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Theoretical Neurobiology, University of Antwerp, Antwerp, Belgium
Submitted 30 May 2006; accepted in final form 13 September 2006
| ABSTRACT |
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| INTRODUCTION |
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The inhibitory PCs are not final projecting neurons of the cerebellum but target the real output neurons in the deep cerebellar nuclei (DCN). In vitro dynamic voltage-clamp experiments showed that
10% synchronization among PCs converging onto a DCN neuron increases the reliability of the neuronal spiking four times more than 1% synchronization (Gauck and Jaeger 2000
). Furthermore, DCN spikes can be precisely controlled by synaptic input at the millisecond level, and such spikes mostly followed short decreases in inhibition lasting
15 ms (Gauck and Jaeger 2000
). However, it is not known whether such short pauses in PC SS trains are synchronized in vivo. Pauses in SS trains can be generated by multiple mechanisms. It has been reported that CSs are always followed by a pause of variable duration: from several tens of milliseconds (Bloedel and Roberts 1971
; Granit and Phillips 1956
) to several hundreds of milliseconds (Bell and Grimm 1969
; Burg and Rubia 1972
; Latham and Paul 1971
; McDevitt et al. 1982
; Murphy and Sabah 1970
, 1971
; Thach 1967
). The CS triggered pauses can be followed by increased, decreased, or unchanged SS firing rates (McDevitt et al. 1982
; Sato et al. 1992
). On the other hand, pauses can also be generated by intrinsic afterhyperpolarization, decreased PF input, and/or increased on beam or lateral inhibition from interneurons (Cohen and Yarom 2000
). Nevertheless, the origin of all these pauses would be indistinguishable in spike trains recorded from PC axons contacting DCN neurons (Monsivais et al. 2005
). Hence we have defined pauses in this study as all SS ISIs that are indistinguishable in duration from the pauses after CSs, as the latter are uniquely defined. Applying this criterion, we have investigated the synchronization of SS pauses by analyzing the cross-correlations of nearby synchronous pairs of PCs.
| METHODS |
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Forty five male Sprague-Dawley rats (300400 g, Iffa Credo, Brussels) were anesthetized with a mixture of ketamine HCl (75 mg/kg; Ketalar, Parke-Davis, Warner Lambert Manufacturing, Dublin), and xylazine HCl (3.9 mg/kg; Rompun, Bayer, Leverkusen, Germany) in normal saline (0.9% NaCl, Baxter, Lessine, Belgium) by intraperitoneal injection. A craniotomy exposing Crus II of left cerebellar hemisphere was performed (Vos et al. 1999b
). Supplemental doses of the anesthetic (one third initial dose) were given intramuscularly to maintain deep anesthesia as evidenced by the lack of a pinch withdrawal reflex and/or lack of whisking.
A new protocol was developed to record from 38 nearby PCs. One electrode was inserted perpendicularly to the cerebellar surface. The second electrode was tilted 58° from a horizontal plane to reduce dimpling and inserted at a distance from the first electrode so that their tips converged at the Purkinje cell layer. As control, we also recorded 12 distant pairs that were recorded from two electrodes separated by
400 µm. In all cases, the two electrodes were positioned along the transverse direction relative to each other. Here we describe data from eight selected pairs of nearby PCs (see RESULTS) and control analysis based on 39 single-unit recordings of PCs. After recording spontaneous activity in four synchronous pairs, tactile stimulus-evoked responses were recorded. Perioral receptive fields were explored as reported elsewhere (Vos et al. 1999b
). A punctate stimulus was applied at 0.5 Hz. Electric lesions (15 µA, 8 s, cathodal DC current) were made to mark the location of the electrodes at the end of five paired recordings of nearby PCs. The distance between pairs was estimated from the distance between the centers of the lesion sites. Rats received a lethal dose of sodium pentobarbital (120 mg/kg ip; Nembutal, SANTOFI, Libourne, France) at the end of the experiment. The brain was removed and fixed in 4% paraformadehyde. The cerebellum was embedded in paraffin, and 10-µm coronal sections were cut and stained with cresylviolet to visualize the electrolytic lesions. All experimental methods were approved by the ethical commission of the University of Antwerp and conformed to the guidelines of the European Commission.
