The Journal of Neuroscience, August 20, 2003, 23(20):7621-7629
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Developmental Modulation of Retinal Wave Dynamics: Shedding Light on the GABA Saga
Evelyne Sernagor,1
Carol Young,1 and
Stephen J. Eglen2
1School of Neurology, Neurobiology, and
Psychiatry, Medical Sciences, University of Newcastle upon Tyne, Newcastle
upon Tyne, NE2 4HH, United Kingdom, and 2Department of
Anatomy and Neurobiology, Washington University School of Medicine, St. Louis,
Missouri 63110
 |
Abstract
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Embryonic spontaneous activity, in the form of propagating waves, is
crucial for refining visual connections. To study what aspects of this
correlated activity are instructive, we must first understand how their
dynamics change with development and what factors trigger their disappearance
after birth. Here we report that in the turtle retina, GABA, rather than
glutamate and acetylcholine, influences developmental changes in wave
dynamics. Using calcium imaging of the ganglion cell layer, we report how
waves switch from fast and broad, when they emerge, to slow and narrow a few
days before hatching, coinciding with the emergence of excitatory
GABAA receptor-mediated activity. Around hatching, waves gradually
become stationary patches, whereas GABAA shifts from excitatory to
inhibitory, coinciding with the upregulation of the cotransporter KCC2,
suggesting that changes in intracellular chloride underlie the shift.
Dark-rearing from hatching causes correlated spontaneous activity to persist,
whereas GABAA responses remain excitatory, and KCC2 expression is
weaker. We conclude that GABA plays an important regulatory role during the
maturation of retinal neural activity. Using a simple and elegant mechanism,
namely the switch from excitatory to inhibitory, GABAA
receptor-mediated activity is necessary and sufficient to cause retinal waves
to stop propagating, ultimately leading to the disappearance of correlated
spontaneous activity. Moreover, our results suggest that visual experience
modulates the GABAergic switch.
Key words: retinal waves; retinal development; GABA; calcium imaging; dark-rearing; visual experience; spontaneous activity
 |
Introduction
|
|---|
Embryonic retinal ganglion cells (RGCs) fire in spontaneous bursts of
action potentials (Sernagor et al.,
2001
) that are correlated between neighbors
(Maffei and Galli-Resta, 1990
;
Zhou, 1998
;
Grzywacz and Sernagor, 2000
),
resulting in waves propagating across the ganglion cell layer (GCL) and the
inner nuclear layer (INL) (Meister et al.,
1991
; Wong et al.,
1993
,
1995
;
Feller et al., 1996
;
Wong et al., 1998
; Sernagor et
al., 2000
,
2001
;
Zhou and Zhao, 2000
). These
waves are believed to encode unique spatiotemporal patterns that could guide
Hebbian development of visual connections
(Katz and Shatz, 1996
;
Crair, 1999
;
Eglen, 1999
;
O'Donovan, 1999
;
Penn and Shatz, 1999
;
Wong, 1999
).
Pharmacological studies indicate the relative importance of different
neurotransmitters in wave propagation. Nicotinic cholinergic neurotransmission
is necessary to generate RGC-correlated spontaneous bursting activity (SBA)
(Sernagor and Grzywacz, 1996
,
1999
) and to propagate waves
at early developmental stages (Feller et
al., 1996
; Catsicas et al.,
1998
; Wong et al.,
1998
; Bansal et al.,
2000
; Sernagor et al.,
2000
; Wong and Wong,
2000
; Zhou and Zhao,
2000
). Later, glutamate modulates the waves
(Wong et al., 1998
;
Bansal et al., 2000
;
Sernagor et al., 2000
;
Wong and Wong, 2000
;
Zhou and Zhao, 2000
). During
the switch, acetylcholine influences the wave size, whereas glutamate
modulates their speed (Sernagor et al.,
2000
). Nicotinic cholinergic neurotransmission also switches to
muscarinic receptor-driven activity in neonatal rabbit
(Zhou and Zhao, 2000
).
Finally, GABAA and glycinergic responses shift from functionally
excitatory to inhibitory at P15-P18 in ferret RGCs
(Fischer et al., 1998
),
whereas a prenatal excitatory glycinergic drive becomes inhibitory in rabbit
(Zhou, 2001
).
Surprisingly little effort has concentrated, however, on long-term
developmental changes in wave dynamics, and little is known about the factors
causing waves to disappear after birth. Light itself may be important, because
SBA disappears shortly after eye opening in mammals
(Wong et al., 1993
), and it
persists in dark-reared turtles (Sernagor
and Grzywacz, 1996
).
If retinal waves change during development, then the way they instruct the
refinement of connections in the visual system could also change
(Shatz, 1996
). Studies making
chronic gross changes to both the amount and the pattern of retinal activity
(Penn et al., 1998
;
Rossi et al., 2001
;
Stellwagen and Shatz, 2002
)
show profound changes in the organization of retinal targets. However, to
understand how wave dynamics guide the precise carving of visual connections
such as retinotopy, the first step is to know how waves change during
development and to elucidate the cellular mechanisms underlying these
changes.
The goal of this study was to document how the dynamics of turtle retinal
waves change with development and to elucidate the cellular mechanisms
underlying these changes. Because we already know that visual experience is
necessary for SBA to disappear in turtle RGCs
(Sernagor and Grzywacz, 1996
),
this model is ideal for investigating how light may modulate the disappearance
of spontaneous correlated activity.
