Abstract
At presynaptic active zones, neurotransmitter release is initiated by the opening of voltage-gated Ca2+ channels close to docked vesicles. The mechanisms that enrich Ca2+ channels at active zones are, however, largely unknown, possibly because of the limited presynaptic accessibility of most synapses. Here, we have established a Cre-lox based conditional knock-out approach at a presynaptically accessible CNS synapse, the calyx of Held, to directly study the functions of RIM proteins. Removal of all RIM1/2 isoforms strongly reduced the presynaptic Ca2+ channel density, revealing a new role of RIM proteins in Ca2+ channel targeting. Removal of RIMs also reduced the readily-releasable pool, paralleled by a similar reduction of the number of docked vesicles, and the Ca2+ channel - vesicle coupling was decreased. Thus, RIM proteins co-ordinately regulate key functions for fast transmitter release: enabling a high presynaptic Ca2+ channel density, and vesicle docking at the active zone.
Keywords: transmitter release, presynaptic cytomatrix, synaptic transmission, readily-releasable pool, Ca2+ secretion-coupling
Introduction
Action potentials (APs) evoke neurotransmitter release from presynaptic nerve terminals in the process of SNARE-protein - mediated vesicle fusion (Chen and Scheller, 2001; Jahn et al., 2003). Transmitter release is triggered by Ca2+ influx through voltage-gated Ca2+ channels, and the fast phase of release closely follows the waveform of presynaptic Ca2+ current with only a sub-millisecond delay (Sabatini and Regehr, 1996; Borst and Sakmann, 1996). One pre-requisite for the temporal precision of transmitter release is a tight spatial co-localization between docked vesicles and Ca2+ channels in the range of a few 10's of nanometers, which enables a short diffusional distance between Ca2+ channels and the Ca2+ sensor for vesicle fusion (see Neher, 1998 for a review). Thus, there is general agreement that Ca2+ channels must be enriched within the active zone, as is also suggested from fast Ca2+ imaging studies (Llinás et al., 1995; Zenisek et al., 2003) and from initial ultrastructural evidence at CNS synapses (Bucurenciu et al., 2008). However, the molecular mechanisms which enable an enrichment of Ca2+ channels at the presynaptic active zone are not well understood.
The presynaptic active zone of synapses consists of a dense accumulation of cytomatrix proteins, some of which, like Munc13, ELKS/CAST and RIM's are localized highly specifically at active zones (Schoch and Gundelfinger, 2006). Amongst these, RIM proteins (Rab3-interacting molecule; Wang et al., 1997) are interesting candidates for scaffolding proteins with possible interactions with voltage-gated Ca2+ channels (Coppola et al., 2001; Hibino et al., 2002; Kiyonaka et al., 2007). RIM proteins are encoded by four genes (Rims1-4) which drive the expression of seven known RIM isoforms: RIM1α, 1β; RIM2α, 2β, 2γ; as well as RIM3γ and RIM4γ (Wang et al., 2000; Wang and Südhof, 2003; Kaeser et al., 2008). RIM proteins bind to multiple other presynaptic proteins – e.g., Rab3, Munc13's, α-liprins, and RIM-binding proteins (RIM-BPs; Wang et al., 1997; Wang et al., 2000; Betz et al., 2001; Schoch et al., 2002; Dulubova et al., 2005). Genetic removal of RIM1α in mice, and of the homologous unc10 protein in c.elegans has indicated a role of RIMs in transmitter release (Koushika et al., 2001; Schoch et al., 2002; Calakos et al., 2004), as well as in presynaptic forms of long-term plasticity in a synapse-specific way (Castillo et al., 2002). Recent studies proposed multiple potential interactions between RIMs and Ca2+ channels. RIM C2-domains were found to bind to L- and P/Q-type Ca2+channels (Coppola et al., 2001). Heterologous expression of RIM1α in non-neuronal cells reduced the inactivation of co-expressed voltage-gated Ca2+ channels via an interaction of the RIM1 C-terminus with Ca2+ channel β4-subunits (Kiyonaka et al., 2007). RIM-BPs have been found to bind to L- and N-type Ca2+-channel α subunits (Hibino et al., 2002). However, the role of RIM proteins for Ca2+ entry at the presynaptic nerve terminal has remained unclear, maybe because no previous study eliminated all RIM1/2 isoforms in vertebrates, and because genetically accessible model synapses, like the neuromuscular junctions of C. elegans and drosophila and cultured CNS neurons, are not accessible to direct presynaptic recordings.
The calyx of Held in the auditory brainstem is a large synapse accessible to patch-clamp recordings directly at the nerve terminal, which has enabled a uniquely direct control of presynaptic Ca2+ for studying the Ca2+ regulation of transmitter release (see Schneggenburger and Forsythe, 2006, for a review). However, the usefulness of the calyx preparation has been limited by the fact that many conventional mouse knock-out (KO) models cause perinatal lethality. To overcome this limitation and to allow for a direct study of the presynaptic roles of RIM proteins, we have devised a Cre-lox based conditional KO approach at the calyx of Held synapse, using newly generated RIM1/2 floxed mouse lines (Kaeser et al., submitted). We show that the conditional removal of RIM proteins leads to a strong decrease of Ca2+ currents in the nerve terminal, providing direct evidence that RIMs enrich Ca2+ channels at the presynaptic active zone. RIM1/2 removal also led to a marked reduction in the number of readily-releasable vesicles, which was paralleled by a similar reduction in the number of docked vesicles. Moreover, RIM proteins help to speed the rates of transmitter release both intrinsically and by increasing the coupling of readily-releasable vesicles with Ca2+ channels. Thus, RIM proteins coordinate essential functions that ensure fast rates of transmitter release at synapses.
