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The Journal of Neuroscience, 1999:RC6:1-5
RAPID COMMUNICATION
Parallel Fibers Synchronize Spontaneous Activity in Cerebellar
Golgi Cells
Bart P.
Vos,
Reinoud
Maex,
Antonia
Volny-Luraghi, and
Erik
De
Schutter
Laboratory for Theoretical Neurobiology, Born-Bunge Foundation,
University of Antwerp, B2610 Antwerp, Belgium
 |
ABSTRACT |
Cerebellar Golgi cells inhibit their afferent interneurons, the
excitatory granule cells. Such a feedback inhibition causes both
inhibitory and excitatory neurons in the circuit to synchronize. Our
modeling work predicts that the long granule cell axons, the parallel
fibers, entrain many Golgi cells and their afferent granule cells in a
single synchronous rhythm. Spontaneous activity of 42 pairs of putative
Golgi cells was recorded in anesthetized rats to test these
predictions. In 25 of 26 pairs of Golgi cells that were positioned
along the transverse axis, and presumed to receive common parallel
fiber input, spontaneous activity showed a high level of coherence
(mean Z score > 6). Conversely, 12 of 16 Golgi
cell pairs positioned along the parasagittal axis (no common parallel
fiber input) were not synchronized; 4 of 16 of them showed only low
levels of synchronicity (mean Z score < 4). For
transverse pairs the accuracy of the coherence, measured as the width
at half-height of the central peak of the cross-correlogram, was rather
low (29.8 ± 12.5 msec) but increased with Golgi cell firing rate,
as predicted by the model. These results suggest that in addition to
their role as gain controllers, cerebellar Golgi cells may control the
timing of granule cell spiking.
Key words:
cerebellum; coherence; computer models; cross-correlation; Crus II; rat
 |
INTRODUCTION |
Golgi
cells play an important role in cerebellar function, because they are
the only element within the circuit that regulates granule cell
activity (Eccles et al., 1964
) (Fig.
1A). Feedback inhibition exerted by Golgi cells may set the activation threshold for
granule cell firing, thus retaining neuronal activity in the granular
layer within operational bounds (Marr, 1969
; Albus, 1971
; Ito, 1984
).
This negative gain control is considered essential because of the
massive excitatory projection to Purkinje cells, which, in rat, receive
~150,000 parallel fiber inputs (Harvey and Napper, 1991
).

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Figure 1.
Effect of firing rate on coherence depends on
orientation of cells. A, Connectivity in the granular
layer. Granule cells (gran, blue) receive
excitation from mossy fibers (MF, orange) and send their
output along their parallel fiber (PF, blue). Golgi
cells (GC, green) receive both MF (orange
triangles) and PF (blue pentagons) excitation
and reciprocally inhibit (green stars) granule
cells. B, Top view of cerebellum demonstrating the two
potential sources of common excitatory input to Golgi cells
(green concentric circles represent dendritic
arbor). Long PFs (thick blue lines) can couple GCs
(thick circles) together for large distances along the
transverse axis, and/or MFs (colored squares; difference
in color denotes different MFs) can directly excite only a few closeby
GCs (filled circles). C, D,
Scattergrams with the mean average firing rate and the width
(milliseconds) of the central peak of the normalized cross-correlogram
(C) or the strength (Z score) of
the correlation (D) plotted for each Golgi cell
pair. Only for cells positioned in the same transverse plane
(blue dots) were significant correlations found.
|
|
The granule cell-Golgi cell circuit has certain properties that make
it unique in the nervous system. Granule cells do not have synaptic
contacts with other granule cells; there are no synaptic connections
within the Golgi cell population either (Ito, 1984
; Voogd and
Glickstein, 1998
). The granule cell-Golgi cell connection thus
constitutes a pure feedback circuit. It is known from other systems
that feedback inhibition causes both inhibitory and excitatory neurons
in the circuit to synchronize (Cobb et al., 1995
; Traub et al., 1996
;
Buzsáki, 1997
). A computer model study (Maex and De Schutter,
1998a
,b
) revealed that the connective properties of the granule
cell-Golgi cell circuit contribute to the emergence of rhythmic
synchronous firing of both cell populations once they are activated by
random mossy fiber input. This synchronization depends on the feedback
inhibition that entrains Golgi cells and granule cells in a common
rhythm, with granule cells firing just before Golgi cells, as well as
on the long parallel fibers (up to 4.7 mm; Pichitpornchai et al., 1994
)
that couple all these oscillators together in a global synchronization.
