GABAergic synaptic transmission regulates calcium influx during spike-timing dependent plasticity

Introduction

GABAergic synaptic transmission can be either excitatory or inhibitory at different stages of nervous system development (Kaila, 1994 ; Blaesse et al., 2009 ), or during various pathological states (Kahle et al., 2008 ). The polarity of GABAergic transmission (hyperpolarizing versus depolarizing) depends on the intracellular concentration of Cl⁻ ([Cl⁻]_i); this is because the GABA_A receptor is a Cl⁻-permeable ion channel (Kaila, 1994 ). The [Cl⁻]_i is largely determined by the cation-chloride cotransporters expressed in the neuronal membrane: NKCC1 accumulates Cl⁻ into the neuron (Yamada et al., 2004 ; Dzhala et al., 2005 ), while KCC2 transports it out (Rivera et al., 1999 ). When neuronal Cl⁻ is relatively high due to the dominant expression of NKCC1 during early development, the reversal potential for GABA (E_GABA ≈ E_Cl) is depolarized with respect to the resting membrane potential and so GABAergic transmission is depolarizing and sometimes excitatory. In contrast, when neuronal Cl⁻ is low due to the expression of KCC2 in the mature nervous system, E_Cl is hyperpolarized with respect to the resting membrane potential making GABAergic transmission inhibitory.

Recent studies have demonstrated that NKCC1 and KCC2 transporter function is not only regulated by their developmental program, but can also be regulated by neuronal activity (Fiumelli and Woodin, 2007 ; Blaesse et al., 2009 ). Coincident pre- and postsynaptic activity at GABAergic synapses results in GABAergic STDP (Woodin et al., 2003 ; Fiumelli and Woodin, 2007 ; Balena and Woodin, 2008 ; Saraga et al., 2008 ; Xu et al., 2008 ; Ormond and Woodin, 2009 ). Early in development, coincident pre- and postsynaptic activity strengthens inhibition through a Ca²⁺-dependent regulation of NKCC1, which hyperpolarizes E_Cl (Balena and Woodin, 2008 ). The same pattern of neuronal activity also modifies GABAergic transmission in the mature nervous system through a Ca²⁺-dependent decrease in KCC2 activity, which depolarizes E_Cl (Woodin et al., 2003 ). The spike-timing window for mature GABAergic inhibition has been characterized as symmetrical. Both positive and negative spike-timing intervals (within 15 ms; ±15 ms) decrease the strength of inhibition due to E_Cl depolarization (as described above). Non-coincident activity (±50 ms) also reduces inhibition, but through a decrease in conductance (Woodin et al., 2003 ).

During GABAergic STDP the Ca²⁺ influx occurs via voltage-gated Ca²⁺ channels (VGCCs) (Woodin et al., 2003 ) opened by the back-propagating action potential. When glutamatergic transmission occurs simultaneously with GABAergic STDP induction in hippocampal slices, Ca²⁺ can also influx via NMDARs (Ormond and Woodin, 2009 ). Because the opening of VGCCs and NMDARs are voltage-dependent, we hypothesize that GABAergic transmission, which regulates the postsynaptic membrane potential, will regulate the opening of these Ca²⁺ channel proteins. In turn, this would regulate the Ca²⁺ influx during GABAergic STDP. It is important to understand how GABAergic synapses regulate Ca²⁺ influx, because the magnitude of this influx can determine the outcome of plasticity induction (Kano, 1994 ; Bi and Poo, 1998 ; Nishiyama et al., 2000 ; Dan and Poo, 2006 ).

We examined Ca²⁺ dynamics during STDP induction in hippocampal neurons which have formed either depolarizing or hyperpolarizing GABAergic synapses. Using perforated patch-clamp recordings (with gramicidin) and imaging postsynaptic Ca²⁺ (using Fluo4), we investigated how the polarity and strength of GABAergic transmission regulates Ca²⁺ influx. We further analyzed this relationship by examining several aspects of GABAergic transmission, including GABA_A conductance, E_Cl, and Cl⁻ driving force. We found that GABA_A-mediated transmission regulates Ca²⁺ influx during the induction of STDP, with the strength of the synapse significantly altering the magnitude of the postsynaptic Ca²⁺ influx in a linear fashion.