Data analysis
After recordings of CSs and SSs, they were separated with off-line spike sorting software (Plexon, Austin, TX). Examples of the waveforms of sorted SSs and CSs from one PC are shown in Fig. 1A, inset. The off-line analysis of PC firing patterns was carried out using Matlab (The Mathworks, Natick, MA) and Microsoft Excel (Microsoft, Redmond, WA). The mean firing rates of SSs and CSs were 41.8 ± 3.6 and 0.73 ± 0.05 (SE) Hz, respectively, and they were not correlated (R2 = 0.003). SS trains were constructed by removing all CS spikes from all recordings; any spike occurring within 10 ms of the start of a CS was considered to be part of the CS response as they probably belonged to the CS burst (Monsivais et al. 2005
).
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3 were considered as synchronized pairs. The broadness of synchronization was measured with the full width at half-height (half-width). To assess the effect of firing rate co-modulation, shuffled spike trains were generated by randomly shuffling the ISIs within blocks of five consecutive ISIs. All P values refer to Students paired or unpaired t-test, unless otherwise specified.
Pauses were defined by setting a threshold for ISI duration, any ISI equal or larger than the threshold was considered a pause. A threshold was chosen based on previous reports that CSs are followed by pauses. The distribution of the first SS ISIs preceding CSs was compared with that of pauses after CSs, where the SS ISIs and pauses after CSs were pooled from 39 PC SS trains (Fig. 1A). The median, 10 percentile and 90 percentile of SS ISIs (pauses after CSs) were 10.0 ms (CS: 31.0 ms), 5.9 ms (CS: 17.9 ms), and 29.9 ms (CS: 617.5 ms) respectively. We then selected a threshold that would optimally detect the pauses after CSs if the two distributions were mixed as is the case in the PC axon because CS bursts are not transmitted faithfully (Monsivais et al. 2005
). This was achieved by computing the proportion of ISIs categorized as pauses for different thresholds (set at 10, 11, 12,..., 20, 30, 50, 100, 200, or 1,000 ms) for all first SS ISIs preceding CSs and for all pauses after a CS (Fig. 1B, inset). The value that maximized the difference between these two proportions was considered as the optimal threshold, 16 ms (Fig. 1B). The smallest threshold which was not significantly different from the optimal, 12 ms, was used as threshold in this study. This threshold included more pauses caused by CSs, resulting in correct detection of 99.3 ± 0.2% of the pauses after CS (compared with 95.4 ± 1.2% for a 16-ms threshold).
Using this definition of pauses, spikes were classified as either pause times (Pt, spikes beginning or ending a pause) or nonpause times (Nt, the rest of the spikes; Fig. 2A). The sensitivity of Z score and HW to the pause threshold was tested by computing these values for different thresholds. Measurements from each threshold were compared with those measured in overall spikes with the Wilcoxon signed-rank test. To avoid bias caused by small sample sizes, we excluded all recordings with a sample size <200. The sample sizes of Pt and Nt at different thresholds are summarized in supplemental Table 1.1
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| RESULTS |
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3) (Vos et al. 1999a
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Using the definition of pauses, spikes were classified as either pause times (Pt) or nonpause times (Nt; METHODS and Fig. 2A). On average, 73.2 ± 4.1% of spikes were classified as Pt (Fig. 2C). This classification was used to recompute the cross-correlogram for either all Pt (Fig. 3, B and C, red) or all Nt (green), taken from both cells of the pairs. The sharp peak of the cross-correlogram consisted exclusively of Pt (sample size: 8763 ± 714, Z score 8.1 ± 1.3, range: 3.915.9; half-width 4.0 ± 0.7 ms, range: 28 ms), whereas the Nt caused the broad peak (sample size: 3,859 ± 840, Z score 5.3 ± 0.6, range: 3.17.2; half-width 60.3 ± 10.0 ms, range: 36110 ms). These observations were robust for the threshold selected (Fig. 3C). For thresholds between 12 and 18 ms, Pt had narrower half-widths and higher Z score than Nt did (P < 0.03, Wilcoxon signed-rank test). Conversely, smaller thresholds gradually destroyed the difference in precision between Pt and Nt (Fig. 3C). The higher synchronization of Pt was not caused by the different sample size as it persisted when the sample sizes for both Pt and Nt were equivalent (threshold of 16 ms, supplemental Table 1).