Results
Conditional knock-out of RIM1/2 at the calyx of Held synapse
We wished to investigate the presynaptic function of RIM proteins at the calyx of Held, a large CNS model synapse at which direct measurement of presynaptic Ca2+ currents can be made (see Introduction). However, constitutive RIM1α/RIM2α double KO mice die at birth (Schoch et al., 2006) which precludes their analysis at the calyx of Held, and deleting individual RIM isoforms might produce only a weak phenotype because of the functional redundancy among the isoforms (Schoch et al., 2006; Kaeser et al., 2008). We therefore aimed to remove RIM1/2 conditionally at the calyx of Held, using newly produced floxed mouse lines in which the expression of all RIM1 and RIM2 isoforms, including RIM1β and RIM2β, can be abolished by expression of Cre-recombinase (Kaeser et al., submitted). For this purpose, we searched for a Cre-driver mouse line that expresses Cre-recombinase specifically in the lower auditory brainstem where calyces of Held are located. We found that in Krox20+/Cre mice (Voiculescu et al., 2000), Cre-activity as revealed by a tandem-dimer red fluorescence protein (tdRFP) reporter mouse line (Luche et al., 2007) was present in the lower auditory brainstem as well as in the trigeminal nucleus and some adjacent areas, but importantly, most other areas of the brainstem and CNS were devoid of Cre activity (Fig. S1A). In the ventral cochlear nucleus, which harbors globular bushy cells that generate calyces of Held (see Cant and Benson, 2003, and references therein), a large number of tdRFP-positive neurons were found (Fig. S1B, Fig. 1A). In the MNTB, the target nucleus of calyces of Held, tdRFP was present in postsynaptic neurons, as well as in calyces of Held, which were identified by co-staining with an anti Synaptotagmin2 (Syt2) antibody (Fig. 1B). Thus, Cre activity in Krox20+/Cre mice is present in a neuron population that includes calyx of Held-generating neurons in the cochlear nucleus, which explains the presence of tdRFP-positive large nerve endings in the MNTB.
We crossed the Krox20Cre/+ mice with floxed RIM1/2 mice (Kaeser et al, submitted) to generate conditional RIM1/2 double KO mice specific for the auditory brainstem. Due to germline recombination in the Krox20Cre line (Voiculescu et al., 2000), we obtained Cre-positive RIM1/2 lox/Δ mice (see Experimental Procedures). These mice were viable and fertile, which allowed us to investigate synaptic transmission in brain slice preparations. We will refer to synapses recorded in Cre-positive RIM1/2 lox/Δ mice as RIM1/2 cDKO synapses (for "conditional double KO"). As a control group, we used Cre-negative, RIM1/2 lox/Δ littermate mice (see Experimental Procedures). EPSCs evoked by afferent fiber stimulation at calyx of Held synapses in RIM1/2 cDKO mice had amplitudes of only 1.86 ± 1.73 nA (n = 12 cells), significantly smaller than in Cre-negative littermate control mice (9.8 ± 4.2 nA; n = 15 cells; Fig. 1C, D). The evoked EPSCs also had slightly, but significantly slower rise times (Fig. 1E, F; p = 0.0038), reflecting slowed release kinetics which will be analyzed in more detail below (see Figs 4; 5). The amplitude of spontaneous, 'miniature' EPSCs (mEPSCs) was unchanged (Fig. 1G), consistent with a presynaptic transmitter release deficit. Synaptic phenotypes were consistently observed in all synapses studied in RIM1/2 cDKO mice (n=73). This indicates that Cre-mediated removal of the RIM proteins was effective, without detectable inhomogeneity across the population of the studied neurons.
RIMs determine presynaptic Ca2+ channel density
Having established the conditional removal of all long RIM isoforms at the calyx of Held, we are now in a position to directly study the presynaptic function of RIM1/2 proteins. In current clamp recordings from calyces of Held, presynaptic APs elicited by afferent fiber stimulation were unchanged in RIM1/2 cDKO calyces (Fig. 2), showing that changes in the AP-waveform do not underlie the reduced transmitter release. We next investigated presynaptic Ca2+ currents in voltage-clamp recordings of the calyx of Held. Surprisingly, these recordings revealed a strong reduction of the amplitude of Ca2+ currents in RIM1/2 cDKO calyces (Fig. 2C). In both genotypes, presynaptic Ca2+ currents started to activate at around −20 mV, and the maximal Ca2+ current was observed at ~ 0 mV (Fig. 2C, D); however, the maximal Ca2+ current was only 500 ± 310 pA (n = 19 cells) in RIM1/2 cDKO calyces, whereas it was 1040 ± 250 pA (n = 9) in calyces of control mice (Fig. 2E; p < 0.001). Control experiments with Krox20+/Cre mice, and with RIM1lox/RIM2lox mice revealed no significant reduction of the presynaptic Ca2+ current (Fig. S2), showing that the reduced Ca2+ currents were not caused by the Krox20+/Cre allele, nor by the non-recombined, floxed RIM1/2 alleles. In order to normalize the measured Ca2+ current amplitudes for the membrane surface of calyx terminals, we recorded the membrane capacitance Cm of calyces of Held, which was unchanged (12.7 ± 4.0 pF, n = 19, and 14.8 ± 3.5 pF, n = 9 in RIM1/2 cDKO and control calyces, respectively; p = 0.16). The maximal Ca2+ current normalized for membrane surface (peak ICa / Cm), was significantly smaller in RIM1/2 cDKO calyces as compared to control mice (Fig. 2F, p < 0.001).
Since RIM1α expression was shown to reduce voltage-dependent inactivation of Ca2+ channels in BHK cells (Kiyonaka et al., 2007), we next tested whether the reduced Ca2+ current amplitude might result from an increased steady-state inactivation at the standardly employed holding potential of −70 mV. Conditioning pre-pulses of 2 s duration to more hyperpolarized membrane potentials (−90 mV, −110 mV; Fig. 2G, H) did not significantly increase the Ca2+ current during a subsequent step to 0 mV, arguing against significant steady-state inactivation at the holding potential. Therefore, the reduced Ca2+ current amplitude most likely reflects a reduced number of Ca2+ channels in the calyx of Held nerve terminals. With conditioning pre-pulses to more positive membrane potentials (−50 and −30 mV), we found a somewhat stronger steady-state inactivation in RIM1/2 cDKO calyces as compared to control (Fig. 2H; p < 0.01), consistent with previous work in cultured non-neuronal cells (Kiyonaka et al., 2007). Overall, however, our data failed to show a strong effect of RIM1/2 removal on the inactivation of presynaptic Ca2+ currents, at least for short depolarizing steps of up to 20 ms lengths (Fig. 2C).