Materials and Methods

Hippocampal Cultures

Low-density cultures of dissociated embryonic rat hippocampal neurons were prepared as previously described (Balena and Woodin, 2008 ). In brief, embryonic day 18 (E18) pregnant Sprague-Dawley rats were briefly exposed to carbon dioxide and cervically dislocated in accordance with guidelines from the University of Toronto Animal Care Committee and the Canadian Council on Animal Care. Hippocampi were then removed and treated with trypsin for 15 min at 37°C, followed by gentle trituration. The dissociated cells were plated at a density of 50,000 cells/mL on poly-l-lysine coated 25 mm glass coverslips (in 35 mm Petri dishes). Cells were plated in Neurobasal medium (Invitrogen, Carlsbad, California, USA), supplemented with 2% B-27 (Invitrogen, Carlsbad, California, USA). Twenty-four hours after plating, half of the medium was replaced with the original plating medium containing 20 mM KCl. Forty-eight hours after plating, and every 3 days following, one third of the medium was replaced with DMEM (Invitrogen, Carlsbad, California, USA) supplemented with 10% heat-inactivated fetal bovine serum (Invitrogen, Carlsbad, California, USA), 10% Ham’s F12 with l-glutamine (Invitrogen, Carlsbad, California, USA), 1% penicillin-streptomycin (Sigma-Adrich, Oakville, Ontario, Canada), 10 mM KCl and 15 mM HEPES. Both glia and neurons were present under these culture conditions. Cells were recorded from after 8–13 days in culture.

Electrophysiology

Whole-cell perforated patch recordings using gramicidin (50 µg/mL; Sigma-Adrich, Oakville, Ontario, Canada) were performed on pairs of synaptically connected cultured hippocampal neurons. The recording pipettes were made from glass capillaries (World Precision Instruments Inc., Sarasota, Florida, USA), with a resistance of 4–10 MΩ. The pipettes were filled with an internal solution containing 150 mM KCl, 10 mM HEPES, and gramicidin, pH 7.4, osmolarity = 300 mOsmol. The cultures were continuously perfused (approximately 1 mL/min) with extracellular recording solution containing (in mM): 150 NaCl, 3 KCl, 3 CaCl₂·2H₂O, 2 MgCl₂·6H₂O, 10 HEPES, 5 Glucose, pH 7.4, osmolarity = 307–315 mOsmol. Recordings were performed with a MultiClamp 700B (Molecular Devices Inc., Sunnyvale, California, USA) patch-clamp amplifier. Signals were filtered at 5 kHz using amplifier circuitry. Data was acquired and analyzed using Clampfit 9 (Molecular Devices Inc., Sunnyvale, California, USA). Recordings started after the series resistance had dropped below 30 MΩ. For assaying synaptic connectivity, each neuron was stimulated at a low frequency (0.05 Hz) by a 1 ms step depolarization from −70 to +20 mV in voltage-clamp mode. GPSCs were distinguishable from excitatory postsynaptic currents (EPSCs) by longer decay times. Upon occasion we did detect autaptic GABAergic synapses in our cultures, however we did not examine these synapses in the present study. During the STDP induction protocol both neurons were switched to current-clamp mode and injected with current (minimal stimulation, 2 ms) both pre- and postsynaptically to generate an action potential in each cell at a frequency of 5 Hz for 30 s. The interval between spike induction was ±5 ms, which resulted in a spike-timing interval of ±1 ms between onset of the GABAergic postsynaptic potential (GPSP) and the postsynaptic action potential. This protocol resulted in 150 pairs of pre- and postsynaptic action potentials. All recordings were performed at room temperature (25°C).

The resting membrane potential was determined in current-clamp mode in the absence of current injection or synaptic activity. E_Cl was determined by varying the holding potential of the postsynaptic cell in 10 mV increments and measuring the resulting GPSC amplitude; each set of current-voltage (I–V) measurements was repeated after a 5-min interval. A linear regression of both sets of GPSC amplitude measurements was then used to calculate the voltage dependence of GPSCs. The intercept of this line with the abscissa was taken as E_Cl. The slope of the same line was taken as GPSC conductance. The difference between the resting membrane potential and E_Cl was taken as the driving force.

