difference reaches a criterion statistical significance.
Because the latter requires the response to reach a fixed level, the latency
estimate will grow as the change in response is scaled down. This is
undesirable because later we show that, on average, the strength of
suppression is approximately scaled down for far surround stimuli (see
Results). We tested both latency methods on PSTHs for simulated Poisson spike
trains in which the firing rate changed at a fixed time from an initial level
to a final level in 20 msec (which was typical for our data). As expected, the
5% latency method was substantially less dependent on the final rate than was
the statistical criterion method for both rate increases and decreases. For
changes in the rate approximating the smallest in our data, even the 5%
latency method began to show an increased bias (up to 4 msec longer than the
true latency). However, such small rate changes occurred only for the most
distant surround stimuli, for which the bias operates in a conservative manner
with respect to our conclusions (see Discussion).
We computed the suppression strength, 1 - rs/rp, for
responses to the dynamic center-surround stimulus from the firing rate
(rp) during the preferred stimulus (preferred CRF, orthogonal
surround) and the rate during suppression (rs; preferred CRF,
preferred surround; recall that, in the surround, the orientation preferred by
the CRF is typically the most suppressive). Firing rates were computed in a
time window equal to one period (drift cycle) of the stimulus. This window was
centered in an epoch twice as long, which corresponded to two consecutive
periods of the pertinent stimulus. This ensured that the response was measured
in an epoch that began after the signals arrived in the cortex (i.e., it
accounted for the visual latency).
The spontaneous firing rate was computed in 500 msec epochs preceding the
onset of each trial of the dynamic center-surround stimulus.
We computed a cortical magnification factor (CMF) using the same equation
that we used previously (Cavanaugh et al.,
2002
):
 | (1) |
where E is the receptive field eccentricity in degrees
(Van Essen et al., 1984
;
Tootell et al., 1988
).
 |
Results
|
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Temporal characteristics of surround suppression
By definition, stimuli outside the CRF do not elicit responses; therefore,
we used stimuli in the CRF to evoke responses that the surround could
modulate. We chose drifting (rather than static) sinusoidal gratings because
they maximized the sustained portion of the CRF-evoked response. This worked
well for complex cells, which have relatively unmodulated responses to
drifting gratings. Simple cells, however, responded with strong modulation at
the fundamental temporal frequency, obscuring the temporal profile of surround
suppression and preventing the measurement of response latencies. Therefore,
we present results for complex cells only. There is strong evidence that
surround suppression operates similarly for simple and complex cells
(Dreher, 1972
;
Rose, 1977
;
Kato et al., 1978
;
Nelson and Frost, 1978
;
Walker et al., 2000
;
Mizobe et al., 2001
;
Cavanaugh et al., 2002
;
Levitt and Lund, 2002
).
We studied surround suppression in 92 orientation-tuned complex cells. A
typical orientation tuning curve is shown for an example neuron in
Figure 2A, where
vertically and horizontally oriented icons depict the preferred and orthogonal
stimuli, respectively. After quantitatively optimizing the orientation,
direction, and spatial and temporal frequencies of a circular patch of
drifting grating, we varied the diameter of the optimal patch to compile a
size tuning curve. The example neuron had an optimal diameter of
1°
of visual angle (Fig.
2B, filled circles, small icon). We defined the CRF
region to be the disk of optimal diameter. Stimuli larger than the CRF yielded
smaller, suppressed responses. Cells for which the largest grating gave the
maximum response were considered unsuppressed and were not among the 92
studied here. The CRF size ranged from 0.35 to 3.1° (mean, 1.0°) for
cells 1-6° eccentric and from 0.72 to 4.2° (mean, 1.9°) for cells
>8° eccentric. To define a region that lay outside the CRF, we
presented the optimal grating in annuli of various inner diameters (the outer
diameter was set to the maximum extent of our screen). The annulus tuning
curve (Fig. 2B, open
circles) shows that the response dropped to zero as the inner diameter of the
annulus pulled away from the center of the CRF. We initially defined the
surround region (Fig.
2B, large icon) to be the annulus of smallest inner
diameter that elicited a response no greater than the spontaneous rate (0
spikes/sec for this example cell). In cases in which there was a gray region
between the surround and CRF stimuli, we tested intermediate inner diameters
to verify that the surround stimulus was as close as possible to the CRF
without eliciting a significant excitatory response.
Within the CRF and surround regions, we presented a random, dynamic
stimulus that consisted of a grating drifting at either the preferred
orientation or the orientation orthogonal to preferred. We will refer to these
orientations as preferred and orthogonal regardless of whether they occurred
in the CRF or surround. Figure
2C shows a sample stimulus sequence for six periods of
the dynamic center-surround stimulus. The stimulus icons show the CRF and
surround orientation in each period, which lasted for the time that it took
the gratings to drift one spatial cycle (typically 160 msec; range, 80-320
msec). At the end of the period, each grating was randomly and independently
assigned either the preferred or orthogonal orientation for the next period.