The classic view of Golgi cell function implies that they control the
amplitude of granule cell activation only (Marr, 1969
; Albus, 1971
;
Ito, 1984
). Our modeling results suggest that Golgi cells also affect
the timing of granule cell spikes. The model predicts that Golgi cells
positioned along the transverse axis fire synchronously as a result of
their common parallel fiber input (Fig. 1B). Golgi
cells positioned along the sagittal axis are not presumed to receive
common parallel fiber input if they are separated by more than the
average size of their dendritic trees (~200 µm;
Dieudonné, 1998b
) and are therefore expected to show
uncorrelated firing. Cells that are very close to each other may also
receive common mossy fiber input (Fig. 1B),
independent of their respective orientation.
To test the model predictions, spontaneous activity of pairs or trios
of Golgi cells was recorded simultaneously in the cerebellar hemisphere
of anesthetized rats (Vos et al., 1999
).
 |
MATERIALS AND METHODS |
Multielectrode extracellular recordings. Recordings
(Vos et al., 1999
) were made in the cerebellar cortex (Crus I and II) of anesthetized (ketamine, 75 mg/kg, i.p.; xylazine, 3.9 mg/kg, i.p.;
hourly supplements, one-third initial dose, i.m.) rats (male, Sprague
Dawley or Wistar, 350-500 gm) with tungsten (2 M
) microelectrodes. Signals were filtered and amplified (bandpass = 400-20,000 Hz; gain = 5000-15,000) using a multichannel neuronal acquisition processor (Plexon Inc., Austin, TX). Spike waveforms were discriminated with a real-time hardware-implemented combined time-voltage window discriminator (Nicolelis and Chapin, 1994
). Up to three separate records of activity at rest (>300 sec each) were concatenated so that
at least 2800 spikes (per unit) were used for further analysis.
Electrolytic lesions (15 µA, 12 sec, cathodal DC current) were made
to mark the location of the electrode tips.
Identification of Golgi cells. Putative Golgi cells were
recognized by the distinctive rhythm of their activity at rest (Atkins et al., 1997
); spikes appeared as pronounced "pops" at a slow cadance with appreciable intervals (no bursting). Golgi cells were
identified using quantitative criteria of others (Eccles et al., 1966
;
Miles et al., 1980
; Edgley and Lidierth, 1987
; Van Kan et al., 1993
;
Atkins et al., 1997
): low discharge rates at rest (interspike intervals
>20 msec), long duration (>0.8 msec) diphasic (negative-positive or
positive-negative) wave shapes, long tuning distances, no complex
spikes, and location in the granular layer. Additional criteria were
used to differentiate other cerebellar units; complex spikes typified
Purkinje cells, and mossy fibers were distinguished by a double peak on
the interspike interval histogram (Vos et al., 1999
). The
small-amplitude, short-duration waveforms that were recorded everywhere
in the granule cell layer, but that could not be isolated to single
units, were presumably granule cell spikes. Categorization of isolated
units as Golgi cells was further confirmed by histological proof that
the electrolytic lesion was in the granule cell layer.
Quantification of coherence of firing. Simultaneously
recorded spike trains of two different units, A and B, represented as binary time series, were cross-correlated to calculate the number of
times (yn) that unit B fired within a time
interval [n
t, (n + 1)
t] from spikes fired by the reference unit A
(yn = counts/bin; bin width,
t = 1 msec;
1000
n < 1000) (Melssen and Epping, 1987
). The cross-correlogram
yn was smoothed four times with a three-point
averaging filter {1/3, 1/3, 1/3}, normalized, and expressed in
standard scores [Z = (yn
E)/sy, with
E = frA frB T
t (frA,B, average
firing rate of A and B; T, recording time), which is the expected value of yn in case of uncorrelated firing
between units (i.e., null hypothesis); and sy = SD
of yn]. Normalization guaranteed cross-correlogram
peak height and width to be independent of T. A Z
score > 3 within [
20
n < 20] was defined as a significant central cross-correlogram peak. Strength of
coherence was determined as the central peak height, i.e., the highest
Z score. Peak width (in milliseconds) was determined at
half-height and was defined between the n values, on either side, marking the first of three successive entries below half-height. Spike train analyses and cross-correlations were performed with STRANGER (Biographics Inc., Austin, TX) and MATLAB (The MathWorks, Inc., Natick, MA).