GABA_A receptors are permeable to both HCO_3⁻ and Cl⁻ (∼0.2–0.4 ratio; Kaila, 1994 ). Due to the relatively positive HCO_3⁻ equilibrium potential (∼−10 mV), which is set by mechanisms that control intracellular pH regulation (Kaila and Voipio, 1987 ), HCO_3⁻ mediates an inward, depolarizing current (Kaila and Voipio, 1987 ; Kaila et al., 1993 ; Gulledge and Stuart, 2003 ). However, our experiments were performed in bicarbonate-free solution buffered with HEPES, and thus GABA_A receptor activation was solely mediating a Cl⁻ current. For this reason we report E_Cl and not E_GABA.

Fluorescence Imaging

To assess the effect of STDP induction on postsynaptic Ca²⁺ influx the hippocampal neurons were loaded with the membrane-permeable fluorescent Ca²⁺ indicator Fluo4-AM (Invitrogen; Carlsbad, CA, USA) for 30 min at 37°C, 5% CO₂. The Fluo4 was dissolved in dimethyl sulfoxide (DMSO) and 20% pluronic acid to a stock concentration of 1 mM and then diluted to 1 µM in our extracellular recording solution. Following dye-loading the cells were thoroughly washed with extracellular recording solution. Cells were then transferred to the recording chamber of an inverted microscope (Olympus IX71) equipped with an Olympus 0.6 NA × 40 objective. Fluo4 was excited at 488 nm through a monochromator (Photon Technology International (Canada) Inc., London, ON), controlled by the ImageMaster software (Photon Technology International (Canada) Inc., London, ON). Fluorescence emission of labeled cells at 510 nm was detected with a 16-bit CCD camera (Cascade 650, Photometrics, Roper Scientific, Tuscon, AZ, USA). Images of 653 × 492 pixels were accumulated at 500–1000 ms intervals.

Fluorescence Analysis

Analysis of the fluorescence signals was performed off-line on the image sequences as they were originally acquired. Analysis was performed on regions of interest (ROIs) that encompassed approximately 80% of the soma (which ranged from 10–50 µM in diameter). Fluorescence was plotted against time to yield a graph of the fluorescence changes over the STDP induction period. F₀ was taken to be the fluorescence from the last image before induction began. F_peak was taken to be the maximum fluorescence level reached over the course of the induction. F₃₀ was taken to be the fluorescence from the final image during the induction period. ΔF₃₀ was calculated as the percentage difference between F₀ and F₃₀; ΔF_peak was calculated as the percentage difference between F₀ and F_peak. The area under the graph was normalized to F₀ to provide F_area. We determined that photobleaching did not impact our Ca²⁺ analysis. This determination was made by comparing the fluorescence of quiescent cells during the first and last 5 s of a 30-s image acquisition and finding no significant difference in fluorescence (p = 0.06). Thus, we did not alter the image analysis further to account for photobleaching.

Statistical Analysis

All data are presented as mean ± SEM. Linear regression analysis was used to obtain correlation coefficients and corresponding p-values. One-way ANOVA was used to compare the F_area values of depolarizing and hyperpolarizing synapses to those of neurons fired alone (post only). Paired t-tests were used to compare E_Cl and resting membrane potential values when those values were obtained from the same neurons. All other statistical analysis used unpaired t-tests. All statistical analysis was performed using SigmaStat 2.03.