In wild-type calyces of Held, about 80% of the presynaptic Ca2+ current is mediated by P/Q-type Ca2+ channels, and N- and R-type Ca2+ channels make up the rest (Wu et al., 1999; Iwasaki et al., 2000). To test whether the reduction of the presynaptic Ca2+ current is accompanied by a change in the contribution of Ca2+ channel subtypes, we blocked Ca2+ currents sequentially with the P/Q-type specific toxin ω-agatoxin-IVa (agatoxin; 0.2 µM; Fig. 2I, green traces) followed by the N-type specific toxin ω-conotoxin-GVIa (conotoxin; 3 µM) in the continued presence of agatoxin (Fig. 2I; blue traces). In RIM1/2 cDKO calyces, 80.6 ± 14 % of the Ca2+ current was blocked by agatoxin, similar to the value in control calyces (92 ± 7.1 %; p = 0.14; Fig. 2J). Another 14.7 ± 10.3 % of the initial Ca2+ current in RIM1/2 cDKO calyces was blocked by conotoxin, as compared to 8.2 ± 7.2 % in control calyces. Thus, removal of RIM1/2 does not significantly alter the relative contribution of P/Q- and N-type Ca2+ channels. Taken together, direct recordings from the nerve terminal reveal a strong reduction of presynaptic Ca2+ currents in RIM1/2 cDKO neurons, which is specific for the nerve terminal since Ca2+ currents in the soma/dendritic compartment of MNTB neurons were unchanged (Fig. S2). Thus, RIM proteins have a so far unrecognized role in enriching voltage-gated Ca2+ channels at the presynaptic nerve terminal (see also Kaeser et al., submitted).
RIMs ensure a large readily-releasable pool and influence release probability
We showed that conditional removal of RIM1/2 leads to a strong reduction of transmitter release (by ~ 80%; Fig. 1), and that presynaptic Ca2+ currents are strongly reduced (~ 50%; Fig. 2). Does the reduced transmitter release primarily reflect a reduced release probability caused by the much smaller presynaptic Ca2+ influx, or are there other factors, like a reduced readily-releasable pool of vesicles (Calakos et al., 2004), which contribute to the decreased transmitter release? To investigate changes in pool size and release probability, we next used brief high-frequency trains of afferent fiber stimulation to measure the size of the readily-releasable pool (Fig. 3; Schneggenburger et al., 1999). In control synapses, the first EPSC was large (~ 8 nA in Fig. 3A), and subsequent EPSCs decreased in amplitude to a new steady-state value (Fig. 3A, B, right). In contrast, RIM1/2 cDKO synapses had much smaller EPSCs (~ 2 nA in Fig. 3A), and depression usually only occurred after the third or forth stimulus (Fig. 3A, B, left; see also Fig. 3D for the average over all cells). To quantify the onset of depression, we made line fits to relative depression curves in the range of the first to the sixth stimulus (Fig. 3B, blue fit lines). This analysis gave slopes of −62 ± 26 % per 5 stimuli (n = 8) and −27 ± 33 % per 5 stimuli (n = 9) for control, and RIM1/2 cDKO synapses, respectively (p < 0.05; see also Fig. 3D, bottom, for line fits to the averaged data sets for each genotype). Thus, the onset of depression was significantly slowed in RIM1/2 cDKO synapses, which suggests a decreased release probability of any given readily-releasable vesicle.
We next analyzed the apparent size of the readily-releasable pool by using the method of cumulative EPSC amplitudes back-extrapolated to time zero (Schneggenburger et al., 1999; Fig. 3C). The back-extrapolated cumulative EPSC amplitude was 51.1 ± 16.2 nA in control mice (corresponding to ~ 1700 vesicles assuming an average mEPSC amplitude of 30 pA; n = 8 cells), but only 11.9 ± 6.9 nA in RIM1/2 cDKO mice (~ 400 vesicles; n = 10 cells). Thus, there was a clear pool size reduction in RIM1/2 cDKO synapses (p < 0.001; Fig. 3E). The average release probability, calculated by dividing the first EPSC amplitude by the pool size estimate (Iwasaki and Takahashi, 2001), was 0.27 ± 0.09 (n = 8) and 0.19 ± 0.05 (n = 9) in control and RIM1/2 cDKO synapses, respectively (p = 0.04; Fig. 3F). These experiments with high-frequency trains show that the release deficit is primarily caused by a decreased pool of readily-releasable vesicles (reduction by ~ 75%; Fig. 3E). In addition, there was also a small but significant reduction of the release probability (by ~ 25 %), which might explain the observed slowing in the onset of synaptic depression.
Ca2+ uncaging reveals a smaller fast-releasable pool and a decreased Ca2+ sensitivity of release
We showed that in the absence of RIM1/2, the number of presynaptic Ca2+ channels was reduced ~ 50% (Fig. 2), and the readily-releasable pool was strongly reduced, together with a small reduction of the release probability (Fig. 3). To study the reduced readily-releasable pool size more directly, we used Ca2+ uncaging to strongly stimulate release independent of Ca2+ channel opening. In addition, Ca2+ uncaging will allow us to address the possibility of a reduced intrinsic Ca2+ sensitivity of release in RIM1/2 cDKO synapses, which could underlie the reduced release probability.