Parts of this study have appeared previously
(Sernagor and Mehta, 2001
;
Sernagor et al., 2001
) and in
abstract form (Sernagor and Eglen,
2001
; Sernagor,
2002
).
 |
Materials and Methods
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Surgical procedure, dye labeling of the retina, and drug
application. Our study was performed on the turtle species Pseudemys
scripta elegans. Embryonic ages were determined according to specific
staging criteria (Yntema,
1968
). S22 corresponds to
3 weeks before hatching, S25, to 1
week before hatching, and S26 to the hatching process. Embryos were kept at
29°C in a dark incubator. Newly hatched turtles were immediately
transferred to water tanks kept at 28°C, either in 12 hr light/dark cycles
(for normal rearing) or in constant darkness. The surgical procedures are
described elsewhere (Sernagor and
Grzywacz, 1995
). RGC retrograde loading with calcium green dextran
(CGD) was similar to our method used in the chick
(O'Donovan et al., 1993
;
Sernagor et al., 2000
), with
the difference that eyecups were incubated overnight in Ringer's solution
(Sernagor and Grzywacz, 1995
)
at room temperature. After isolation, retinas were mounted, GCL facing up,
onto gray blotting paper (Millipore, Bedford, MA) and transferred to the
experimental chamber onto the stage of an upright microscope (AX70; Olympus
Optical, Tokyo, Japan). The chamber was continuously perfused (2-5 ml/min)
with oxygenated Ringer's solution (containing KCl 4.9 instead of 2.9
mM, to increase background spontaneous activity) kept at
26-28°C.
Pharmacological blockers (Sigma, St. Louis, MO; or Tocris Cookson, Bristol,
UK) were bath-applied through the perfusate. GABA, however, was applied with a
micropipette in single puffs of 50 µl of a 5 mM solution to
avoid receptor desensitization. Because the volume of the bath is
1 ml,
the final concentration of GABA was 100 µM. This peak
concentration was reached only briefly because the perfusion was kept on
during the application of the drug. GABA was always applied near the chamber
inflow and then diffused toward the retina placed in the center of the
chamber, with the imaged region
1.2 cm away from the inflow. As control,
puffs of Ringer's solution had no effect on spontaneous activity (N =
3), suggesting that merely puffing did not trigger activity by mechanical
stimulation. Drug washout led to full activity recovery within 15-30 min.
Analysis of calcium transients. The imaging techniques and
analysis of the calcium transients were similar to those used in our previous
study in the chick (Sernagor et al.,
2000
). Briefly, RGCs labeled with CGD were viewed at 20x
(which is sufficient to resolve individual cells) (see
Fig. 1) over a field of view of
600 x 600 µm 2, which represents approximately a
fifth of the retina. Fluorescence changes were detected using a Video Rate
Intensified CCD camera (Princeton Scientific Instruments, Monmouth Junction,
NJ) and recorded continuously (25 frames/sec) onto videotape while
simultaneously viewed with the imaging software Meta-Morph (Universal Imaging
Corporation, Downingtown, PA).

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Figure 1. Retinal waves in the turtle embryo. A, Raw image (averaged over 60
frames) of calcium green dextran-labeled GCL from a whole-mount S24 retina.
Each dot represents a labeled RGC. The white circles delimit three cells whose
activity is illustrated in B. B, Video rate recording of increases in
fluorescence intensity ( F/F) during a spontaneous
wave of activity for the three cells demarcated in A. The horizontal
dotted line shows the threshold for activity onset. The vertical line shows
the onset time for cell 1, the first to become recruited in the wave. Delays
to onset increase from cell 1-3, indicating wave propagation. All three cells
exhibit recurring outbursts of activity during the wave, indicating the
quality of temporal resolution in our recordings. C, Time-lapse
images of a Ca2+ wave in a S22 retina. The background
fluorescence has been subtracted from the images, so that only changes in
fluorescence are apparent. Each image illustrates a single video frame
obtained at a particular time elapsed from the beginning of the recording
(indicated in seconds in the top left side of the image). The wave propagates
from top (time 0) to bottom. Scale bar, 250 µm.
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Episodes of activity were digitized (MetaMorph) to measure the average
fluorescence over time in many cells, typically 150-200 per retina
(Sernagor et al., 2000
). Each
event was normalized such that the mean of the first five frames of activity
was 100%; we then measured deviations from this baseline. Traces were smoothed
using an exponential smoothing function (half-life 3.5 frames). The onset time
of a calcium elevation within a trace was the time at which the trace exceeded
20% of its peak value. To calculate the relative onset plots, a cell that was
activated early in a wave was chosen as the reference cell. Then, for every
other active cell, we plotted the difference in onset time for that cell and
the reference cell as a function of the distance between them. The first-order
moments (Sernagor et al.,
2000
) relative to the wave center, calculated parallel and
perpendicular to the dominant orientation, were averaged to estimate wave
spatial extent. Wave speed was calculated by dividing the difference in onset
times for two cells by the distance between them and averaging over several
cell pairs (at least five pairs per wave)
(Sernagor et al., 2000
).
Immunocytochemical localization of KCC2. Eyes were fixed in 1% PBS
paraformaldehyde for 1 1/2 hr and subsequently washed in 0.1 M PBS.
Eyecups were cryoprotected in 30% sucrose overnight at 4°C, embedded in a
mixture of gelatin and O.C.T. (Sakura, The Netherlands) and frozen in
isopentane cooled in liquid nitrogen. Serial cross-sections (20
µM) were prepared using a Microm HM560 cryostat, mounted on
chrome-alum-gelatin-subbed slides and stored at -40°C. Alternate 10 µm
sections were collected from the same eyecups for hematoxylin and eosin
(H&E) staining (see below).