Thus, at each period boundary, a grating either drifted seamlessly or made an
abrupt 90° orientation shift. For example, at the first transition in
Figure 2C, the CRF
stimulus changed from orthogonal to preferred (i.e., horizontal to vertical),
whereas the surround stimulus remained orthogonal. This transition, labeled
onset, usually provoked a strong CRF-driven excitatory response. At the next
transition, suppression, the surround changed to the preferred orientation.
This configuration usually maximized surround suppression. The suppression is
released at the next transition (release), when the surround changes back to
orthogonal. At the fourth transition (offset), the CRF stimulus changed from
preferred to orthogonal. The final transition shown in
Figure 2 involves a
simultaneous change in the CRF and surround stimuli that sets the excitation
of the preferred CRF stimulus against the suppression of the surround. During
the actual stimulus, these five state transitions occurred at random and among
the 16 possibilities (see Materials and Methods).
Our first goal was to assess whether the timing of response onsets and
offsets driven by the CRF and surround were consistent with the circuit in
Figure 1. To do this, we focus
on the responses to the five stimulus transitions just described.
Figure 3 shows the responses
for the example cell, which was typical of the population. The onset of the
preferred CRF stimulus (Fig.
3A, change between left, right icons) caused a sudden
increase in mean firing rate (black line) 52 msec after the stimulus
transition (t = 0). The response curve was computed by averaging
together the spike trains surrounding all occurrences (here, 119) of this
stimulus transition. Also shown is the reference curve (gray line), which is
the average response for two periods of the stimulus depicted by the left icon
(i.e., orthogonal orientation is maintained in CRF and surround). We defined
the response latency to be the time at which the response diverged from the
reference curve by a criterion amount (see Materials and Methods), which is
indicated by the distance between the pair of dots beneath the arrow (see
Fig. 3A legend). For
the opposite stimulus transition, i.e., a change from preferred to orthogonal
in the CRF, a decrease in the rate ensued
(Fig. 3B, black line).
The reference curve (gray line) shows the response to the maintained preferred
stimulus. For clarity, the change in response (response minus reference) is
plotted in the gray inset. The offset latency (29 msec) was
23 msec
shorter than the onset latency, consistent with our previous findings
(Bair et al., 2002
).

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Figure 3. The dynamic center-surround stimulus elicited rapid increases and decreases
in firing rate via the CRF and the surround. In each plot, the black trace
shows the mean firing rate (calibration in A) versus time for the
stimulus transition indicated by the pair of icons. The icons straddle
t = 0, the time of the stimulus transition. A-D, Reference
curves (gray lines) show the response to two consecutive periods of the
stimulus indicated by the left icon. All curves are averages over 100-120
repeats (see Materials and Methods). A, The response increased when
the CRF stimulus changed from orthogonal (shown as horizontal in icons) to
preferred (vertical) but the surround orientation stayed orthogonal
(nonsuppressive). The reference response, 0 spikes/sec, lies on the
x-axis. The arrow labeled onset points to an open circle on the
response curve (black line) and shows the response latency, which is defined
as the time of 5% rise to the maximum difference between the response and the
reference curves (see Materials and Methods). The distance from the open
circle to the black dot (on the reference curve) indicates the 5% response
difference. The onset time is also marked by a vertical dotted line for
comparison with plots below. B, The response decreased when the CRF
stimulus changed from preferred to orthogonal (with orthogonal surround). This
response offset began earlier (arrow) than the response onset in A.
The inset shows the difference between the response and reference curves,
where the dashed line is 0 difference, and the circle marks 5% of the maximum
difference. C, The response to the preferred CRF stimulus was
suppressed by a transition of the surround from orthogonal to preferred. The
decrease was at least as rapid as that for CRF offset in B.
Suppression latency (arrow) is indicated by a vertical dotted line. The inset
shows the difference, as in B. D, The release of suppression, caused
by the surround changing to orthogonal with the CRF stimulus remaining
preferred, occurred at about the same time (arrow) as suppression in C.
E, A simultaneous change in the center and the surround caused a response
(thick line) that followed the CRF onset response (gray dashed line, replotted
from A) until approximately the time of suppression (right vertical
dotted line). Thereafter, the response followed the time course of suppression
(black dashed line, replotted from C).
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The time course for surround suppression is shown in
Figure 3C, where only
the surround stimulus changed. The latency of suppression (indicated by the
arrow) was larger than both the onset and offset latencies for the CRF.
However, the suppression was nearly absolute, and its onset was as abrupt as
the rate changes elicited via the CRF. The release of suppression
(Fig. 3D) was not as
abrupt, but it occurred with a latency similar to that of suppression. The
data in Figure 3, A and
C, imply that the suppressive signal from the surround
took longer to affect the spike rate than did the CRF excitation. A compelling
demonstration of this is provided by the response to the simultaneous change
of the CRF and surround from the orthogonal to the preferred orientation
(Fig. 3E). The
response to this simultaneous transition (thick black line) followed the
response for CRF onset alone (gray dashed line, replotted from
Fig. 3A) for
20
msec (during the period between the vertical dotted lines). Thereafter, the
response was suppressed with a time course consistent with the suppression
observed in Figure 3C
(replotted in Fig. 3E
as the black dashed line).