These results indicate that mainly the spikes around pauses were precisely synchronized. Conversely, two facts suggest that the broad peak consisting of Nt spikes was caused by firing rate co-modulation, a mechanism that causes spurious synchronization between two neurons which have firing rates that co-vary in time (Eggermont and Smith 1995
; Maex et al. 2000
). First, in properly shuffled spike trains the broad peak was conserved for Nt but not for Pt (Fig. 3B, left inset). Second, precision of synchronization correlated with firing rate as Nt occurring in the central 2-ms window of the broad peak (18.3 ± 3.3% of all nonpause ISIs) corresponded to ISIs that were significantly shorter than overall Nt (Fig. 5).
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Our analysis thus suggests that Pt or Nt of one PC tended to be correlated with corresponding spikes of the other PC. Pt can be related to a pause in three ways: they can start a pause (sPt), end it (ePt), or be interspersed between two consecutive pauses (iPt). We checked whether any of these categories of Pt was preferentially synchronized by correlating only sPt, ePt, or iPt of one PC with the corresponding spikes of the other PC. These specific correlations did not show significant differences compared with each other (Fig. 6, P > 0.4, Wilcoxon signed-rank test), indicating that the accurately synchronized spikes did not have a preferential timing relative to the pause. Next, we investigated whether pauses after CSs were responsible for the synchronization observed. The correlation of SS trains where the first SS after a CS was removed for all CSs in one of the SS trains (n = 4, mean CS firing rate = 0.9 ± 0.1) did not show any significant changes in the peak Z score (9.4 ± 1.4) or half-width (30.0 ± 18.7) of the central peak (P > 0.6, Wilcoxon paired rank test), suggesting that the precise synchronization of Pt was not caused by CSs.
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The analysis presented in Figs. 3, 4C, and 6 was based on cross-correlation of specific categories of spikes. This does not guarantee that pauses were highly synchronized because a spike at the start of a pause in one PC can be synchronous with a spike at the end of a pause in the other PC. Therefore in a final analysis, we selected all Pt synchronous within ±2 ms and checked whether the corresponding pauses where also synchronized. The pauses starting together (S-sP) represented 4.0% of overall pauses. Similar proportions were found for pauses ending together (S-eP, 3.6%) or followed by another pause (S-iP, 5.4%; Fig. 7A). If this synchrony was caused by chance, these proportions would be similar to the values obtained from randomly shuffled spike trains. However, all cases were significantly more synchronous than chance level (P < 0.002, Wilcoxon signed-rank test). Interestingly, the synchronous pauses (SM-P, the sum of S-sP, S-eP, and S-iP) had a significantly longer duration (median: 19.9 ± 0.6 ms) than the averaged duration of all pauses (Fig. 7B, P < 0.03, Wilcoxon signed-rank test). But, the durations of SM-P were not correlated in paired PCs (correlation coefficient = 0.14 ± 0.04).
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Taken together, in this study, we have shown that around half of SS intervals are pauses defined as ISIs of
12 ms; in transverse pairs of PCs separated by <100 µm,
35% of spikes are precisely synchronized and
13% of the pauses occur synchronously, either starting or ending precisely together; CSs do not cause the precise synchronization of pauses; and coincident pauses are longer than other pauses, but their durations are not correlated.
| DISCUSSION |
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13% of all pauses are synchronized in nearby PC pairs in vivo. Synchronized pauses had a median ISI of
20 ms which is longer than the minimum duration of 15 ms reported by Gauck et al. (2000) to reliably evoke a DCN spike, it is also similar to the duration of the IPSC recorded in DCN neurons in vitro (Pedroarena and Schwarz 2003
If we assume that the recorded PC pairs are random samples of the
1,000 PCs converging onto a DCN neuron in rats (Chan-Palay 1977
), we expect that statistically a similar percentage of spikes and pauses will be synchronized among PCs converging on a DCN. The DCN spikes generated during the decrease of inhibition caused by synchronous pauses are most probably postinhibitory rebound spikes (Llinas and Muhlethaler 1988
). Other in vitro experiments have shown that DCN neurons generate pronounced postinhibitory rebound spikes with a delay of
30 ms to the onset of the last inhibitory postsynaptic potential (IPSP) (Aizenman and Linden 1999
). Such rebound spikes, which rely on the strength and duration of preceding hyperpolarization (Aizenman and Linden 1999
), are a good candidate cerebellar timing signal (Kistler and De Zeeuw 2002
; Koekkoek et al. 2005
).