We used a standard immunolabeling protocol
(Vu et al., 2000
). All
antibodies were diluted in PBS containing 3% bovine albumin and 0.1 M
L-lysine monohydrochloride. Sections were soaked for 10 min in 0.1%
Triton X-100 in PBS followed by a brief rinse in PBS. They were incubated
overnight at 4°C in 1:200 diluted rabbit polyclonal anti-KCC2 primary
antibody (Upstate Biotechnology, Lake Placid, NY) raised against a 111 amino
acid fusion protein (Payne et al.,
1996
). After three washes (10 min each) in PBS, slides were
incubated for 2 hr at room temperature in tetramethylrhodamine-conjugated
swine anti-rabbit IgGs (DakoCytomation, Cambridge, UK), washed in PBS and
mounted in Vectashield (Vector Laboratories, Peterborough, UK). Negative
controls consisted of alternate sections from the same retinas from which the
primary antibody was omitted. Sections were viewed at 40x using a Leica
DMRA fluorescence microscope, and images from sections prepared on the same
day were captured at the same exposure (1 sec) with a SPOT digital camera
(Diagnostic Instruments Inc., Sterling Heights, MI) using MetaMorph. KCC2
labeling bandwidth [thickness of labeling within the inner plexiform layer
(IPL)] and labeling intensity (gray levels) were measured in MetaMorph by
drawing rectangles (length = KCC2 bandwidth in IPL; width = 25 pixels)
perpendicular to the IPL. These rectangles were drawn only in places where
there was a clear delimitation between labeled and nonlabeled areas (sometimes
the labeling is not strictly limited to the IPL, it is often seen on the
membrane of cell bodies) (see Fig. 8
A,B). For each section labeled with KCC2 antibodies, we
processed an adjacent section with hematoxylin and eosin to measure the entire
IPL thickness (see next section). Values in
Figure 8 E were
obtained by normalizing (measured with percentage) all "raw" KCC2
bandwidth measurements to the mean IPL thickness at each corresponding stage.
The average labeling intensity (within the rectangles) was normalized
(measured with percentage) to the peak value obtained at PH3 (see
Fig. 8 F).

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Figure 8. The neural cotransporter KCC2 is upregulated by a light-controlled
mechanism during turtle retinal development. A, Left panel, Light
micrograph of a vertical section through the central retina at S25. Cells and
processes are revealed with the H&E stain. Horizontal lines demarcate the
outer nuclear (ONL) layer. OPL, Outer plexiform layer; INL, inner nuclear
layer; IPL, inner plexiform layer; GCL, ganglion cell layer. Middle panel,
Fluorescence micrograph revealing the expression of KCC2 in the same retina as
in the left panel. KCC2 is almost entirely restricted to the IPL and OPL,
although there is some weak expression on cell bodies in the INL. The
bandwidth of the labeling is narrower than the IPL itself (left panel). Right
panel, Negative control (no primary antibody, NP). B, Same as
A but for a PH3 retina. The bandwidth of the labeling is virtually
the same as the IPL itself. C, Same as B but for a DR3
retina. The bandwidth of the labeling is narrower than the IPL itself, as in
A. D, Developmental changes in IPL thickness. There is a
large increase from S25 to S26, followed by a small decrease from S26 to PH3.
The IPL is thicker in DR conditions (gray bar) than in matching controls
(PH3). E, Developmental changes in the relative proportion of the IPL
occupied by KCC2. There is a major increase from S25 to S26. DR leads to
weakening of the labeling compared with matching controls (PH3). F,
Developmental changes in KCC2 labeling intensity. The intensity decreases from
S25 to S26, but then peaks at PH3, while it reaches its minimum at DR3.
**p < 0.001; *p < 0.01 (N-K post
test, each column is compared with the preceding one).
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|
Hematoxylin and eosin staining technique. We used this standard
histological technique to measure the IPL thickness. Slides were immersed in
Mayer's hematoxylin for 10-15 min, washed under running water, counterstained
in eosin for 4-5 min, washed again under running water, dehydrated, cleared,
and mounted in Histomount. Sections were viewed under bright-field, and images
captured as for KCC2 immunofluorescence. The IPL thickness was then measured
in Metamorph.
 |
Results
|
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Developmental changes in wave dynamics
We started investigating retinal waves at S22,
3 weeks before hatching
(gestation lasts 8 weeks), when turtle RGCs start firing spontaneous
correlated bursts of action potentials (Sernagor and Grzywacz,
1995
,
1999
;
Grzywacz and Sernagor, 2000
;
Sernagor et al., 2001
,
Sernagor and Mehta, 2001
). All
our optical recordings were made from central retina, where the density of
labeled cells was highest (Fig.
1A). Individual RGCs exhibited strong spontaneous
increases in fluorescence, often in oscillations, presumably reflecting
recurring bursts of spikes (Fig.
1B), as we commonly observe with conventional
electrophysiological techniques (Sernagor and Grzywacz,
1995
,
1999
;
Grzywacz and Sernagor, 2000
;
Sernagor et al., 2001
) (see
also Sernagor et al.,
2000
).
At S22, waves are relatively fast, propagating at 233.6 ± 14.7
µm/sec (mean ± SE) (N = 18, 6; first number, waves; second
number, retinas) and broad, with a mean moment (an estimate of spatial extent)
of 121.7 ± 3.9 µm (N = 18, 6), recruiting 78.3 ±
4.7% of RGCs on their trajectory (N = 18, 6). A propagating wave at
S22 is illustrated in Figure
1C. As in other species
(Sernagor et al., 2001
), waves
in turtle originate at random locations and do not show a preferential
direction of propagation. The spatiotemporal characteristics of the waves do
not change significantly over the next 10 d, between S23 and S24
(Fig. 2A-C) (see movie
1, available at
www.jneurosci.org,
for a wave at S23). The waves remain fast [226.4 ± 14 µm/sec
(N = 36, 10)] and broad, with a mean spatial extent of 123.1 ±
2.2µm(N = 41, 10), recruiting 68.3 ± 3.2% of the cells as
they sweep through the GCL (N = 43, 10).