In RIM1/2 cDKO synapses, Ca2+ uncaging stimuli evoked EPSCs with small amplitudes (~ 6 nA in the example of Fig. 4B, left), and flashes that elevated [Ca2+]i above ~15 µM did not evoke EPSCs with larger amplitudes in RIM1/2 cDKO synapses (Fig. 4B), showing directly the limited pool of readily-releasable vesicles in RIM1/2 cDKO synapses. The maximal EPSC amplitudes at 10 – 15 µM [Ca2+]i were much smaller in RIM1/2 cDKO synapses (5.7 ± 4.9 nA, n = 7) than in control synapses (14.2 ± 7.8 nA, n = 6; p < 0.01), indicating a reduced pool size. To analyze the number of releasable vesicles and their release kinetics in more detail, we deconvolved the Ca2+ uncaging-evoked EPSCs to reveal rates of transmitter release (Fig. 4B, inset) and cumulative release rates (Fig. 4C). These were best fitted by the sum of at least two exponential functions (see Experimental Procedures), indicating a fast- and a slow release component in response to Ca2+ uncaging (Wölfel et al., 2007; Kochubey et al., 2009). Thus, the pool of readily-releasable vesicles can be kinetically subdivided into a fast- and a slowly releasable pool, FRP and SRP (Sakaba and Neher, 2001; Wölfel et al., 2007). To estimate the size of the FRP, we analyzed the number of vesicles released in the fast release component in response to [Ca2+]i steps to 10 – 15 µM. The FRP was strongly reduced, from 1091 ± 396 vesicles in control synapses, to 271 ± 178 vesicles in RIM1/2 cDKO synapses (n = 6 and 7 respectively; Fig. 4D). In addition, the amplitude of the slow release component was also reduced, from 833 ± 658 to 211 ± 205 vesicles in control and RIM1/2 cDKO synapses, respectively (p = 0.036).
We next plotted the absolute peak release rates as a function of the presynaptic [Ca2+]i step amplitude (Fig. 4E). This plot showed that the peak release rates were significantly smaller at all [Ca2+]i in RIM1/2 cDKO synapses as compared to control (p < 0.001; analysis of covariance, ANCOVA). However, the absolute peak release rates at any given [Ca2+]i are a function of the intrinsic Ca2+ sensitivity of release, as well as of the absolute pool size. Therefore, to normalize for the reduced FRP size, we divided the absolute peak release rates by the FRP estimated in each cell pair. This revealed slightly reduced pool-normalized release rates in RIM1/2 cDKO synapses (Fig. 4F), but this difference did not reach statistical significance (p = 0.13; ANCOVA). In contrast, other kinetic parameters of release, like the minimal delay and the fast release time constant, showed a significant slowing at all [Ca2+]i investigated (p < 0.001 and p < 0.01; see Fig. 4G, H), indicating that the intrinsic Ca2+ sensitivity of release was lower in the absence of RIM1/2.
To analyze the lowered intrinsic Ca2+ sensitivity quantitatively, the kinetic data, as well as the pool-normalized peak release rates, were globally fitted by a model of cooperative Ca2+ binding and vesicle fusion (Schneggenburger and Neher, 2000). The fits showed that a lowering of the on rate of Ca2+ binding (kon) and a slight lowering of the off rate (koff) led to a good description of the RIM1/2 cDKO data as compared to the control synapses (Fig. 4F, G, H; red and black fit lines, respectively; see Experimental Procedures for model parameters). The Ca2+ uncaging experiments therefore show that RIM1/2 proteins determine the size of the readily-releasable pool since both the FRP and SRP were reduced, and RIM1/2 increases the intracellular Ca2+ - sensitivity of release by a factor of ~ 1.5 to 2 - fold.
RIM proteins contribute to Ca2+ channel - vesicle coupling
We have shown that RIM proteins are necessary to enrich Ca2+ channels at the presynaptic nerve terminal (Fig. 2), and to maintain a high number of readily-releasable vesicles (Figs 3, 4). How well are the remaining readily-releasable vesicles coupled to the remaining Ca2+ channels? To address this question, we made paired pre- and postsynaptic recordings and performed a kinetic analysis of transmitter release in response to Ca2+ influx through voltage-gated Ca2+ channels (Fig. 5). Analyzing such data in the light of the intracellular Ca2+ sensitivities as determined by Ca2+ uncaging for each genotype (Fig. 4), should then allow us to examine the efficiency of the coupling between Ca2+ channels and readily-releasable vesicles (Wadel et al., 2007).
In most experiments, the presynaptic membrane potential was briefly stepped to +80 mV to open Ca2+ channels rapidly, and then returned to 0 mV to admit a pulse-like presynaptic Ca2+ influx (Fig. 5A, B, top; Sakaba and Neher, 2001). As expected, the resulting Ca2+ currents were smaller in RIM1/2 cDKO calyces (Fig. 5A, top), and the EPSCs in response to such pool-depleting Ca2+ currents were significantly smaller in RIM1/2 cDKO synapses (6.8 ± 2.4 nA; n = 6) as compared to control (25.9 ± 6.4 nA; n = 5; p < 0.001), indicative of the reduced pool size (see above). Interestingly, the 20 – 80% rise time of the EPSCs was prolonged in RIM1/2 cDKO synapses (3.4 ± 1.5 ms; n = 6) as compared to control synapses (1.24 ± 0.4 ms, n = 5; p = 0.012), which indicates an additional deficit in the kinetics of transmitter release.