For each orientation-tuned complex cell that had orientationtuned
suppression, we measured the latencies for the stimulus transitions described
in Figure 3A-D. Their
distributions are plotted in Figure
4. The histograms for the CRF
(Fig. 4A,B) show that
the mean offset latency was shorter than the mean onset latency (arrows show
means). When offset latency was plotted against onset latency for each cell,
nearly all of the points fell below the diagonal
(Fig. 4E), indicating
that stimulus offset consistently affected neuronal output more rapidly than
stimulus onset. This temporal asymmetry, or onset delay, is characteristic of
signals driven by changes between preferred and antipreferred stimuli in the
CRF (Bair et al., 2002
).
However, the same comparison for the surround
(Fig. 4C,D) indicates
that suppressive modulation showed no such asymmetry in timing; the points in
Figure 4F cluster
around the diagonal. This outcome is somewhat surprising in the context of the
circuit for surround suppression shown in
Figure 1. If cells driving the
surround signal have an onset delay, then suppression, which is caused by
response onset in the surround, should have a longer latency than release of
suppression, which is caused by offsets in the surround. The naive prediction
that suppression onset is slower than its release is not borne out in
Figure 4F. If this
simple circuit is fundamental to surround suppression, how can we explain the
lack of onset delay for suppression? Keeping the assumption that signals
arriving at the inhibitory neuron (Fig.
1, black circle) have an onset delay, one possible solution is
that the inhibitory relay somehow delays the release, but not the onset, of
suppression. In Discussion, we describe how such a delay could occur if the
effect of inhibition on the target neuron persists for 10-20 msec after the
inhibitory neuron stops firing.

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Figure 4. Comparison of response timing for CRF and surround signals across cells.
A-D, The distribution of response latencies (see Materials and
Methods) for CRF transitions (gray histograms) and surround transitions (open
histograms) are plotted for 92 cells (arrows show means). On average, CRF
offset (A) was earliest (35 msec; SD, 10 msec). CRF onset
(B) occurred on average 17 msec later (52 msec; SD, 13 msec).
Surround modulation occurred the latest on average [61 and 60 msec for
suppression (C) and release (D), respectively; SD, 17 msec].
E, For each neuron, offset time is plotted against onset time. Almost
all points fall below the unity diagonal, indicating that almost all cells
responded to the offset faster than to the onset of the preferred stimulus in
the CRF. Offset latency also was significantly less variable than onset
latency (SD, 9.7 and 13 msec; F test, p = 0.009).
F, For the surround, suppression time is plotted against release
time. These values were on average not different across cells (paired
t test, p = 0.87; n = 85) and were significantly
correlated (r = 0.70; p <
10-6).
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The second prominent feature of the latency histograms is that suppression
is delayed on average relative to CRF onset
(Fig. 4, compare B,
C). The average delay, 9 msec (SD, 15 msec), was shorter than
the 15-20 msec range reported by previous studies
(Knierim and Van Essen, 1992
;
Nothdurft et al., 1999
). Those
studies, however, used sparse fields of short bars, which may be a weaker
stimulus for surround suppression, and they relied on averages across
populations of cells. Our data allowed a cell-by-cell examination of the delay
and its relationship to other parameters, so we will briefly describe several
major trends and some of their implications.
Plotting suppression latency versus CRF onset latency
(Fig. 5A) shows that
suppression occurred later than CRF onset for most cells, but that for some
cells (points below the diagonal), suppression began before the CRF response.
Examples of responses for two such cells
(Fig. 5A, circled
points) are shown in Figure
5B, where the divergence of the solid black and gray
lines shows the time of onset (same format as
Fig. 3A), and the
divergence of the dashed black and gray lines shows the time of suppression
(similar to Fig. 3C).
In both examples, suppression starts
20 msec before onset. This predicts
a range of behavior for suppressed cells when preferred orientation is
presented simultaneously in the CRF and surround. Some cells should fire
briefly before being suppressed (as in Fig.
3E), whereas others should be suppressed early and may
not respond at all if suppression is strong. This range of behavior is what we
observed across neuronal responses (data not shown) to stimulus transitions
such as that depicted in Figure
3E.

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Figure 5. Latency of suppression relative to CRF onset. A, Suppression
latency is plotted against CRF onset latency for 87 cells. In most cells,
suppression arrived later than CRF excitation, but in some (points below
diagonal line), suppression arrived sooner. B, For two example cells
(A, C, circled points) for which suppression came before onset,
response curves are shown for suppression (suppr.; dashed lines) and onset
(solid lines). Solid lines show response (black) and reference (gray) curves
for the transition like that of Fig.
3A. Dashed lines show the response (black) and reference
(gray) curves for the transition like that of
Fig. 3C. Open circles
mark 5% latencies, as in A and C. C, For each cell,
suppression delay (suppression latency minus CRF onset latency) is plotted
against suppression strength (1 indicates complete suppression; 0, no
suppression). There is a significant negative correlation between suppression
delay and strength (r = -0.48; p <
10-5; n = 87). Strong suppression often
occurred as early as CRF onset, whereas weak suppression was delayed by
30 msec on average. The dashed line shows a linear regression.