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Figure 2. Developmental changes in wave dynamics. S22_A-S22_D, Relative
onset plots from four different S22 retinas. S22_D shows two
consecutive waves ( 3 sec apart) propagating in the same direction, as
indicated by the similar slopes. Waves are fast and have a uniform front, as
indicated by a linear increase in delays to onset with distance from the
reference cell. S25_A-S25_D, Relative onset plots from four different
S25 retinas. The plots reveal that waves are much slower and more winding than
at S22. A-C respectively illustrate developmental changes (between
S22 and S25) in wave speed, spatial extent, and cellular recruitment within
waves. All three parameters decrease significantly at S25. Asterisks indicate
statistical significance between that bar and the previous one
(**p < 0.001; N-K post test). Error bars indicate
SEM.
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|
However, by S25, 1 week before hatching, the waves suddenly slow down,
becoming narrow and sinuous (see movie 2, available at
www.jneurosci.org).
To visualize these developmental changes in propagation,
Figure 2 (top and middle rows)
shows the activity onset of cells relative to a reference cell. The top row
shows examples of wave propagation from four different S22 retinas. S22_A to
S22_C illustrate a single wave, and S22_D illustrates two consecutive waves
propagating in the same direction. Propagation patterns in these examples are
remarkably similar, indicating smooth propagation, without much variability.
The middle row shows relative onset plots obtained in four different retinas
at S25. Wave propagation is much slower. S25_A, B, and D exhibit complicated,
"zigzagging" propagation patterns. A summary of the developmental
changes in wave speed, spatial extent, and cellular recruitment is illustrated
in Figure 2A-C,
respectively. All three parameters decrease significantly at S25 (ANOVA,
p < 0.0001). Wave speeds undergo the most dramatic decrease,
dropping by 85.7% (N = 19, 5) [p < 0.001, Newman-Keuls
multiple comparison post-test (N-K test)]. The wave spatial extent and the
cellular recruitment decrease, respectively, more modestly by 19.7%
(N = 22, 5; p < 0.001, N-K test) and by 37% (N =
26, 5; p < 0.001, N-K test).
One week later, when turtles are about to hatch (S26), once again
spontaneous activity patterns change substantially because waves no longer
propagate. Instead, patches of coactive neighboring RGCS were observed, which
sometimes propagated, but over much smaller areas than before
(Fig. 3A). The top row
of Figure 3 illustrates four
examples of relative onset plots at S26. The plots reveal sets of nearly
horizontal lines, each line representing one patch of coactivated RGCs, with
its length reflecting the spread of the patch. Like waves at earlier stages,
the patches occur at random locations, and they are not confined to the same
RGCs, but are rather dynamic. Once turtles have hatched, the spontaneous
patches become smaller and less frequent
(Fig. 3, middle panel).
Figure 3B shows the
steady decrease in cellular recruitment during spontaneous activity from S26
to 3 weeks PH (PH3), the entire period of patchy activity, indicating a
weakening of spontaneous correlated activity in RGCs before it disappears, at
approximately PH4. Cellular recruitment is now arbitrarily calculated over
consecutive 5 sec intervals, because periodic, wave-like, activity has been
replaced by more continuous activity across the population of cells. Cellular
recruitment decreases by 28.7% between S26 (N = 83 intervals, 6) and
PH1 (N = 60, 4) (p < 0.001; N-K test). It then drops once
again by 21.3% between PH2 (N = 75, 4) and PH3 (N = 75, 6)
(p < 0.05, N-K test).

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Figure 3. Waves become localized activity patches at hatching. S26_A-S26_D,
Relative onset plots from four different retinas at S26. The plots reveal
patches of synchronized activity across RGCs. In S26_A, there is
still some propagation because the lines are slightly oblique.
PH3_A-PH3_D, Relative onset plots from four different retinas at 3
weeks PH. Patches are now smaller and recruit fewer cells. A,
Time-lapse images of spontaneous activity in a S26 retina. Conventions are
like Figure 1C. The
activity is now restricted to local patches. B, Decrease in cellular
recruitment during spontaneous activity from S26 onward. Asterisks indicate
statistical significance between that bar and the previous one
(**p < 0.001; *p < 0.05; N-K
post-test). Error bars indicate SEM.
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Acetylcholine, glutamate, and wave dynamics
In our search for the factors responsible for the dramatic changes in wave
dynamics at S25, we first investigated potential developmental changes in the
contribution of acetylcholine and glutamate because both are necessary to
generate spontaneous activity in turtle RGCs from early developmental stages
(Sernagor and Grzywacz, 1999
;
Sernagor et al., 2001
), and
also to propagate retinal waves (Sernagor
et al., 2001
). Moreover, there is a clear developmental switch in
wave control from acetylcholine to glutamate in chick
(Wong et al., 1998
;
Sernagor et al., 2000
) and in
mammals (Bansal et al., 2000
;
Wong and Wong, 2000
;
Zhou and Zhao, 2000
). We
observed the same effects of partial cholinergic and glutamatergic receptor
blockade (with low doses of antagonists, because high doses completely block
SBA) on wave dynamics as previously found in the chick
(Sernagor et al., 2000
)
(Fig. 4). However, unlike in
chick and mammals, both neurotransmitters were required at all embryonic
stages tested (S23 to S25). During partial nicotinic cholinergic receptor
blockade (with mecamylamine 0.5-1 µM), the waves shrank: their
spatial extent and cellular recruitment decreased, respectively, by 45.3%
(N = 33, 4; p < 0.0001, two-tailed t test) and
by 58.8% (N = 32, 4; p < 0.0001, two-tailed t
test), whereas the speed did not change

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Figure 4. Effects of partial cholinergic and glutamatergic blockade on wave dynamics.