To investigate the defects in release kinetics in more detail, we deconvolved the EPSCs to derive transmitter release rates (Fig. 5B, black traces), and traces of cumulative release (Fig. 5C, black trace below blue fit line). The peak release rates were strongly reduced in RIM1/2 cDKO synapses (Fig. 5D) and the width of the transmitter release at half-maximal amplitudes was longer in RIM1/2 cDKO synapses (5.1 ± 1.8 ms, n = 6) than in control (2.3 ± 1.1 ms, n = 5; p < 0.05). The integrated release rate traces were fitted with a series of single- and double exponential function with or without line component, to determine the best fit function (see Experimental Procedures). In both genotypes, cumulative release was best fitted by functions which contained at least two exponential components (Fig. 5C, blue fit lines), indicating a fast- and a slow release component (Sakaba and Neher, 2001; Wadel et al., 2007; Wölfel et al., 2007). In RIM1/2 cDKO synapses, the fast release time constant was significantly slower (5.2 ± 1.7 ms, n = 6) than in control synapses (1.8 ± 0.8 ms, n = 5; Fig. 5E; p = 0.002), but is was significantly faster than the slow release time constant in control synapses, which was 23 ± 3.7 ms (n = 5; Fig. 5F; p < 0.001). Similarly, when cumulative release traces were arbitrarily fitted with monoexponential functions, the resulting time constant in RIM1/2 cDKO synapses (9.3 ± 1.1 ms; n = 6) was still significantly faster than the slow release time constant in wild-type cells (p < 0.001). Both of these comparisons show that the FRP is not simply missing completely, but rather, that release from the remaining FRP is slowed in the RIM1/2 cDKO synapses. Figure 5 (E, F) shows further parameters extracted from the kinetic analysis of transmitter release for each genotype. Overall, the analysis shows a strongly reduced number of readily-releasable vesicles in both the FRP and the SRP, as well as a significant, ~ 2.5 -fold slowing of the fast release component.
The kinetics of transmitter release in response to Ca2+ influx depends on the intrinsic speed of release, as well as on the 'local' [Ca2+]i that builds up close to the readily -releasable vesicles, which, in turn, is a function of the distance between Ca2+ channels and vesicles (Neher, 1998; Wadel et al., 2007). The Ca2+ uncaging experiments showed that the intrinsic Ca2+ sensitivity is reduced in the absence of RIM1/2 (Fig. 4). To ask whether the spatial coupling between Ca2+ channels and vesicles was impaired as well, we back-calculated the 'local' [Ca2+]i that was necessary to reproduce the kinetics of the fast release component in response to depolarizations (Fig. 5B, C; grey traces; Schneggenburger and Neher, 2000). This was done by using the specific sets of kinetic parameters which describe the intracellular Ca2+ sensitivities of transmitter release of RIM1/2 cDKO - and control synapses (Fig. 4). In the examples of Fig. 5C, a step-like local [Ca2+]i signal of 7.7 µM predicted the time-course of the fast release component in the RIM1/2 cDKO synapse, whereas a [Ca2+]i signal of 9.4 µM was necessary in the case of the control synapse. On average, the back-calculated local [Ca2+]i signal was 12.0 ± 2.5 µM (n = 5) and 9.0 ± 1.2 µM (n = 6) in control - and RIM1/2 cDKO synapses, respectively (Fig. 5G; p < 0.05). Thus, the local [Ca2+]i signal experienced by average readily-releasable vesicles during a Ca2+ current at 0 mV is significantly smaller in RIM1/2 cDKO synapses. This suggests that there are either fewer 'local' Ca2+ channels around each given readily-releasable vesicle, and/or that the average distance between Ca2+ channels and vesicles is increased in the absence of RIM1/2.
In further experiments designed to analyze a decreased coupling between Ca2+ channels and vesicles, we measured the suppression of EPSCs by the slow Ca2+ buffer, EGTA-AM (Fig. S3). These experiments showed a trend towards a faster block by EGTA-AM in RIM1/2 cDKO synapses, as would be expected for a longer Ca2+ channel - vesicle distance (Borst and Sakmann, 1996; Fedchyshyn and Wang, 2005); however, the difference did not reach statistical significance (p = 0.073).
RIMs dock vesicles to the active zone
We showed that RIM1/2 deletion led to a strong reduction of the readily-releasable pool (Figs 3–5). Does this reduction of the functional pool size reflect a deficit in "priming" docked vesicles to fusion competence as suggested before (Koushika et al., 2001; Calakos et al., 2004); or else, might RIM proteins have an additional role in vesicle docking? To distinguish between these possibilities, we investigated the synaptic ultrastructure of RIM1/2 cDKO calyces and control calyces using serial section transmission electron microscopy (EM) (Fig. 6). Large calyx of Held nerve terminals in the MNTB area of both genotypes had overall normal appearance (not shown). In high-resolution images of active zones, there was a conspicuous reduction in the number of vesicles at active zones, and fewer docked vesicles were apparent (Fig. 6A), suggesting that RIM1/2 is involved in vesicle docking.
To quantify the spatial distribution of vesicles, we reconstructed entire active zones, taking into account all detected vesicles within a distance of 300 nm to the active zone membrane (Fig. 6B). From the reconstructions, histograms of the shortest membrane-to-membrane distance between each vesicle and the active zone were computed (Fig. 6C; n = 18 and 17 active zones for RIM1/2 cDKO and control tissue, sampled over n = 4 calyces each). For the control data, there was a clear peak for the membrane - nearest bin (10 nm or less; Fig. 5C, arrow), which most likely represents the pool of docked vesicles (Verhage and Sorensen, 2008). Importantly, in RIM1/2 cDKO synapses, the vesicle number in this membrane-near bin was strongly reduced (Fig. 6C; arrow). Fig. 6D shows the relative vesicle number (RIM1/2 cDKO / control * 100 for each bin), which illustrates a quite selective decrease in the membrane-near bin, although there was also a modest decrease in the number of vesicles located further away in the cytoplasm (~ 20%; Fig. 5D). Defining "docked" vesicles as those that are located within 10 nm of the active zone membrane, we found 7.0 ± 4.6 docked vesicles in control synapses (n = 17 active zones), but only 1.5 ± 1.8 in RIM1/2 cDKO synapses (n = 18; Fig. 6E; p < 0.001). This shows a drastic reduction of the number of vesicles docked at the active zone membrane in RIM1/2 cDKO synapses.