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Figure 5A also
reveals a positive correlation between suppression and onset latencies
(r = 0.44; p < 0.0001; n = 87), indicating that,
on average, cells responding early to CRF stimulation also received
suppression early. If CRF and surround signals operated through primarily
independent mechanisms and if suppression entailed extensive pooling, one
might expect the timing of these signals to be uncorrelated. Perhaps the
observed correlation is caused by some delaying operation that acts downstream
from the point where CRF and surround signals are combined. This is possible
if the two signals are combined early in a subset of cells whose outputs incur
delays along their paths to drive other cells downstream within V1.
An unexpected relationship was revealed when suppression delay (suppression
latency minus CRF onset latency) was plotted against suppression strength
(Fig. 5C). Suppression
delay was inversely correlated with suppression strength across cells
(r = -0.48; p < 0.0001; n = 87). The delay was
on average
30 msec longer for weak suppression than for strong
suppression. This relationship was supported by weaker correlations (data not
shown) between suppression strength and the two components of suppression
delay: suppression strength was correlated positively with CRF onset latency
(r = 0.20; p = 0.05) and negatively with suppression latency
(r =-0.34; p = 0.001). Thus, cells with stronger suppression
responded sooner to surround suppression and later to CRF excitation compared
with cells with weaker suppression on average. We also found that suppression
strength was inversely correlated with the spontaneous firing rate (r
= -0.37; p = 0.0006; n = 82; correlation against log of
spontaneous rate). Perhaps one factor, variation in the strength of inhibitory
input across cells, is responsible for all of these correlations. For example,
if the target cell in Figure 1
received more (or stronger) inhibitory synapses, it might suppress faster when
those synapses were activated and might have a lower spontaneous rate because
of greater tonic inhibition. The slower CRF onset could be caused by the CRF
stimulus partially activating the strong inhibitory surround or could result
from greater tonic inhibition.
However, an important possibility to consider is that the negative
correlation between suppression strength and suppression latency could be
caused by variations in our choice of the inner diameter for the surround
stimulus. For surround stimuli placed farther from the CRF, we expect
suppression to be weaker (Jones,
1970
; Nothdurft et al.,
1999
; Levitt and Lund,
2002
). If suppression from more distant stimuli also takes longer
to arrive, as expected for the horizontal propagation model shown in
Figure 1, then a negative
correlation between strength and latency would ensue. The results of the next
section show that such an explanation is unlikely to account for our data.
Time course as a function of distance
An important yet untested prediction of the circuit in
Figure 1, in which surround
suppression arises via horizontal propagation of signals from cells with
similar tuning in nearby columns of visual cortex, is that the distance
traveled should be related to the time of arrival of suppression. To test for
such a relationship, we measured the time course of suppression for surround
stimuli at various distances from the CRF in 31 cells. We presented surround
stimuli for 300 msec during an ongoing optimized CRF stimulus. We used brief
stimuli to maximize the number of repeated trials and thereby increase the
accuracy of our timing estimates. Figure
6A, right panel, depicts the stimulus at an instant when
the surround was present. The surround grating extended from the outer edge of
the video display to an inner circular border that was concentric with the
circular CRF stimulus in the center of the display. The diagram shows the far
surround stimulus (that most remote from the CRF), whereas the two dashed
circles mark the inner borders for a mid surround (at an intermediate
distance) and the near surround (that closest to the CRF).

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Figure 6. The time course of suppression is shown for surround stimuli that lie at
several distances from the CRF for two example neurons. A, The
stimulus display (right) shows the CRF stimulus, which was a central patch of
grating optimized for the CRF, and the far surround stimulus, which was a
grating extending from the edges of the display to a circular inner border.
The dashed circles mark inner borders for two other surround stimuli: the mid
and near surrounds. The CRF stimulus appeared for 1 sec starting at t
= 0, and the surround stimulus appeared for 300 msec starting at t =
400 msec (timing bar at bottom). The preferred orientation and spatial
frequency were as shown. The mean firing rates (n = 20 trials,
convolved with Gaussian; SD, 4 msec) are shown for the near, mid, and far
surrounds (thick to thin lines). The response to the CRF stimulus alone is
shown by the dotted line. The near surround strongly suppressed the response
to the CRF (thickest black line; arrows indicate onset of suppression). The
suppression caused by the mid surround initially had a time course similar to
that of the far surround but became weaker after 50 msec. The far
surround suppression (thin solid line) was strikingly transient but did not
deviate substantially in the first 50 msec from the near surround suppression.
The square gray inset shows a blowup of the curves around the time of
suppression onset. For this cell, the onset of near suppression occurred at 65
msec compared with 48 msec for the onset of the CRF response. B, Data
for a second example neuron are formatted as in A. Averages are of 30
trials. As in A, the suppression became more transient as the
surround withdrew from the CRF, but unlike the previous example, the latency
of suppression consistently increased as the surround withdrew. The onset of
near suppression occurred at 46 msec, which was earlier than the onset of the
CRF response at 50 msec.