Percentage difference from control in cellular recruitment, wave spatial
extent, and speed in the presence of cholinergic nicotinic (black bars) or
glutamatergic (gray bars) antagonists (see Results for more details). Waves
shrink during nicotinic blockade, whereas the main effect of glutamate
blockade is to slow waves down. Asterisks indicate statistical significance
between control and drug (***p < 0.0001;
**p < 0.0067; two-tailed t test). Error bars
indicate SEM.
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|
(N = 25, 4; p = 0.1719). During partial glutamatergic
blockade (with
-GLU-GLY, a broad spectrum antagonist or Chicago Sky
Blue, a glutamate uptake inhibitor, 2-5 µM), the wave speed
decreased by 30.9% (N = 62, 7; p < 0.0067, two-tailed
t test), whereas the spatial extent (N = 62, 7; p =
0.2645) and cellular recruitment (N = 61, 7; p = 0.7091) did
not change.
Developmental changes in GABAA responses
Given the importance of GABAA-mediated activity in other aspects
of developing circuits (Leinekugel et al.,
1999
; Ben-Ari,
2002
), we chose to test its role in generating correlated
spontaneous activity. First we blocked endogenous GABA with the
GABAA antagonist bicuculline (1-10 µM) at various
developmental stages. Between S22 and S24, bicuculline had no noticeable
effect on wave dynamics (nine retinas). At S25, however, when waves suddenly
become slower and more winding, bicuculline became effective at modulating the
waves. At low concentrations (1-5 µM), the drug abolished the
waves (four retinas). At higher concentrations, however, bicuculline did not
block the waves, but on the contrary, it accelerated them
(Fig. 5A). Wave speed
dramatically increased by 886.5% in the presence of 20 µM
bicuculline (N = 16, 2; p < 0.0003, two-tailed t
test), up to 211.5 ± 39.5 µm/sec, similar to wave speed in younger
embryos (see above). In contrast, there was no effect on spatial extent
(N = 16, 2; p < 0.7680, two-tailed t test) and
cellular recruitment (N = 16, 2; p < 0.2969, two-tailed
t test).

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Figure 5. Effects of GABAA receptor blockade on spontaneous activity.
A, Relative onset plots from a S25 retina in control conditions and
in the presence of bicuculline (20 µM). Propagation speed is
10-fold faster in bicuculline. B, Relative onset plots from a
S26 retina in control conditions, 10, and 20 µM bicuculline. The
dose-response effect of bicuculline is remarkable; at 10 µM,
patches become larger and stronger, and when the concentration is doubled,
activity reverts to fast propagation. C, Bicuculline-induced increase
in cellular recruitment during spontaneous activity from S26 to PH3. Black
bars, control; gray bars, bicuculline (2-5 µM)
(**p < 0.001; ***p < 0.0001;
two-tailed t test). Error bars indicate SEM. D, Percentage
increase in cellular recruitment illustrated in C. The significance
of the t test and the number of observations is indicated below each
data point. The enhancing effect of bicuculline increases with development,
suggesting that GABA becomes inhibitory.
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To clarify the intriguing effect of GABA on retinal activity at S25, we
applied single puffs of GABA in the experimental chamber. The purpose of this
was to test whether GABA would produce excitatory or inhibitory responses in
RGCs. Single puffs indeed could induce elevated calcium levels in single
cells. However, much to our surprise, GABA puffs triggered very large waves of
excitation (Fig. 6, movie 3,
available at
www.jneurosci.org).
The dynamics of these "tidal" waves of excitation were completely
different from those of spontaneous waves. They propagated slowly, at 52.3
± 1.8 µm/sec (N = 4, 4), recruiting all RGCs, and they were
long lasting (38.2 ± 5.5 sec) (Fig.
6B), especially when compared with the spontaneous waves
observed at S25 (Fig.
2A,C). Given the great difference in dynamics between
these GABA-induced waves and spontaneously generated waves, we suggest that
different mechanisms are involved in the propagation of these two types of
waves (see Discussion).

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Figure 6. GABA is excitatory at S25. A, Time-lapse images of a GABA-induced
wave in a S25 retina. Conventions are the same as in Figures
1C and
3A. These
"tidal" excitation waves recruit all RGCs, and they are very
prolonged (last frame is taken at 95 sec from the beginning). B,
GABA-evoked waves at S25 and S26. Each trace illustrates the activity averaged
over the entire population of RGCs analyzed. Individual traces were shifted in
time so that all peaks occurred at the same time. Dotted line as in
Figure 1 B. C,
Decrease in GABA-evoked wave duration from S26 onwards.
**p < 0.001, N-K post-test. Error bars indicate
SEM.
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|
As we have reported above, waves stop propagating around hatching, at S26.
Our findings about GABAergic effects at S25 suggest these changes in wave
dynamics at S26 might reflect a change in the nature, or polarity of
GABAA responses, a possibility that was confirmed with bicuculline
at S26 and at post-hatching stages. Figure
5B illustrates a dose-response effect of bicuculline in a
S26 retina that had extremely patchy activity in control conditions. At 10
µM, the drug caused the patches to become much larger, and when
the concentration was doubled, at 20 µM, they reverted to fast
propagating waves (218.7 ± 41.2 µm/sec, calculated over four waves).