Results

Characterization and Localization of GABAergic Synapses

In order to examine Ca²⁺ influx during STDP induction, we first had to locate synaptically connected neurons and characterize the synapse between them. We did this using dual perforated patch-clamp recordings from pairs of hippocampal neurons cultured at a low density. Hippocampal cultures were prepared from E18 rats and recorded from after 8–13 days in culture; they contained glia, pyramidal neurons and GABAergic interneurons. Synaptic connections were identified by stimulating one neuron and monitoring for the presence of postsynaptic currents in the other. After we located a synapse, our first indication that it was GABAergic came from the relatively long time course of the GPSC in voltage-clamp mode (35.50 ± 3.37 ms for GPSCs, as opposed to 5.76 ± 0.64 ms for glutamatergic currents; Balena and Woodin, 2008 ). If the synapse had a time course consistent with GABAergic currents we then determined the E_Cl by constructing an I–V curve; the intersection of the curve with the x-axis was taken to be E_Cl (Figures 1 A,B). Because the extracellular recording solution was free of HCO_3⁻, E_Cl ≈ E_GABA. Based on the relation of E_Cl to resting membrane potential, we characterized GABAergic synapses as either: (1) depolarizing, when E_Cl was more positive than the resting membrane potential (Figure 1 A); or (2) hyperpolarizing, when E_Cl was more negative than the resting membrane potential (Figure 1 B). Depolarizing GABAergic synapses had an average E_Cl of −58.33 ± 2.63 mV, which was significantly different from the resting membrane potential of those neurons (−70.33 ± 1.17 mV; n = 12; paired t-test p < 0.001; Figure 1 C). In all cases E_Cl was hyperpolarizing with respect to action potential threshold, and thus depolarizing synapses were not excitatory. Hyperpolarizing synapses had an average E_Cl of −75.87 ± 1.74 mV, which was significantly different from their resting membrane potential values (−63.40 ± 2.44 mV; n = 10; paired t-test p < 0.001; Figure 1 C). There was a significant difference between the E_Cl values (p < 0.001) and resting membrane potential values (p = 0.014) of depolarizing and hyperpolarizing synapses. The slope of each I–V curve provided the GABA_A conductance of that synapse. Depolarizing GABAergic synapses had a conductance of 1.85 ± 0.34 pS (n = 12), and hyperpolarizing synapses had a conductance of 1.74 ± 0.35 pS (n = 10); there was no significant difference between the conductances of the two populations (p = 0.824).

FIGURE 1

Figure 1. Characterization of GABAergic synapses. (A) Example of an I–V curve from a depolarizing GABAergic synapse. The postsynaptic membrane potential was stepped in 10 mV increments while stimulating GABAergic synapses to generate the I–V curve. The holding potential at which the GPSC amplitude was 0 mV (dashed line) was taken as E_Cl. Inset: sample traces of GPSCs recorded during the construction of the I–V curve. Legend: 20 ms, 45 mV. (B) Example of an I–V curve from a hyperpolarizing GABAergic synapse. Characterized as in (A). Legend: 20 ms, 45 mV. (C) The average ± SEM for E_Cl and resting membrane potential (RMP) at depolarizing and hyperpolarizing synapses. *indicates statistical significance.

Simultaneous STDP Induction and Imaging of Ca²⁺ Dynamics

Following characterization of the GABAergic synapse we examined the Ca²⁺ dynamics during the induction of STDP. To do this, we loaded neurons with the Ca²⁺-sensitive cell permeant fluorescent dye Fluo4-AM (Figures 2 A,B). A sequence of fluorescence images was then acquired at 1–2 Hz during STDP induction. GABAergic STDP was induced in current-clamp mode; both the pre- and postsynaptic neurons were induced to fire action potentials (using minimal stimulation) at a frequency of 5 Hz for 30 s. The interval between spike induction was ±5 ms, which resulted in a spike-timing interval of ±1 ms between onset of the GPSP and the postsynaptic action potential. This yielded a graph representing the changes in Fluo4 fluorescence (as a measure of Ca²⁺) over time (Figure 2 C). This data was normalized to the baseline fluorescence level and expressed as a percentage increase. We analyzed three measures of the change in fluorescence during STDP induction: (1) ΔF₃₀ (%), the change in fluorescence from F₀ to F₃₀; (2) ΔF_peak (%), the change in fluorescence from F₀ to F_peak; and (3) F_area, the area under the curve normalized to F₀. Increasing the image acquisition frequency to 100–200 ms intervals did not significantly change the ΔF_peak for depolarizing GABAergic synapses (p = 0.898), indicating that the standard acquisition rate was sufficient to resolve the peak of the Ca²⁺ fluorescence. We chose to exclusively examine the Ca²⁺ influx at the soma of the postsynaptic neurons for two reasons. First, the majority of GABAergic neurons innervate the proximal dendrites and soma of postsynaptic neurons (Cobb et al., 1995 ; Freund and Buzsaki, 1996 ; Di Cristo et al., 2004 ; Huang, 2006 ). Second, we recently demonstrated that GABAergic STDP is induced by feed-forward interneurons which target the soma of pyramidal neurons in the CA1 region of the hippocampus (Ormond and Woodin, 2009 ).