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Responses to four stimulus conditions are shown in
Figure 6A for one
example neuron. The dashed line shows the response to the CRF stimulus
presented alone, and the three solid lines, from thick to thin, show the
responses to near, mid, and far surround stimuli, respectively. The thick line
shows that the firing rate of this cell was strongly suppressed during a
period of
300 msec that corresponded to the epoch when the near surround
was present (allowing for 50 msec response latency). For surrounds that were
farther away (thinner lines), the suppression was weaker on average during the
300 msec interval. However, the onset of suppression occurred at approximately
the same time (arrows; inset shows blowup), and the suppression was initially
strong (100%) for all surrounds. Figure
6B shows results for a second example neuron that
displayed a systematic change in suppression latency with distance of the
surround (curves between arrows; inset shows blowup). For this cell,
suppression from more distant surrounds arrived later. Like the first example
cell, suppression was weaker and displayed a strong transient component for
more distant surrounds.
For each complex cell, we computed the change in suppression onset time,
t, associated with the change from the near to far surround.
In particular,
t was the onset latency for far suppression
minus that for near suppression, where onset latency was defined as the time
at which suppression reached 5% of its maximum value (see Materials and
Methods). We also estimated the associated change in distance,
x, that the signals would have to travel if they propagated
laterally within V1. We multiplied the distance between the inner borders of
the near and far surrounds (i.e., the number of degrees of visual angle that
the surround receded) by the cortical magnification factor
(Van Essen et al., 1984
;
Tootell et al., 1988
) that was
appropriate for the eccentricity of the receptive field (see Materials and
Methods, Eq. 1). Figure
7A shows these values for all 31 neurons tested. The two
circled points show values for the example cells of
Figure 6. The point for
Figure 6A,
x = 2.15 mm and
t = 1 msec, fell near the
vertical line at
t = 0, indicating that suppression from the
far surround required little or no additional time to arrive compared with
suppression from the near surround. For the example cell of
Figure 6B,
x = 1.84 mm, and
t = 22 msec. The effective
propagation speed in this case is just under 0.1 m/sec, which is indicated by
the dashed line of the shallowest slope in
Figure 7A.

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Figure 7. Dependence of latency and time course of surround suppression on surround
distance and its implications for propagation velocity. A, The
x-axis plots the latency for far suppression minus that for near
suppression, t; see Results). The y-axis plots the
cortical distance associated with the change in radius between the near and
far surrounds ( x; see Results). Points show data for 31
neurons. The dashed lines mark propagation speeds of 1, 0.1, and 0.2 m/sec.
The vertical line indicates zero delay, i.e., instantaneous propagation.
B, The propagation speed for suppression implied by the data in
A was computed for each cell by dividing the cortical distance by the
delay time. The bar at the right marked >1 represents all cells that had
propagation speeds of >1 m/sec and includes the six cells that had
t of <0 in A. The shading indicates the estimated
laminar location (see Materials and Methods) of the cells within the cortex.
Histological reconstruction was not available for two cells (diagonal lines).
C, Average suppression strength is plotted as a function of time. For
each cell, suppression versus time was computed for each of five surrounds by
subtracting the suppressed response from the response to the CRF alone. This
difference was expressed as a percentage of the unsuppressed (CRF-alone)
response. All curves for a cell were aligned to the latency of that cell for
near suppression. The average onset latency for near suppression was 46 msec.
The solid line shows the average near surround curve for all cells. The open
and filled circles mark the time of 50% suppression (at 7 msec) and the time
of peak suppression (85% at 41 msec) on the near surround curve. Lines with
shorter dashes show averages for more distant surrounds. The average
suppression curve for the far surround (line with shortest dashes) has a
significant transient component that exceeds 40% suppression from 30 to
70 msec. Suppression from 200 to 300 msec was weak for far surround stimuli.
The region around t = 0 (main plot, gray bar) is expanded at the
right.
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If horizontal axonal projections mediate surround suppression, we would
expect our data to reflect their conduction speed. Several studies suggest
that propagation speed in such thin, unmyelinated fibers is
0.1-0.2 m/sec
(Grinvald et al., 1994
;
Bringuier et al., 1999
;
Girard et al., 2001
;
Slovin et al., 2002
). Dashed
lines mark these speeds in Figure
7A. Almost all of our data fall above these lines,
suggesting that iso-orientation surround suppression must be carried by a
mechanism that does not rely on the slow propagation associated with
long-range horizontal connections. The propagation speed associated with each
point is plotted in a frequency histogram in
Figure 7B, where
shading indicates the cortical layer assigned to each cell from histological
reconstruction of the recording sites. Points near and to the left of the
y-axis (Fig.
7A) account for the 12 cells having speeds of >1 m/sec
(Fig. 7B). These
points, distributed widely throughout the depth of the cortex, imply an
unprecedented speed for horizontal propagation. A more tenable hypothesis,
considered in Discussion, involves feedback from cells with large receptive
fields.
It might be argued that we overestimated propagation speed because some
cells driving the surround suppression had RFs that overlapped the inner edge
of the surround stimulus and hence were closer to the center of the CRF.
However, such cells probably did not contribute to the short latency of
suppression. Rossi et al.