In c.elegans synapses, RIM1 enables the lateral localization of docked vesicles close to a central membrane specialization of the active zone (Gracheva et al., 2008). In analogy, it is possible that in mammalian synapses, the loss of RIM proteins could lead to a lateral mis - localization of docked vesicles into areas adjacent to the active zone ("outliers"). To address this possibility, we made flat surface renderings of each three-dimensionally reconstructed active zone and its adjacent plasma membrane (Fig. 6F), and then analyzed the density of "outlier" docked vesicles, which were defined as docked vesicles localized up to 100 nm outside of active zones (Fig. 6F, see green symbols). As can be seen in the example images in Fig. 6F, active zone size varied greatly between individual contact sites (Schikorski and Stevens, 1997; Taschenberger et al., 2002), but the average active zone size was unchanged between the genotypes (Fig. 6G, H). Overall, we only found n = 8 and n = 9 outlier vesicles in the set of n = 17 and 18 active zones analyzed here. Normalized to the corresponding membrane area, the density of outliers was similarly low for both genotypes (~ 3 – 4 vesicles / µm2; see TableS1); note that this value is less than 5% of the density of docked vesicles within the active zones of wild-type synapses (Fig. 6 I). Thus, removal of RIM proteins specifically reduces the density of docked vesicles within the active zone (Fig. 5I, p < 0.001), but does not affect the number of vesicles docked adjacent to the active zone.
Discussion
We have established a Cre-lox based conditional KO approach at a presynaptically accessible CNS synapse, the calyx of Held. This has allowed us to use presynaptic recordings and Ca2+ uncaging, as well as EM analyses of synapses which have developed in vivo, to directly study the presynaptic functions of RIM proteins. We have found three main roles of RIM proteins: First, the presynaptic Ca2+ current density was strongly reduced about two-fold in RIM1/2 cDKO nerve terminals. This, together with the accompanying paper by Kaeser et al. (submitted to Cell), establishes an important role for RIM proteins in localizing Ca2+ channels to the active zone. Second, we find a reduced pool of readily-releasable vesicles in agreement with previous studies (Calakos et al., 2004), and a decreased number of membrane-near vesicles at the active zone, revealing a vesicle docking function of RIM proteins. Third, RIM proteins speed the rate of transmitter release by increasing the intrinsic Ca2+-sensitivity of release, as well as by contributing to the tight co-localization of readily-releasable vesicles with Ca2+ channels. Taken together, our study shows that RIM proteins coordinately regulate Ca2+ channel targeting, vesicle docking and priming, and Ca2+ channel - vesicle co-localization at the presynaptic active zone.
Conditional knock out approach at the calyx of Held
For the generation of calyx-specific conditional knock-out mice, we have made use of recently generated floxed mouse lines for RIM1αβ (Kaeser et al., 2008) and RIM2αβγ (Kaeser et al., submitted), and of a previously available Cre knock-in mouse line in the Krox20 locus (Voiculescu et al., 2000). The presynaptic neuron pool that generates the large calyx of Held nerve terminals onto MNTB neurons is located in the contralateral VCN, and is largely represented by globular bushy cells (Cant and Benson, 2003). Krox20 is a transcription factor that is highly specifically active in rombomeres 3 and 5 of the developing hindbrain (Voiculescu et al., 2000), which give rise to a majority of neurons in the VCN (Farago et al., 2006; Maricich et al., 2009). We found homogeneous phenotypes amongst the recorded calyx of Held synapses, which indicates, together with morphological analysis (Fig. 1B; L. Xiao, N. Michalski & R.S., unpublished observations; Renier et al., 2010) that the entire population of calyx of Held - generating neurons stems from Krox20Cre positive neurons. Thus, the Krox20Cre mouse line allows to conditionally remove floxed alleles at the calyx of Held synapse, which will make it a useful tool to advance our understanding also of other proteins of the presynaptic vesicle cycle.
RIM proteins localize Ca2+ channels to the active zone
Using direct presynaptic recordings at the nerve terminal, we demonstrated that RIM proteins are essential for localizing Ca2+ channels to the active zone, as shown by the clear decrease in the presynaptic Ca2+ current density in RIM1/2 cDKO calyces. These direct recordings at the nerve terminal show that RIMs determine presynaptic Ca2+ channel density without changing major biophysical parameters of Ca2+ channel gating, although we cannot exclude that RIMs influence Ca2+ channel inactivation with prolonged pulses (> 50 ms, Fig. 2; Kiyonaka et al., 2007); this, however, will be relevant only for prolonged presynaptic AP trains. Analyzing RIM-dependent presynaptic Ca2+ channel targeting has been limited because previously no KO mice deleting all RIM1/2 isoforms were available (Schoch et al., 2002; Calakos et al., 2004), and because previously investigated synapses, including the c.elegans neuromuscular synapse (Koushika et al., 2001), did not allow for measurements of presynaptic Ca2+ currents. Using cultured RIM1/2 cDKO neurons, Kaeser et al. (submitted to Cell) have observed an about two-fold reduction in Ca2+ transients in presynaptic boutons during an AP, and observed an equal reduction in the staining intensity with anti-α1A Ca2+ channel subunit antibodies. This, together with our finding that presynaptic APs are unchanged (Fig. 2), is evidence for a reduced Ca2+ channel density also at small bouton-like synapses. We conclude that the role of RIM1/2 proteins in enriching Ca2+ channels at the nerve terminal is a widespread mechanism found at many CNS synapses including the calyx of Held, and hippocampal excitatory and inhibitory synapses (Kaeser et al., submitted).
What might be the molecular mechanism by which RIM proteins hold Ca2+ channels at the active zone? In a parallel study, Kaeser et al. (submitted) showed that the RIM1 and RIM2 PDZ domains directly bind to the C-terminal sequences of the P/Q- and N-type Ca2+ channel α-subunits, and that the PDZ domain was required to rescue the decreased Ca2+ transients and the abnormal Ca2+ channel localization. In addition, the proline-rich domain of RIM1/2 was also necessary for the rescue, suggesting that a tripartite interaction between RIM1/2, RIM-BPs (which bind to the proline-rich domain of RIMs; Hibino et al., 2002) and the Ca2+ channel α subunits is critical for the Ca2+ channel targeting function of RIM1/2 (Kaeser et al., submitted). This, together with the present work identifies RIM1/2 as a presynaptic scaffolding proteins with a clear role in maintaining a high Ca2+ channel density at the presynaptic active zone. Previous work has suggested a role for Bruchpilot, a drosophila gene related to ELKS/CAST proteins, in maintaining presynaptic Ca2+ channel density and structural entirety at drosophila presynaptic active zones (Kittel et al., 2006).