FIGURE 2

Figure 2. Postsynaptic Ca²⁺ imaging during GABAergic STDP induction. (A) Bright field image of neurons during recording. The recording pipettes have been overlaid with black lines to clearly indicate the neurons being recorded. (B) Fluo4-AM fluorescence image of the same neurons as in (A), measuring changes in Ca²⁺ during STDP induction. Ca²⁺ was measured in the area of interest on the soma (circle). (C) Example graph of the increase in Fluo4 fluorescence during induction, which begins at F₀ with the onset of stimulation, peaks at F_peak, and ends at F₃₀ after 30 s of stimulation. The area of under the curve over this time period was used to calculate F_area, which normalizes the area to F₀. Left axis: arbitrary fluorescence units. Right axis: the same graph expressed as a percentage increase from baseline.

GPSC Polarity Determines the Magnitude of Ca²⁺ Influx During STDP Induction

Ca²⁺ influx is required for GABAergic STDP (Woodin et al., 2003 ), but whether or not the dynamics of the influx depend on the properties of the synapse had not yet been determined. After recording from a population of neurons that included both depolarizing and hyperpolarizing GPSCs and imaging their Ca²⁺ dynamics, we examined the relationship between GPSC amplitude and Ca²⁺ influx during STDP induction. GPSC amplitude correlated strongly with Ca²⁺ influx (F_area); the linear regression analysis yielded similarly high r-squared value regardless of the spike-timing order [pre/post r-squared = 0.66 (p = 0.002), post/pre r-squared = 0.65 (p = 0.003), all synapses r-squared = 0.65 (p < 0.001); Figure 3 A]. GPSC amplitude also correlated strongly with other measure of Ca²⁺ influx, ΔF₃₀ [pre/post r-squared = 0.65 (p = 0.002), post/pre r-squared = 0.60 (p = 0.005), all synapses r-squared = 0.62 (p < 0.001)] and ΔF_peak [pre/post r-squared = 0.62 (p = 0.004), post/pre r-squared = 0.63 (p = 0.004), all synapses r-squared = 0.62 (p < 0.001)]. Thus, regardless of the fluorescence measure examined, there was a strong relationship between Ca²⁺ influx and the nature of the GABAergic synapse; depolarizing synapses correlated with large increases in Ca²⁺, while hyperpolarizing synapses correlated with smaller increases.

FIGURE 3

Figure 3. GPSC amplitude affects postsynaptic Ca²⁺ dynamics during STDP induction. (A) GPSC amplitude strongly correlates with Ca²⁺ influx regardless of the order of spike-timing. (B) Depolarizing synapses result in a significantly larger Ca²⁺ influx during STDP induction than do hyperpolarizing synapses (p = 0.004). Hyperpolarizing synapses also result in a significantly lower Ca²⁺ influx than the firing of a neuron alone (post only; p = 0.045). (C) There was no significant difference in Ca²⁺ influx when STDP was induced in post/pre or pre/post orders at depolarizing (p = 0.96) and hyperpolarizing synapses (p = 0.77).

The correlation between Ca²⁺ influx and GPSC amplitude was further quantified by comparing the fluorescence increase during STDP induction between all depolarizing synapses (E_Cl = −58.33 ± 2.63 mV; n = 12), all hyperpolarizing synapses (E_Cl = −75.87 ± 1.74 mV; n = 10), and neurons with no synapses (which we call “post only”; n = 11). The post only neurons were also stimulated at 5 Hz for 30 s. There were significant differences between the Ca²⁺ influx at depolarizing and hyperpolarizing synapses regardless of the measure analyzed (F_area p = 0.004; F_peak p = 0.005; F₃₀ p = 0.004; Figure 3 B). Ca²⁺ influx at hyperpolarizing synapses were also significantly different from the influx at post only neurons that fired in the absence of a synapse when F_area and F₃₀ were analyzed (p = 0.04 and p = 0.048, respectively); however when F_peak was analyzed there was not a significant difference between hyperpolarizing synapses and post only neurons (p = 0.06). Thus, we can conclude that depolarizing neurons let in the same amount of Ca²⁺ during STDP induction as the postsynaptic neurons spiking alone (independent of a synapse). However, when the GPSC becomes hyperpolarizing it has a strong ability to decrease the Ca²⁺ influx.