(2001
) showed that neuronal
response latency increased precipitously as stimuli were withdrawn from the
center of the CRF. Their Figure 9 shows that a stimulus receding by
0.5° at a position 0.5° from the CRF center leads to a delay of
10 msec. This is consistent with delays on the order of 10 msec/° shown in
intracellular recordings in V1 by Bringuier et al.
(1999
). Thus, signals from any
cell closer than one centered at the inner edge of the surround stimulus would
be delayed. Furthermore, the weakening of suppression with distance should
lead us to overestimate its latency by several milliseconds (see Materials and
Methods). These factors suggest that our estimates of effective propagation
speed are not inflated.
The most striking change that we observed for more distant surrounds was
neither the change in latency nor the expected weakening of suppression.
Rather, the examples in Figure
6 show that responses to far surround stimuli were dominated by a
transient component that was less evident for near surrounds. Most cells (22
of 31) showed clear signs that the sustained component of suppression weakened
more than the initial transient component for far surrounds, but several
others (4 of 31) had strictly sustained suppression that decreased evenly in
time for surround stimuli lying farther from the CRF. To quantify this trend
across the database, we computed for each cell the average suppression as a
function of time for the response to surrounds at each of five successive
distances. All resulting curves for a given cell were shifted by the latency
of near suppression onset for that cell, making t = 0 the time of
near suppression onset. The time-shifted curves for near suppression were
averaged across all cells to produce the near surround average in
Figure 7C (solid
line). This plot shows that suppression peaked at 85% at t = 41 msec
(filled circle). The conventional, steady-state method of estimating
suppression from the size tuning curve yielded a significantly smaller value
of 58% (SEM, 5%, computed as the ratio of response for the optimal size to the
response asymptote for large stimuli;
Cavanaugh et al., 2002
). The
average of all curves for far surround stimuli is also shown (line with
shortest dashes). The average far surround curve peaks at
45% suppression
around 30-70 msec. Its peak width partly reflects variability in the timing of
narrow transients for individual cells. In the second half of the 300 msec
test period, the far surround curve drops to around 15% suppression, less than
half of its peak value. By comparison, the near surround curve is less
transient, decreasing by only a small fraction of its peak value. Average
curves for the three successive mid surrounds are also plotted, and these show
a systematic progression from near to far in which suppression in the latter
half of the 300 msec period weakens with distance more than does the
suppression in the early part of the period.
It is worth emphasizing that curves for each cell in
Figure 7C were aligned
to its time of near-suppression onset, yet the population averages all show
rapidly increasing suppression starting at time 0 (or a few milliseconds
thereafter for the far surround curve). This reinforces the observation made
above that, for a substantial fraction of cells, there was very little change
in timing of the onset of suppression with distance from the CRF.
Finally, an important aspect of our study is that we tested only the part
of the surround that did not significantly overlap the CRF. For each cell, we
attempted to move the inner diameter of our surround stimulus closer to the
CRF but found that the surround stimulus then elicited a CRF response that
obscured the time course of suppression. On average, our surround stimuli were
separated from the CRF stimulus by 28% of the CRF diameter Therefore, we
cannot say how the timing of suppression depends on distance within the very
near surround. However, we used high-contrast stimuli, which minimize the
apparent size of the CRF (Kapadia et al.,
1999
; Sceniak et al.,
1999
; Cavanaugh et al.,
2002
), and therefore have tested as close to the CRF as our
methods allow.
 |
Discussion
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We will first briefly discuss two basic novel findings about the time
course of surround suppression: that, on average, more strongly suppressed
cells were suppressed sooner and that suppression had a transient component
that was prominent for surround stimuli lying farther from the CRF. We will
then discuss the answers to the two questions that motivated this study.
First, is the asymmetry in the timing of CRF response onset and offset
reflected in the timing of surround suppression? Second, how does the timing
of suppression depend on the distance of the surround stimulus from the CRF?
The answers were not the ones anticipated for the simple circuit of
Figure 1. We will argue that
the lack of onset-offset asymmetry for surround suppression may be accounted
for in terms of the dynamics of signals at the inhibitory relay, whereas the
effectively rapid propagation of signals from distant surround stimuli
constrains the circuitry carrying the excitatory responses that drive the
inhibition.
Delay of signals from the surround relative to those from the
CRF
The delay of surround suppression with respect to CRF excitation has been
reported previously to range from 15 to 60 msec
(Knierim and Van Essen, 1992
;
Lamme, 1995
;
Zipser et al., 1996
;
Lee et al., 1998
;
Lamme et al., 1999
; Nothdurft
et al., 1999
,
2000
;
Hupé et al., 2001b
).
Our measurements revealed that this delay varies systematically across cells:
the delay was on average 30 msec longer for weakly suppressed cells compared
with strongly suppressed cells. In strongly suppressed cells, suppression
often arrived earlier than CRF excitation. It is possible that variation in
the sizing of surrounds caused some to be near, giving strong, early
suppression, and others to be far, giving weak, late suppression. It is also
possible that our method of measuring timing was biased to find that weaker
suppression came later. However, our results on the distance dependence of
suppression argue strongly against these explanations. In those experiments,
suppression became substantially weaker as we moved the surround great
distances from the CRF, yet in only 2 of 31 cells did this yield a delay of
>25 msec. Variations in surround placement in our onset-offset experiments
could be only a small fraction of distances used in the distance dependence
experiments. They cannot account for the 30 msec change in delay with
suppression strength. Therefore, we conclude that the relationship between
suppression strength and timing reflects a property of the cortex. Perhaps
iso-orientation suppression is carried by multiple pathways, some being more
direct, thus faster, and more powerful than others.