At lower concentrations (1-5 µM), bicuculline increased cellular
recruitment in all retinas (Fig.
5C). This enhancing effect increased with development
(Fig. 5D). At the same
time, GABA-evoked waves were already shorter at S26 than at S25 (20.9 ±
3 sec; N = 4, 4) (Fig.
6B,C). They were also harder to evoke PH: they were
elicited in four of five retinas at PH1-2, and only in two of six retinas at
PH3, suggesting that during development, GABAA responses slowly
shift from being excitatory to inhibitory.
Visual experience, GABAA, and spontaneous activity
In all species, RGC-correlated spontaneous activity disappears within the
first postnatal month (Sernagor et al.,
2001
). Although visual experience does not appear to influence the
disappearance of retinal waves in mice
(Demas et al., 2003
), light
deprivation in turtles (which become sensitive to light earlier than mammals)
(Sernagor and Grzywacz, 1995
)
causes spontaneous bursting activity to persist, and consequently, receptive
fields to become much larger than normal
(Sernagor and Grzywacz, 1996
;
Sernagor and Mehta, 2001
).
Calcium imaging confirmed the findings that retinas from dark-reared (DR)
turtles are considerably more spontaneously active than normal
(Fig. 7, top row, compare with
PH3 plots in Fig. 3, second
row; movie 4, available at
www.jneurosci.org).
Both patches (DR4_B, the number indicates weeks of dark-rearing) and
propagation (DR3_B, showing two waves propagating in different directions) are
frequently seen, and cellular recruitment is much higher than normal at that
age (Fig. 7A). Because
our observations from normal development suggest that GABA may be shifting
polarity during that period (see Results, "Developmental changes in
GABAA responses"), perhaps causing the disappearance of
spontaneous activity, we have investigated GABA responses after DR2-4. To our
surprise, we found that GABA retained a substantial excitatory component, even
after 4 weeks of dark-rearing. Indeed, GABA-evoked waves were observed in all
twelve DR2-4 retinas examined, including six retinas from DR4 turtles
(Fig. 7B). These waves
were of similar strength, as indicated by cellular recruitment and duration,
as in younger PH retinas from normally reared animals. Although bicuculline
(1-5 µM) increased cellular recruitment during correlated
spontaneous activity in DR retinas by 49.5% (N = 145, 4; p
< 0.0001, two-tailed t test)
(Fig. 7C), the
increase was much weaker than in the oldest control animals tested (122.2%
increase) (Fig. 7D),
suggesting that as a result of dark-rearing, GABA remained excitatory.

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|
Figure 7. Dark-rearing enhances spontaneous activity and causes GABA to retain an
excitatory component. DR3_A-DR4_B, Relative onset plots from two
retinas at DR3 and two retinas at DR4. Spontaneous activity is strong
(Fig. 3, compare PH3_A to
PH3_D), and sometimes propagates smoothly (DR3_B). A, Cellular
recruitment at PH2, PH3 (black bars), DR2-3, and DR4 (gray bars). Recruitment
is much higher in DR retinas. **p < 0.001 (N-K post
test, PH2 compared with DR2-3 and PH3, with DR4). B, GABA-induced
wave in a DR4 retina (conventions as in
Fig. 6 B). In normal
rearing conditions, GABA is already inhibitory at that age. C,
Bicuculline-induced (2-5 µM) increase in cellular recruitment in
DR2-4 retinas. ***p < 0.0001. Error bars indicate SEM.
D, Percentage increase in cellular recruitment induced by bicuculline
(2-5 µM) from S26 to PH3 and in DR2-4. The progressive
developmental increase in bicuculline efficacy at enhancing spontaneous
activity is much weaker in DR conditions, suggesting that GABA has remained
excitatory.
|
|
Developmental changes in KCC2 expression
Many studies report that the excitatory effect of GABA in the immature
nervous system is caused by elevated intracellular Cl-
concentration ([Cl-]i) because of the late developmental
up-regulation (Payne et al.,
1996
; Rivera et al.,
1999
; Vu et al.,
2000
) of the extruding neural K+/Cl-
cotransporter KCC2 (Williams et al.,
1999
; Delpire,
2000
). Using immunofluorescence, we have looked at the expression
of KCC2 between S25 and PH3 and at DR3
(Fig. 8). KCC2 was expressed in
the IPL and outer plexiform layers (OPL)
(Fig. 8) at all stages, but it
increased with development in the IPL (we did not study the OPL). To ensure
that changes were not simply caused by retinal growth, we normalized our
measurements to the IPL thickness (retinal layers were revealed using the
H&E stain) (Fig.
8A-C). IPL thickness increased by 27% between S25
(N = 93 sampling lines, from three retinas) and S26 (N = 93,
3) (Fig. 8D). The
fraction of the IPL labeled with KCC2 (Fig.
8E) increased from 62.3% at S25 (N = 162, 3) to
93.8% at S26 (N = 126, 3) and 94.3% at PH3 (N = 172, 4)
(Fig. 8A,B) (despite a
small but significant reduction in the IPL thickness between S26 and PH3)
(Fig. 8D), indicating
that KCC2 is indeed upregulated with development. The IPL was thicker at DR3
(21.7 ± 0.5 µm; N = 117, 3) than at PH3 (17.9 ± 0.4
µm; N = 83, 3) (Fig.
8D). This is consistent with our previous observations
that dark-rearing causes RGC dendritic trees
(Sernagor and Mehta, 2001
) and
receptive fields (Sernagor and Grzywacz,
1996
) to grow far beyond normal. Nevertheless, the KCC2 IPL
fraction labeling (Fig.