Statistical analysis. Pearson correlation coefficients were
calculated to test the relation between the average firing rate of a
Golgi cell pair and the strength of the coherence (Z score). A
2 test of independence was performed to determine
whether the frequency of pairs with a significant level of coherent
firing was different between sagittal and transversely oriented pairs.
The relation between distance and peak parameters was determined by
calculating Spearman's rank correlations (
). Differences between
groups for peak parameters were tested using unpaired, two-tailed
t tests.
Ethical considerations. Animals were treated and cared for
according to the ethical standards and the guidelines for the use of
animals in research of the National Research Committee on Pain and
Distress in Laboratory Animals (National Research Council, 1992
).
Testing procedures were approved by the Ethical Committee of the
University of Antwerp, in accordance with federal laws.
 |
RESULTS |
We recorded 42 putative Golgi cell pairs (24 pairs and 6 trios) in
38 ketamine-xylazine-anesthetized rats. Of these, 26 pairs were
positioned along the transverse axis, and 16 were positioned along the
sagittal axis. Synchronization was measured as the height of the
central peak in the normalized cross-correlogram.
Almost all transverse pairs (25 of 26) showed high levels of coherent
firing (Table 1). Distances between these
pairs varied from 300 to 2100 µm, and no significant relationships
between distance and parameters describing the central peak were found (
0.326 < Spearman's
< 0.052; p
0.2227). An example of a transverse trio of Golgi cells is shown in
Figure 2. The coherence between these
cells was highly significant, with Z scores from 7.6 to 8.5. Central peaks were rather broad, with half-height widths of 23-25
msec.

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Figure 2.
Three Golgi cells simultaneously recorded in Crus
IIa and positioned along the transverse axis. A,
Schematic representation of the localization of the recorded units.
Scale bar, 1 mm. B, Superimposed records of 100 waveforms. Calibration, 1 msec. C, Raster plots of
simultaneously recorded spike trains (4 sec sample). D,
Cross-correlograms (1 msec bin) based on 5124 spikes of cell 1, 2862 spikes of cell 2, and 3538 spikes of cell 3, fired at rest (500 sec
recording). The maximum Z scores in each of the
cross-correlograms were, respectively, 8.25, 8.32, and 7.94. The
red line in each graph represents the cross-correlogram
between spikes of one neuron (2, 1, 3) with all spikes that were fired
coherently between the other two (1/3, 3/2, 2/1); the maximal
Z scores were, respectively, 4.28, 3.95, and 4.16.
|
|
The majority of sagittal pairs (12 of 16) did not fire coherently
(distances were between 150 and 1500 µm). An example of a sagittal
trio with flat cross-correlograms is shown in Figure 3. Of the four sagittal pairs that did
show coherent firing, the level of coherence was significantly lower
(Z scores < 4) than the level of coherence found in
transverse pairs (Table 1). Subsequent histological analysis revealed
that in each of these four pairs the distance between the recording
sites was <200 µm.

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Figure 3.
Three Golgi cells simultaneously recorded in Crus
IIa and positioned along the parasagittal axis. See legend of Figure 2
for details and scales. Cross-correlograms were based on 3945 spikes of
cell 1, 3857 spikes of cell 2, and 6531 spikes of cell 3, fired at rest
(500 sec continuous recording). The maximal Z scores at
~0 msec (±20 msec) were, respectively, 2.55, 1.82, and 3.83.
|
|
These findings confirm the prediction generated by our network
simulations, i.e., that Golgi cells that receive common parallel fiber
input are synchronized, whereas others are not, unless they are so
close to each other that they may receive common mossy fiber input. The
results were independent of the type of anesthetic used, because
similar patterns were found for five pairs of Golgi cells recorded in
three
-chloralose-anesthetized rats (results not shown).
In our network simulations (Maex and De Schutter, 1998b
) synchronicity
of firing usually occurs in the context of rhythmic oscillations,
except when Golgi cells fire at very low rates, such as those found in
our recordings (average, 7.7 spikes/sec; median interspike
interval, 100 msec; Vos et al., 1999
). We did observe small side
peaks (Z score < 3.5) in 17 of 26 cross-correlograms of transverse pairs (e.g., Fig. 2D,
center, right). The absence of more obvious
rhythmicity could be related to the Golgi cells not firing at constant
rates (Figs. 2C, 3C), and this would imply that
even at rest mossy fiber input is modulated. Because particularly the
rhythmicity appeared very sensitive to mossy fiber firing rate in the
model (Maex and De Schutter, 1998b
), fluctuating activation levels
could obscure the detection of distinct side peaks in the cross-correlogram (Eggermont and Smith, 1996
). In fact, oscillations at
frequencies corresponding to periods at which most side peaks occurred
in the present study (100-200 msec) have been observed in the granular
layer of awake, behaving rats (Hartmann and Bower, 1998
) and monkeys
(Pellerin and Lamarre, 1997
).