Onset and transience of surround suppression
Iso-orientation surround suppression achieved its maximum strength on
average within 50 msec from its onset (Fig.
7C). Thus, despite its modulatory nature, surround
suppression can act as suddenly as the direct-driving CRF signals. In addition
to its abrupt onset, suppression often had a strong transient component that
was revealed as surround stimuli were placed farther from the CRF. We had
expected suppression from distant surrounds to be weaker
(Jones, 1970
;
Hess et al., 1975
;
Nothdurft et al., 1999
;
Levitt and Lund, 2002
), but
past studies of the time course of surround signals did not mention a
transient component (Knierim and Van
Essen, 1992
; Lamme,
1995
; Zipser et al.,
1996
; Lee et al.,
1998
; Lamme et al.,
1999
; Nothdurft et al.,
1999
,
2000
). However, those studies
used different stimuli and focused on population-averaged responses. Further
characterization of the set of stimulus conditions required to elicit
transient suppression is necessary before we can understand its functional
significance.
There is no onset delay for surround suppression
We previously reported that neurons in the visual system have an
onset-offset asymmetry in their CRF-driven responses
(Bair et al., 2002
). This holds
for the CRF-driven responses here: CRF onset latencies were on average 17 msec
longer than offset latencies. In the circuit of
Figure 1, the neurons that
generate the surround signal should also have the onset delay because their
CRFs experience orientation changes similar to those in the center. If the
inhibitory relay retains the timing of the surround signal, then the onset of
suppression should be delayed because it is driven by delayed responses to
preferred orientation in the surround. Contrary to this prediction, we found
no timing difference between the onset and release of suppression. Perhaps we
observed no timing asymmetry for suppression because the orientation-tuned
signal that drives suppression has no asymmetry. This might occur if
suppression originated from a subset of cells that lacked the onset-offset
asymmetry; however, very few cells fit this criterion.
Alternatively, it is possible that the onset delay exists in the signal
that drives suppression but is canceled by the inhibitory relay. How this
could happen is depicted by the four traces in
Figure 8A. Trace F
plots the level of activity in the CRF-driven feedforward inputs to the cells
(S) that supply the surround signal. The S cells are activated (high state,
trace S) by F after a delay (light gray band) that corresponds to their CRF
onset delay (17 msec on average). Trace I shows that the response of the
inhibitory relay follows its excitatory input from S with little delay. This
is supported by reports that inhibitory neurons are activated very rapidly and
can retain the temporal structure of their inputs
(Simons, 1978
;
Swadlow, 1989
;
Connors and Gutnick, 1990
;
Tama's et al., 1997). The target neuron (T) receives the suppression from I
and suppresses rapidly after I activates. This sequence of events defines the
period marked suppression (Fig.
8A, bottom left). If either the inhibitory neuron or the
target neuron had not followed its inputs rapidly, suppression onset would
have occurred even later than shown. Now, consider the timing of the release
of suppression. If the response of T recovered rapidly (dashed line) when I
inactivated, then the delay to release would be shorter than that to
suppression onset (see short bar marked release and associated dashed lines).
However, if the inhibition persisted through the period marked by the light
gray band, then suppression and release latencies would be similar (solid
lines, timing bars). In particular, if the effect of inhibition on the target
cell persisted for a time equal to the onset delay for the CRF (17 msec on
average), then the onset delay would be canceled for surround suppression. The
required time is similar to the half-width of GABAA IPSPs, 16 msec,
reported in the cat visual cortex
(Tamás et al., 1997
).
In fact, it is possible that the CRF onset delay is itself the result of
inhibition that persists after the removal of the orthogonal CRF stimulus.
This inhibition might work by a mechanism similar to surround suppression and
could use the same inhibitory neurons.