Conditional removal of RIM1/2 did not significantly change the relative contribution of P/Q-type - and N-type channels to the total presynaptic Ca2+ current, despite a strongly reduced total Ca2+ current. This finding is different to the situation in P/Q-type (α1A-subunit) KO mice (Jun et al., 1999), in which a strong compensatory upregulation of presynaptic N-type channels was observed at the calyx of Held (Inchauspe et al., 2004; Ishikawa et al., 2005). Thus, in the absence of RIM1/2, N-type Ca2+ channels are not capable to compensate for the missing P/Q-type channels and therefore, the absence of RIM1/2 likely affects both Ca2+ channel α subunits equally. This agrees with the finding by Kaeser et al. (submitted) who showed that RIM1/2 binds to both P/Q- and N-type channel α-subunits.
RIMs' function in vesicle docking and formation of the readily-releasable pool
The calyx synapse has been an ideal preparation to functionally define a fast and a slow subpool of the readily-releasable pool (Sakaba and Neher, 2001; Wölfel et al., 2007; Wadel et al., 2007; see Neher, 2006 for a review). Here, we find that conditional removal of all major RIM isoforms leads to a strong, ~ 70% decrease of the readily-releasable pool size as defined by various types of pool-depleting Ca2+ stimuli (Figs 3–5). Importantly, we found a very similar decrease of the number of docked vesicles at the active zone (by ~ 70%; Fig. 6), demonstrating a genetic manipulation that leads to a parallel decrease in the number of docked vesicles, and of the readily-releasable pool size determined functionally. Thus, at the calyx of Held, the amount of vesicle docking seems to determine the size of the readily releasable pool. This conclusion is further supported by the reasonable quantitative agreement between the number of docked vesicles on the one hand (~ 7 docked vesicle per active zone * 500 ≈ 3500; assuming that a calyx has ~ 500 active zones; Sätzler et al., 2002; Taschenberger et al., 2002), and the sum of FRP and SRP vesicles on the other hand (~ 3000 – 3500; see Fig. 5). This indicates that most docked vesicles belong to the readily-releasable pool at the wild-type calyx of Held. Genetic removal of all RIM1/2 isoforms strongly reduced docking, and thereby determined the size of the readily-releasable pool. This conclusion does not rule out the possibility that an additional priming step is necessary to make docked vesicles fusion-competent (see Südhof, 2004 for review), and that RIMs might have an additional role in vesicle priming (Koushika et al., 2001; Calakos et al., 2004).
Further work is needed to unravel the molecular mechanisms by which RIM determines vesicle docking, and how vesicle docking and priming are related to each other. The long isoforms of RIMs interact via their N-termini with Munc13, and with the small GTPase Rab3 (Wang et al., 1997; Dulubova et al., 2005) and related Rab's including Rab8A, −10, and −26 (Fukuda, 2003). It is thought that the interaction of RIMs with Munc13 is important for priming docked vesicles to fusion competence (Betz et al., 2001), since Munc13 was described as a priming factor with no role in vesicle docking (Augustin et al., 1999). However, recent studies on Munc13 suggested also a role in docking (Siksou et al., 2009), somewhat blurring the distinction between vesicle docking and priming. Single Rab3A KO mice exhibit a deficit in the activity-dependent recruitment of docked vesicles in synaptosomes (Leenders et al., 2001) and show a vesicle docking phenotype at the neuromuscular junction (Coleman et al., 2007), but surprisingly, quadruple Rab3A/B/C/D KO mice do not exhibit a docking phenotype in cultured hippocampal neurons (Schlüter et al., 2004). Taken together, the interaction of the long RIM isoforms with Rab3 and related Rabs could explain the docking function of RIM proteins, and it is possible that in RIM1α KO mice (Schoch et al., 2002) the docking deficit was compensated by the continued presence of RIM1β, 2α, and 2β. Thus, our experiments in the context of previous data show that RIM proteins have an important role in vesicle docking.
RIMs influence release probability and the intrinsic Ca2+ -dependent speed of release
A third role of RIM proteins regards the release probability of any given readily-releasable vesicle. Kinetic analysis showed a clear slowing of the release of the remaining FRP vesicles in RIM1/2 cDKO synapses (Fig. 5). This was mediated, in part, by a reduction of the intracellular Ca2+ sensitivity of release demonstrated in Ca2+ uncaging experiments (Fig. 4), mediated by a so far unknown molecular mechanism of RIM. In addition, there was a defect in the coupling between Ca2+ channels and vesicles for FRP vesicles, visible as a decreased 'local' [Ca2+]i signal that we back-calculated during stimulation of release with presynaptic depolarizations (Fig. 5). Thus, RIM proteins contribute to a tight Ca2+ channel - vesicle co-localization, a function which likely reflects the interaction of RIMs with Ca2+ channels on the one hand (see above; Kaeser et al., submitted), and with vesicle proteins like Rab3 on the other hand.
Taken together, establishing a conditional KO approach at a presynaptically accessible CNS synapse has allowed us to dissect multiple intertwined roles of the presynaptic scaffolding protein RIM1/2. Overall, the interaction of RIM proteins with a large number of presynaptic proteins (Schoch et al., 2002) allow RIMs to influence several important functions vital for fast transmitter release: first, the targeting of Ca2+ channels to the active zone, likely mediated by interactions of the central RIM1/2 PDZ domain with Ca2+ channel α-subunits (Kaeser et al., submitted); second, vesicle docking and the formation of a standing readily-releasable pool important for maintaining fast release during repeated stimuli (Sorensen, 2004); and third, intrinsic speeding of release and a tighter coupling between vesicles and Ca2+ channels. Thus, RIM proteins coordinate multiple functions late in the vesicle cycle which all guarantee a fast speed of Ca2+ evoked release at CNS synapses.