8E) was significantly lower than in matching controls,
decreasing by 23.5% (N = 126, 3). Interestingly, we found that the
labeling intensity decreased from S25 to S26, but then increased again and
peaked at PH3. These changes are perhaps caused by the initial thickening of
the IPL, causing a "dilution" of the labeling, followed by the
delayed addition of KCC2 molecules to these new processes. The labeling
intensity decreased to its minimum value in DR3 retinas (12.4% decrease;
N = 126, 3) (Fig.
8F).
 |
Discussion
|
|---|
In this study, we have reported on the developmental modulation of retinal
waves in turtle retina. In brief, waves propagate for approximately 2 weeks,
before slowing down and narrowing at S25. Shortly after, the activity weakens
until disappearing at approximately PH4. Spatial extent is controlled by
acetylcholine, whereas glutamatergic connections influence wave speed. Neither
transmitter, however, is responsible for the changes in wave propagation at
S25. Instead, GABA, which is excitatory at S25, controls wave dynamics. As
GABA becomes inhibitory, stationary patches gradually replace waves. Finally,
our dark-rearing studies suggest that light deprivation suppresses the
developmental upregulation of KCC2, causing GABAA responses to
remain excitatory, and hence maintain waves.
Our results suggest that spatiotemporal activity patterns change with
development, and this has potentially important implications for guiding the
establishment of vertebrate visual connections
(Wong et al., 1993
;
Katz and Shatz, 1996
;
Shatz, 1996
;
Crair, 1999
;
Wong, 1999
). By interfering
with specific propagation aspects at different developmental stages, it will
be possible to establish to what extent the information encoded in the waves
refines the formation of visual connections. For example, it will be
interesting to see how reverting patches to propagating waves influences the
size and shape of receptive fields and dendritic arbors in RGCs or their
axonal projections as well as tuning of retinotopy in retinal projections.
Our findings suggest that rather than acetylcholine or glutamate, GABA is
the major neurotransmitter involved in developmental changes of propagation
patterns in turtle. The introduction of excitatory GABAA responses
at S25 causes waves to suddenly slow down and then, as GABA becomes
inhibitory, waves first become stationary patches and then disappear. Although
previous studies in mammals (Bansal et al.,
2000
; Zhou and Zhao,
2000
; Wong and Wong,
2000
) and chick (Wong et al.,
1998
; Sernagor et al.,
2000
) report a switch from acetylcholine to glutamate, none of
them demonstrate that the switch underlies changes in propagation patterns.
Moreover, GABA shifts from excitatory to inhibitory at approximately P15-P18
in ferret (Fischer et al.,
1998
), shortly before waves stop propagating
(Wong et al., 1993
). A recent
study on rabbit has reported similar findings to ours, namely that blockade of
GABAA (and glycinergic) receptors transforms late, weak, and
localized waves to strong propagating ones
(Zhou et al., 2002
). It is
therefore unlikely that the novel role of GABA reported here is unique to
reptiles. Estimates from cat retina suggest that at least 30-40% of amacrine
cells are GABAergic (Vaney,
1990
), and hence many types of amacrine cells may contribute to
the generation and propagation of spontaneous activity. Glycine does not play
a major role in spontaneous burst modulation in turtle RGCs
(Sernagor and Grzywacz, 1999
),
and therefore is unlikely to control wave dynamics.
Early excitatory expression of GABAA
(Leinekugel et al., 1999
;
Ben-Ari, 2002
) and glycine
(Kandler and Friauf, 1995
;
Singer et al., 1998
;
Ehrlich et al., 1999
) is
common in the developing CNS. Our findings suggest a strong correlation
between the developmental shift in GABAA responses and the
upregulation of KCC2 (Vu et al.,
2000
), the neural K+/Cl- cotransporter
responsible for extruding Cl- from the cytoplasm in adult neurons.
Remarkably, visual experience may influence this process. Indeed, we find that
although the IPL thickness increases at S26, presumably because new dendrites
are added, the proportion of IPL dendrites expressing KCC2 also increases.
Growth from S25 to S26-PH3 enhances KCC2 expression mainly in the inner part
of the IPL, near the GCL, whereas dark-rearing has the opposite effect,
suggesting that these changes in KCC2 levels originate from RGC dendrites,
where GABAergic amacrine cells contact RGCs. In support of this idea, KCC2 is
expressed primarily on RGC dendrites (Vu
et al., 2000
). Furthermore, control PH3 (and S25) retinas exhibit
more fluorescent labeling in the inner nuclear layer than DR3 retinas
(Fig. 8, compare B,
C). Ultrastructural studies will help us find the sites where
KCC2 expression changes. All of this supports our physiological observation
that waves stop propagating at approximately S25 to S26 because GABA starts
its inhibitory switch. Our results do not exclude the possibility that there
is a concomitant developmental downregulation of the
Na+-K+-2Cl- cotransporter NKCC1, known to
maintain high [Cl-]i in immature neurons
(Delpire, 2000
).
One could argue that introducing a new excitatory component to the network
at S25 should accelerate and enhance the waves. However, by shunting the
membrane to approximately -40 mV, the presumed Cl- reversal
potential (ECl), GABA cannot evoke spikes, and therefore is not
truly excitatory, although it generates "tidal" calcium waves.