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Figure 8. Refinements to the model shown in Figure
1 to account for the timing of the surround response. A,
This hypothetical timing diagram can account for the presence of the onset
delay for the CRF and its absence for the surround. The circuit (at the left)
consists of a population of surround neurons (S), which inhibit a target
neuron (T) via an inhibitory relay (I). The target and surround neurons have
the same orientation preference. The four thick traces show the feedforward
input (F) and responses versus time for three elements in the circuit. Active
and inactive states are shown by high and low values, respectively. The CRF
input to the target neuron (T) is assumed to be active (preferred stimulus) at
all times (not plotted). The feedforward input driving the surround neurons is
meant to indicate the timing of signals as they arrive in cortex; i.e., the
subcortical delay is not represented. When the input is high, the surround
stimulus is in the preferred configuration. The response of the surround
neurons (S) has a delayed onset (light gray band), but response offset has
little delay. Thus, the top traces (F, S) show the onset-offset asymmetry for
neurons responding to their CRF stimulus (i.e., the bar marked offset is
shorter than that marked onset). The response of the inhibitory relay (I)
follows rapidly the signal from S. The response of the target neuron (T) is
initially high (its CRF stimulus is preferred; data not shown) and is then
suppressed by the inhibitory signal. When inhibition from I turns off, the
response of the target neuron should recover rapidly (dashed line). However,
if the recovery of the response of T were delayed (light gray band), then the
latency of its release from suppression (release bar) would be equal to its
latency for suppression onset (suppression bar), consistent with our
observations. B, Cells (triangles) in V1 (bottom gray box) project
via fast axons (arrows) to a higher visual area (top gray box) where neurons
have larger CRFs created by convergent input. If cells from the higher area
project back (dotted line) directly or indirectly to local inhibitory neurons
in V1 (black circle), then suppression from far regions of the surround could
arrive on target cells in V1 with little additional delay compared with
suppression from the near surround. This could explain the data points in
Fig. 7A that fall
along the vertical line for zero delay.
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Thus, we hypothesize that the persistence of GABAA inhibition
may be responsible for both the onset delay observed for the CRF and the lack
of a similar delay for surround suppression. Such an asymmetry is consistent
with the notion that inhibition has veto power over excitation.
Suppression delay versus distance
We measured the change in latency of suppression as the surround stimulus
was moved farther from the CRF. For many cells, suppression was somewhat
delayed for more distant surrounds, but for a substantial fraction of cells,
there was very little delay, even for surround stimuli that were far from the
CRF and evoked relatively weak suppression. The apparent propagation speed of
suppression was >1 m/sec for 40% of cells, whereas only 1 of 31 cells
yielded a speed <0.2 m/sec. This effectively rapid propagation occurred in
cells recorded in layers 2 and 3, layer 4, and deep layers. The most widely
cited circuit for iso-orientation surround suppression involves long-range
horizontal projections (Allman et al.,
1985
; Gilbert and Wiesel,
1989
), which can extend for up to a 3.5-4.5 mm radius in layers 2
and 3 of macaque V1 (Angelucci et al.,
2002
; Stettler et al.,
2002
). Grinvald et al.
(1994
)
(Slovin et al., 2002
)
described a wave of optically imaged activity that traveled at 0.09-0.25 m/sec
across V1 and suggested that it was related to surround suppression carried by
long-range projections. Other studies reported that slowly conducting
horizontal axons carry information at typically 0.1-0.2 m/sec across the
visual cortex (Bringuier et al.,
1999
; Girard et al.,
2001
). Our results strongly suggest that this form of slow
propagation across the visual cortex cannot account for iso-orientation
suppression. It follows that if long-range horizontal connections underlie
slow propagation, they are insufficient to mediate the suppression that we
have observed.
Can faster propagation within V1 explain our data? Higher conduction speeds
have been found using electric shock. In cat cortical slices, Hirsch and
Gilbert (1991
) reported 0.3
m/sec propagation in the upper layers over short distances (
1 mm). Girard
et al. (2001
) reported 0.3
m/sec in upper layers and 1.0 m/sec in lower layers in monkeys across <2
mm; however, they stated that most horizontal fibers conduct slowly,
0.1
m/sec, in agreement with others (Grinvald
et al., 1994
; Bringuier et al.,
1999
; Slovin et al.,
2002
). Furthermore, recent studies showed that horizontal
connections within V1 are limited in extent to 3.5-4.5 mm
(Angelucci et al., 2002
;
Stettler et al., 2002
), yet
significant suppression came from >4 mm away from the CRF center in 23 of
31 cells (median, 7.5 mm; range, 2-15 mm) for which we estimated propagation
speed. This is consistent with earlier estimates that suppression in most
cells extended to at least 7 mm in the cortex
(Cavanaugh et al., 2002
). In
terms of RF size, Levitt and Lund
(2002
) reported a median
diameter of 7.1° for suppression in parafoveal recordings, which agrees
with our median diameter of 6.6° (n = 21, parafoveal cells).
Synaptic relays could enhance the reach of horizontal connection, but each
relay would add an integration time of
5-20 msec
(Nowak and Bullier, 1997
;
Azouz and Gray, 1999
). In
summary, the documented speeds and distances for horizontal connections in V1
make them poor candidates for explaining our data.
Alternatively, rapid effective propagation of suppression could result from
feedback from visual areas with large RFs, such as V2 or MT
(Allman et al., 1985
;
Knierim and Van Essen,
1992
;
Lamme, 1995
,
Zipser et al., 1996
;
Nothdurft et al., 2000
;
Hupé et al., 2001a
;
Jones et al., 2001
) (but see
Hupé et al., 2001b
). A
feedback circuit is shown in Figure
8B, where fast axons (arrows) carry convergent inputs to
create large CRFs in extrastriate cells (triangle, upper gray band). Feedback
(dotted line) from such cells in an area remote from the foveal portion of V1
is an elegant geometrical way to achieve a surround latency that is mostly
independent of distance. Area MT is well suited for this. Connections from V1
to MT conduct at
10 m/sec (Movshon
and Newsome, 1996