At glutamatergic synapses the order of spiking (pre/post versus post/pre) during STDP induction determines the polarity of the plasticity (LTP versus LTD, respectively; Bi and Poo, 1998 ). However, at GABAergic synapses the order of spiking during induction does not determine the nature of plasticity (as evidenced by the symmetrical spike-timing window Woodin et al., 2003 ). We thus hypothesized that Ca²⁺ influx during STDP induction should be independent of the spike-timing order. We found no significant difference in Ca²⁺ influx (F_area) between synapses induced with positive or negative spike-timing intervals; this was true for both depolarizing (p = 0.96) and hyperpolarizing synapses (p = 0.77; Figure 3 C). We also found no significant difference between the time taken for the Ca²⁺ influx to reach its maximum between pre/post and post/pre synapses (p = 0.968).

GABAergic Synapse Properties Determine Ca²⁺ Dynamics During STDP Induction

The Ca²⁺ influx during STDP induction was affected by GPSC amplitude. GPSC amplitude is determined by both E_Cl and GABA_A conductance (Kaila, 1994 ); thus we asked which of these properties was the most influential in regulating postsynaptic Ca²⁺. We found that the linear regression of E_Cl versus Ca²⁺ influx (F_area) yielded low r-squared values [0.31 (p = 0.078) for pre/post synapses, 0.25 (p = 0.114) for post/pre synapses, and 0.26 (p = 0.015) for all synapses] (Figure 4 A). Low r-squared values indicate that the trend line does not accurately predict the relationship between E_Cl and Ca²⁺ influx. Thus, the difference between the slopes of the trend lines for pre/post and post/pre synapses does not necessarily indicate that the spike-timing order influences the Ca²⁺ influx. E_Cl also did not correlate strongly with ΔF₃₀ [pre/post r-squared = 0.26 (p = 0.114), post/pre r-squared = 0.27 (p = 0.104), all synapses r-squared = 0.26 (p = 0.017)] or ΔF_peak [pre/post r-squared = 0.29 (p = 0.086), post/pre r-squared = 0.25 (p = 0.119), all synapses r-squared = 0.26 (p = 0.016)].

FIGURE 4

Figure 4. E_Cl, driving force, and GABA_A conductance influence Ca²⁺ influx during STDP induction. (A) E_Cl does not correlate well with Ca²⁺ influx. Gray points and solid gray line represent pre/post synapses. Black points and solid black line indicate post/pre synapses. Dotted line indicates all synapses combined. (B) Driving force correlates better with Ca²⁺ influx. Gray points and solid gray line represent pre/post synapses. Black points and solid black line indicate post/pre synapses. Dotted line indicates all synapses combined. (C) GABA_A conductance also correlates well with Ca²⁺ influx. Gray points and solid gray line represent pre/post synapses. Black points and solid black line indicate post/pre synapses. Dotted line indicates all synapses combined.

Perhaps a more useful measure when considering the Cl⁻ gradient is the driving force for Cl⁻, which is the difference between the membrane potential and E_Cl. We found that the driving force correlated more strongly with Ca²⁺ influx (F_area) than did E_Cl alone, with r-squared values of 0.39 (p = 0.041) for pre/post synapses, 0.31 (p = 0.076) for post/pre synapses, and 0.34 (p = 0.004) for all synapses (Figure 4 B). Other measures of Ca²⁺ influx, ΔF₃₀ [pre/post r-squared = 0.42 (p = 0.032), post/pre r-squared = 0.33 (p = 0.063), all synapses r-squared = 0.37 (p = 0.003)] and ΔF_peak [pre/post r-squared = 0.35 (p = 0.055), post/pre r-squared = 0.33 (p = 0.066), all synapses r-squared = 0.33 (p = 0.005)], provided similar results as F_area.