Based on a perfusion rate of 2-5 ml/min (see Materials and Methods), we
estimate that it took GABA 5-15 sec to reach the retina. GABA-evoked waves
took longer to appear, 10-30 sec after the puff. Although we cannot refute the
possibility that these waves simply result from the diffusion of GABA across
the retina, such a delay in wave appearance suggests they are triggered by an
intrinsic induction mechanism. In support, waves did not always propagate in
the direction of the perfusion flow, but sometimes came from the opposite
direction. Occasionally, waves coming from opposite directions even invaded
the imaged region simultaneously. Moreover, GABA puffs at older stages did not
elicit excitation waves. It is conceivable that these GABA-evoked waves
reflect Ca2+ activity rather than spiking, because
voltage-gated Ca2+ channels open with depolarization.
This could explain the fundamentally different dynamics between GABA-evoked
waves and spontaneous waves. Perhaps the prolonged depolarization induced by
GABA and Ca2+ influx causes K+ efflux, which
in turn depolarizes neighboring cells, resulting in these slow but massive and
rather uniform waves of excitation. In support of GABA not being truly
excitatory (in the sense that it cannot generate sustained spiking activity)
although depolarizing at S25, spontaneous wave speed decreases significantly
and waves revert to fast propagation in the presence of high concentrations of
bicuculline. Moreover, waves are much narrower, recruiting fewer RGCs than at
earlier developmental stages. Whether waves, albeit slower and narrower, still
propagate at S25 may depend of the fine balance between the respective
contributions of acetylcholine, glutamate, and GABA to activity generation and
propagation.
The intriguing blockade effect of bicuculline at lower concentrations may
be attributable to the removal of an excitatory component provided by
GABAA responses at this stage. Whether bicuculline produces an
inhibitory or an excitatory effect at S25 perhaps depends on the fine balance
between the overall membrane depolarization and shunting (to approximately -40
mV) caused by GABA. There are, however, other potential explanations to this
bimodal effect of bicuculline at S25. One possibility is that at that S25,
bicuculline acts on separate subclasses of GABAA receptors at low
and high concentrations. For example, extrasynaptic GABAA receptors
might be blocked at lower concentrations than synaptic receptors
(Mody, 2001
). Another
possibility is that [Cl-]in differs among retinal
neuronal types because of differential expression of KCC2 at S25 (but not at
later stages, because later on, activity monotonically increases with drug
concentration) (Fig. 5),
resulting in different effects of GABA on RGCs and amacrine cells
(Vardi et al., 2000
). We
suggest that by gradually shifting to more hyperpolarized levels,
ECl causes the developmental changes in wave dynamics. In support,
activity enhancement by bicuculline increases with development, and
GABA-evoked waves become shorter and ultimately disappear. More detailed
biophysical studies using small, controlled puffs of GABA directly onto
synaptically isolated individual RGCs while recording GABA-evoked currents
will help understanding of these processes.
Light controlling the polarity of GABAA responses is perhaps a
new concept in visual development, but not in circadian physiology, where GABA
is a major player (Cardinali and Golombek,
1998
), and retinal GABA levels are under circadian clock control
(Jaliffa et al., 2001
).
Remarkably, in the suprachiasmatic nucleus, the circadian rhythm generator,
GABAA responses switch polarity between day and night, presumably
because of oscillations in [Cl]in
(De Jeu and Pennartz, 2002
).
Retinal GABA levels increase with light activation
(Roberts, 1995
), and GABA acts
as a self-limiting factor for its polarity switch during development
(Ganguly et al., 2001
).
Therefore, perhaps visual experience increases GABA levels in the retina,
thereby promoting the switch.
However, light cannot entirely account for the shift because the effect of
GABAA receptor activation has already started shifting polarity at
hatching. Perhaps high levels of GABA itself initially trigger the switch
(Ganguly et al., 2001
). In
turtle, GABA-expressing cells are present long before hatching
(Nguyen and Grzywacz, 2000
),
and recent unpublished observations from our laboratory confirm that chronic
GABAA activity is necessary even from before hatching to operate
the switch.
A recent study in the mouse retina found that dark rearing does not prolong
the period during which RGCs exhibit correlated activity
(Demas et al., 2003
). In
control mice, correlated SBA is still present at approximately P15, just after
eye opening, but has disappeared by P21. The developmental loss of correlated
activity was similar for dark-reared mice. Hence, the effects of dark rearing
on correlated activity vary from species to species, possibly because they
have different reliances on vision at birth. Newborn mice are not dependent on
vision, whereas newly hatched turtles must immediately rely on visual cues for
survival (for example marine turtles must run to the sea as soon as they hatch
to escape predators and start their long migratory journey). This suggests
that the onset of visual experience may be of much more importance in turtle
than in mouse retina. Nevertheless, this does not exclude the possibility that
a developmental switch in GABAA activity is as necessary in mammals
as in reptiles to induce the disappearance of correlated SBA. Many more
studies manipulating GABAergic systems and light conditions are required to
reach a fundamental understanding of these fascinating questions.
 |
Footnotes
|
|---|
Received Dec. 27, 2002;
revised Jun. 24, 2003;
accepted Jul. 2, 2003.
This work was funded by the Biotechnology and Biological Sciences Research
Council (E.S.) and the Wellcome Trust (S.J.E.). We thank C. Slater for letting
us use his equipment for analyzing KCC2 immunofluorescence and J. Payne for
his help with selecting the appropriate KCC2 antibodies. We thank J. Demas, C.
Slater, and R. Wong for critical reading of this manuscript.
Correspondence should be addressed to Evelyne Sernagor, School of
Neurology, Neurobiology, and Psychiatry, Medical Sciences, University of
Newcastle upon Tyne, Framlington Place, Newcastle upon Tyne, NE2 4HH, UK.
E-mail:
Evelyne.Sernagor{at}ncl.ac.uk.
Copyright © 2003 Society for Neuroscience
0270-6474/03/237621-
$15.00/0
 |
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