The model also predicted that synchronization is more accurate at
higher Golgi cell firing rates (Maex and De Schutter, 1998b
), such as
those observed in awake animals (Edgley and Lidierth, 1987
; Van Kan et
al., 1993
). In transverse pairs we did find a significant reverse
correlation between average firing rate and the accuracy of coherence
(width of central peak at half height; r =
0.582;
p < 0.005) (Fig. 1C) and a significant
positive correlation between firing rate and coherence strength
(r = 0.497; p < 0.05) (Fig.
1D). No significant correlations were found for the
sagittal pairs (width, r = 0.087; p = 0.7570; strength, r = 0.399; p = 0.1263) (Fig. 1C,D).
Despite the strong correlation between firing rate and accuracy of
coherence in transverse Golgi cell pairs, cross-correlogram peaks were
relatively wide (Table 1). This can be attributed to two factors.
First, the broad peaks could be an epiphenomenon of the lower
spontaneous firing rates found in anesthetized preparations. Second,
the lack of millisecond synchrony may be attributable to the low
efficacy of parallel fiber synapses onto Golgi cells (Dieudonné,
1998b
). The latter implies that many parallel fiber inputs have to
summate to reach spiking threshold. We have recently found that this
causes loose synchronization of Golgi cells in the model (Maex et al.,
1998
). Conversely, the sparser but stronger mossy fiber synapses
(Dieudonné, 1998a
) are expected to synchronize Golgi cells more
tightly; there was a tendency for narrower cross-correlogram peaks for
the four sagittal pairs showing weak correlations (Table 1).
The broad cross-correlogram peaks could also have resulted from
nonsynchronous, phase-delayed activation of Golgi cells, the delay of
which would depend on the location of the excited granule cells
relative to the two Golgi cells. To uncover such nonsynchronous modes
of activation, simultaneously recorded activity of transversely oriented Golgi cell trios was reanalyzed, and cross-correlograms were
generated between spikes of cell A and the spikes of cell B that were
synchronous with those of cell C (time lag, ±1 msec). If the central
peak on these cross-correlograms would be systematically offset from 0 msec, this would imply a successive wave of Golgi cell activation
traveling along the parallel fibers. However, for all transverse trios
(n = 4), cross-correlograms between spikes of one cell
and only the synchronous spikes between the other two had a peak
centered at 0 msec (e.g., Fig. 2D, red lines). This implies that the broad central peaks were not attributable to
nonsynchronous modes of activation. It suggests that the Golgi cell
synchronization occurred as a rather global phenomenon along the
parallel fiber axis, as in the model.
 |
DISCUSSION |
Our results confirmed two predictions of the model (Maex and De
Schutter, 1998b
): 1) Golgi cells that receive common parallel fiber
input fire coherently, whereas activity of Golgi cells that do not
receive common parallel fiber input is less coherent; and 2) the
accuracy of the coherence increases with the level of network activity.
Another model prediction, that granule cell activity along the parallel
fiber axis is also synchronized, could not be investigated
experimentally, because it is impossible to isolate single granule cell
units using extracellular electrodes because of the dense packing of
these very small neurons (Ito, 1984
).
Although our recordings do not prove that the parallel fiber system was
solely responsible for the coherence observed, the low level of
coherence (Z score < 4) found for a few sagittal pairs
puts an upper limit on the possible influence of mossy fibers in the
synchronization process. Moreover, the parallel fibers and the poorly
studied Lugaro axons (Lainé and Axelrad, 1996
) are the only axons
branching along the transverse axis; all other cerebellar afferents and
axons branch completely (climbing fibers and inhibitory axons) or
mostly (mossy fibers) along the sagittal axis (Ito, 1984
; Voogd and
Glickstein, 1998
).