Experimental Procedures
Conditional RIM1/2 KO mice specific for the auditory brainstem
We identified the Krox20Cre mouse line (Voiculescu et al., 2000); gift of Dr. Patrick Charnay, Paris, France) as a suitable Cre mouse line which drives Cre expression in calyx of Held - generating neurons of the VCN (Fig. 1A, and Fig. S1). We crossed heterozygous Krox20+/Cre mice with a mouse line which carried a floxed RIM1 allele (Kaeser et al., 2008), as well as a floxed RIM2 allele (Kaeser et al., submitted) (see also Supplementary Experimental Procedures). The offspring of the final breeding pairs gave rise to an expected 50 % Cre-positive, RIM1lox/Δ, RIM2lox/Δ mice. Due to germline recombination in the Krox20Cre line (Voiculescu et al., 2000), one of each floxed RIM allele was deleted in these mice as confirmed by PCR-based genotyping. Synapses recorded in these mice are referred to as RIM1/2 cDKO synapses (for conditional double KO). Since Cre-expression turns on at ~ E11 in Krox20+/Cre mice (Voiculescu et al., 2000), the floxed RIM1/2 alleles should be deleted even before synapses initially form at ~ E17 in brainstem. As control mice, we used Cre-negative littermate mice with otherwise the same genetic background; thus, the control mice were heterozygous with respect to the RIM alleles. Cre-positive, RIM1lox/Δ, RIM2lox/Δ mice were viable and fertile, and were used for further interbreeding. For the analysis of neuron populations in which Cre-recombinase was active, we crossed Krox20+/Cre mice with tdRFP reporter mice (Luche et al., 2007), and performed anti-RFP and anti-Syt2 immunohistochemistry (see Supplementary Experimental Procedures) to reveal Cre-positive neurons and nerve terminals (Fig. 1A, B; Fig. S1).
Slice preparation and electrophysiology
Transverse brainstem slices were prepared from postnatal (P) 9 – 11 days mice according to standard methods, using a LEICA VT1000S slicer. Paired pre- and postsynaptic whole-cell recordings at the calyx of Held synapse were made with an EPC10/double patch-clamp amplifier (HEKA), under visualization in an upright microscope (Zeiss Axioskop 2 FS) equipped with gradient contrast infrared visualization (Luigs & Neumann) and a 60× objective. Details on the electrophysiological methods, and on the composition of the patch pipette - and extracellular solutions are provided in Supplementary Experimental Procedures.
EPSC deconvolution and data analysis
Deconvolution of EPSCs to calculate the rates of transmitter release was done similarly as first described by (Neher and Sakaba, 2001), using routines written in IgorPro. The deconvolution analysis assumes that mEPSC with a double-exponential decay (Schneggenburger and Neher, 2000) add linearly to give rise to an evoked EPSC. The calculated release rates were corrected for a contribution of a spillover glutamate current as described (Neher and Sakaba, 2001). Cumulative release traces were obtained by simple integration of the transmitter release traces, without further correction for an assumed recovery process. Cumulative release traces were fitted with the following functions: single-exponential, exponential plus line, double-exponential, double-exponential plus line, and triple-exponential (Wölfel et al., 2007), and the best-fit function was selected based on the Bayesian information criterion (BIC; Kochubey et al., 2009). Data are reported as average ± S.D. values, and statistical significance was evaluated with Student's t-test, and accepted at p < 0.05. For the comparison of release rates, release delays and fast release time constants between two data sets at various [Ca2+]i (Fig. 4E–H), the data sets were double-logarithmized, and then assessed for statistical significance by analysis of covariance (ANCOVA). The Ca2+ uncaging data was fitted by a five-site model of Ca2+ binding and vesicle fusion (Schneggenburger and Neher, 2000). The following parameters were used for control / RIM1/2 cDKO synapses respectively: kon, 1.65 * 108 / 1.05 * 108 [M−1s−1]; koff, 7000 / 5000 [s−1]; pool size, 315 / 1390 vesicles. The remaining parameters were the same for both data sets (cooperativity factor b, 0.35; final fusion rate γ, 7000 s−1).
Presynaptic Ca2+ uncaging
Ca2+ uncaging was done with a DP-10 flash-lamp (Rapp Optoelektronik) according to standard procedures described before (Schneggenburger and Neher, 2000; Wölfel et al., 2007); details are given in Supplementary Experimental Procedures.
Electron microscopy
Transmission EM was performed in the MNTB area of a RIM1/2 cDKO mouse and its control cre-negative littermate (both at P11), using standard fixation and resin embedding procedures (see Supplementary Experimental Procedures). Serial images were taken with a Philips CM10 TEM operated at 80 kV at a magnification of 16000 times, using 10 – 20 adjacent sections. Only active zones that were completely contained in the series were analyzed. The image series were aligned and active zones, including vesicles and surrounding plasma membrane, were reconstructed in 3D with the Fiji software (http://pacific.mpi-cbg.de/wiki/index.php/Main_Page). The shortest distance from the vesicle membrane to the active zone membrane was then calculated in the 3D model, and all vesicles at distances of less than 300 nm were taken into account. Flat rendering of the active zone surface was done by a MatLab function.
Supplementary Material
Acknowledgments
We thank Heather Murray for expert technical assistance; Dr. Graham Knott (Center for Interdisciplinary Electron Microscopy; EPFL) for help and advice with EM; Dr. Daniel Keller for help with flat surface rendering of active zone profiles; Dr. Patrick Charnay and Dr. Hans Jörg Fehling for the gift of mouse lines, and Dr. Olexiy Kochubey, Dr. Erwin Neher and Dr. David Perkel for comments on the manuscript. This research was supported by grants from the Swiss National Science Foundation (SNF; 31003A_122496) and the Synapsis foundation (both to R.S.).
Footnotes
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