What causes the precise synchronization of pauses in nearby pairs of PCs receiving common PF input remains unclear, but we could exclude an important contribution of CSs. It has recently been suggested that CFs may evoke transitions between up and down states in PCs in vivo (Loewenstein et al. 2005
; but see also Schonewille et al. 2006
). It is unlikely that the synchronized pauses we observed correspond to quiescent down states because the latter last on average several seconds (Loewenstein et al. 2005
). Moreover we did not find any evidence for a causal relationship between CF occurrence and transitions between high and low firing rate regimes (S. L. Shin, F. E. Hoebeek, M. Schonewille, A. Aertsen, and E. De Schutter, unpublished data). Indirect effects of CFs on molecular layer interneurons or of mossy fiber branching are also unlikely as these are expected to affect PC synchronization over much longer distances (Shinoda et al. 2000
; Welsh et al. 1995
; Woolston et al. 1981
) than observed here.
A more likely mechanism for the pauses is synchronized IPSPs caused by feed-forward inhibition, which is an important regulator of the timing of the neuronal responses of cerebellar PCs and molecular layer interneurons (MLIs) (Cohen and Yarom 1998
; Eccles et al. 1967
; Mittmann et al. 2005
; Solinas et al. 2006
). The role of common feed-forward inhibition in the precise synchronization is supported by the facts that the sharp synchrony has been observed only in very close pairs (Jaeger 2003
) and that interneurons have short axonal collaterals (Palay and Chan-Palay 1974
; Solinas et al. 2003
; Sultan and Bower 1998
). However, feed-forward inhibition is more likely responsible for the synchronization of pauses, not for the synchronous spikes that may have been generated by parallel fiber inputs. As not all excitatory PF inputs trigger feed-forward inhibition (Mittmann et al. 2005
), carefully designed follow-up studies will be required to understand their exact contribution to the observed synchrony. Another possible cause of the synchronous pauses is intrinsic afterhyperpolarization, which may be modified by learning processes (V. Steuber, W. Mittmann, M. Häusser, and E. De Schutter, unpublished results). An intrinsic origin of pauses could explain the large variation between PCs (Fig. 2B, bottom) as PCs show a large variability in the expression of voltage gated channels (Achard and De Schutter 2006
; Swensen and Bean 2005
). Although CSs were not directly responsible for the synchronous pauses, this does not exclude that previous learning processes induced by CSs modified dendritic excitability (Schreurs et al. 1998
).
Not only precisely synchronized Pt but also the loosely synchronized Nt may be important for controlling DCN neurons. The latter may regulate DCN baseline firing rates (S. L. Shin, F. E. Hoebeek, M. Schonewille, A. Aertsen, and E. De Schutter, unpublished data), which are linearly correlated to the input frequencies of converging PCs (Gauck and Jaeger 2000
). In this study we have shown that fast firing spikes tend to be only loosely synchronized. This will raise the actual firing rate of the converged high-frequency input, resulting in more efficient suppression of the DCN neurons.
Our estimate of 35 and 13% of synchronization of simple spikes and pauses, respectively, were made during spontaneous activity under anesthesia. Although it was recently reported that there was no difference in the occurrence of pauses of 50 ms or longer between anesthetized and awake mice (Schonewille et al. 2006
), we do not know whether this also applies to synchrony of pauses. We did not find a strong effect of tactile stimulation, but this may have been due to the lack of a behavioral context in the anesthetized preparation (Krupa et al. 2004
). Indeed, similar spike correlations with different degrees of temporal precision were observed in motor cortex of behaving monkeys (Riehle et al. 1997
). In the motor cortex, precise synchronization without rate modulation was observed during internal (expectation) events. To understand the functional significance of dynamic synchronization in cerebellar PCs experiments in awake, behaving animals will be needed, but under these conditions, recording from nearby PCs on different electrodes will be a technical challenge. Nevertheless, at this time we can propose that the dynamic synchronization of PC SSs may be important for fine control of the target neurons in DCN neurons and that, especially, the precisely synchronized pauses may serve to control the timely generation of rebound spikes in DCN neurons.
| GRANTS |
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| ACKNOWLEDGMENTS |
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| FOOTNOTES |
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1 The online version of this article contains supplemental material. ![]()
Address for reprint requests and other correspondence: E. De Schutter, Theoretical Neurobiology University of Antwerp, Universiteitsplein 1, B2610, Antwerp, Belgium (E-mail: erik{at}tnb.ua.ac.be)
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