In the model (Maex and De Schutter, 1998b
) synchrony is maintained over
distances many times larger than the length of the parallel fiber. If
common parallel fiber input to Golgi cells were the only cause of
synchronization, synchrony should have decreased linearly to zero over
a distance of ~4 mm (the length of a parallel fiber). We did not find
such a relation between the strength of coherence and the transverse
distance. This could be attributable to the limited sampling of
"long"-distance (>2 mm) pairs. Our recordings of Golgi cell trios
(Fig. 2) suggested however that the coherence was rather global along
the parallel fiber axis. And this implied that, as in the model, not
only the common parallel fiber excitation but also the negative
feedback of Golgi to granule cells contributed to the synchronization. Hartmann and Bower (1998)
also reported widespread synchronous granular
layer activity, even between two cerebellar hemispheres, but they
proposed that the global synchrony in the cerebellum is of
extracerebellar origin. However, a cross-hemispheric synchrony could be
related to parallel fibers that cross the midline (Voogd, 1995
).
Furthermore, if synchronization would be of extracerebellar origin,
Golgi cell pairs along the sagittal axis should have shown the same
high levels of coherent firing.
The granular layer of the cerebellar cortex can be considered as an
input layer, which preprocesses mossy fiber input before transmission
over the parallel fibers to the output neurons, the Purkinje cells. In
classic theories this input layer performs a combinatorial expansion of
the input under gain control by Golgi cells (Marr, 1969
; Albus, 1971
).
Our modeling data and the results reported here suggest that this
circuit performs, in addition, a tight control over the spike timing of
both Golgi and granule cells. Although the central peaks on the
cross-correlograms were relatively broad, we expect more accurate
synchronization in awake animals in view of the reverse correlation
between the average firing rate and the width of the cross-correlogram
peak and under the assumption that firing rates will be higher without
anesthesia. In addition, preliminary modeling and experimental data
suggest that the coherent firing prevails with temporally and spatially modulated mossy fiber input.
In contrast to stimulus-evoked synchronous firing in cortex (Engel et
al., 1997
), which is thought to provide for dynamic binding of neuronal
ensembles, the spontaneous synchronization of cerebellar Golgi cells
may be instrumental to the transformation of spatial patterns encoded
in mossy fiber input into temporal patterns on the parallel fiber
system. Because of the patchy, fractured somatotopy of mossy fiber
input to the granular layer (Bower and Kassel, 1990
; Welker, 1987
),
this input shows complex spatial patterning. By synchronization of
granule cell firing the spatial information encoded in mossy fiber
activation patterns can be transformed into a temporal code (Hopfield,
1995
). The Purkinje cells will thus receive a temporal spike pattern in
which the relative position of coactivated patches is coded by the
phase difference between the activity transmitted along parallel fibers originating from these different patches. These phase differences will
change depending on the location along the transverse axis of the folium.
Recent optical imaging data by Cohen and Yarom (1998)
suggest that the
effect of parallel fiber synapses onto Purkinje cells is weak compared
with that of synapses from the ascending part of the granule cell axon,
because no beams of activation along the parallel fiber axis (Eccles et
al., 1967
) were found. Our study suggests that, in fact, such beam-like
effects may instead exist at the level of synchronously activated Golgi
cells. The parallel fiber spike patterns are not expected to directly
activate the Purkinje cell: a coincidence detection such as the one
proposed by Braitenberg et al. (1997)
would not be very robust,
considering the results of Cohen and Yarom (1998)
. As proposed in our
modeling studies of Purkinje cells (De Schutter, 1995
, 1998
), the
temporal spike patterns on the parallel fibers are thought to cause
reproducible changes in the excitability of its active dendrite (Jaeger
et al., 1997
) and thus to affect the firing probability during
subsequent input.
In conclusion, we propose that Golgi cells control the timing of
granule cell spiking. The proposed role of the granular layer as a
temporal encoder fits well with the general importance of timing in
cerebellar function (Welsh et al., 1995
; Raymond et al., 1996
; Ivry,
1997
; Thach, 1998
).
 |
FOOTNOTES |
Received Dec. 9, 1998; revised Feb. 19, 1999; accepted March 4, 1999.
This research was funded by European Community contract BIO4-CT98-0182,
by Interuniversitaire Attractie Pool Belgium Grant P4/22, and by Fund
for Scientific Research-Flanders (FWO-Vl) Grant 1.5.504.98. B.P.V. and E.D.S. are supported by the FWO-Vl. We thank Inge Bats for
the photography and Evelyne De Leenheir and Ursula Lubke for the
histology. We gratefully acknowledge the technical wizardry of Mike
Wijnants. We also thank the reviewers for their comments on an earlier
version of this manuscript.
Correspondence should be addressed to Dr. Bart P. Vos, Born-Bunge
Foundation, University of Antwerp, Universitaire Instelling Antwerpen, Universiteitsplein 1, B2610 Antwerp, Belgium.
 |
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