GABA_A conductance was found to correlate with F_area to a higher degree than did E_Cl or driving force, with r-squared values of 0.57 (p = 0.007) for pre/post synapses, 0.68 (p = 0.002) for post/pre synapses, and 0.62 (p < 0.001) for all synapses (Figure 4 C). Conductance also correlated well with ΔF₃₀ [pre/post r-squared = 0.52 (p = 0.013), post/pre r-squared = 0.62 (p = 0.004), all synapses r-squared = 0.56 (p < 0.001)] and ΔF_peak [pre/post r-squared = 0.52 (p = 0.012), post/pre r-squared = 0.66 (p = 0.003, all synapses r-squared = 0.58(p < 0.001)].

Discussion

At GABAergic synapses, the induction of STDP requires an increase in postsynaptic Ca²⁺ (Woodin et al., 2003 ; Xu et al., 2008 ; Ormond and Woodin, 2009 ). Depending on the stage of nervous system development GABAergic synapses can be either depolarizing or hyperpolarizing, which led us to hypothesize that the nature of GABAergic transmission regulates the magnitude of the Ca²⁺ influx. Our present results found this hypothesis to be true; depolarizing GABAergic synapses characteristic of immature neuronal circuits produced larger Ca²⁺ influxes during STDP induction than hyperpolarizing GABAergic synapses, which are more commonly found in the mature central nervous system. Our analysis further revealed that this relationship between GABAergic synapses and Ca²⁺ influx can be accounted for by the two main properties of GABAergic synapses (the driving force for Cl⁻ and the GABA_A receptor conductance) but did not depend on the order of spike timing.

It is already well known that synaptic transmission contributes to the postsynaptic Ca²⁺ influx during glutamatergic STDP induction (Markram et al., 1997 ; Bi and Poo, 1998 , 2001 ; Debanne et al., 1998 ; Zhang et al., 1998 ). At these excitatory synapses, Ca²⁺ influx occurs primarily via VGCCs opened by the back-propagating action potential, and via NMDARs opened by the coincident occurrence of the back-propagating action potential and postsynaptic glutamate binding. How can our understanding of the Ca²⁺ influx during glutamatergic STDP induction be related to GABAergic STDP? It depends on the polarity of the GABAergic synapse. When E_Cl sits below the resting membrane potential the GPSC will hyperpolarize the postsynaptic membrane during STDP induction, resulting in a smaller Ca²⁺ influx than if that same postsynaptic neuron was spiking alone (at 5 Hz for 30 s, in the absence of synaptic transmission). This smaller Ca²⁺ influx presumably results from hyperpolarizing GPSCs decreases the opening of VGCCs (which are activated by action potential firing during STDP induction). However, at depolarizing GABAergic synapses, the Ca²⁺ influx during STDP induction for both positive and negative spike-timing intervals does not differ significantly from when the postsynaptic neuron spikes alone. This indicates that the additional depolarization is insufficient to open more VGCCs, either because the majority of available VGCCs have already been opened by the action potential, or because the magnitude of depolarization is not sufficient to open VGCCs.

We already know that the required Ca²⁺ influx during GABAergic STDP occurs partly through L-type VGCCs (Woodin et al., 2003 ; Ormond and Woodin, 2009 ). However, this cannot be the only source of Ca²⁺ influx because when GABAergic synapses are blocked or absent (post only) the same spiking pattern which also opens VGCCs fails to induce plasticity. This indicates that there are either additional sources of Ca²⁺ influx required for STDP, or that a component of the GABAergic signaling combines with the L-type Ca²⁺ influx to induce plasticity. We have preliminary evidence for the involvement of T-type VGCCs during hyperpolarizing GABAergic STDP (Balena and Woodin, 2009 ); these channels require membrane hyperpolarization to be removed from their inactive state but also require subsequent membrane depolarization to become activated (Magee et al., 1995 ; Perez-Reyes and Lory, 2006 ). Thus during hyperpolarizing GABAergic transmission we believe that the Ca²⁺ influx occurs both through L-type VGCCs (which have a reduced opening compared to post only) and through T-type VGCCs.

The strength of GABAergic synapses depends upon both the conductance of the channel and on the driving force for ions flowing through the channel. Because we recorded in a HCO_3⁻-free medium, E_GABA ≈ E_Cl; thus the driving force through the GABA_A receptors was largely determined by E_Cl. We found that neither the channel conductance nor the Cl⁻ driving force alone could predict the relationship between GPSC amplitude and Ca²⁺ influx. This indicates that it is the combination of these properties of GABAergic transmission that is important in regulating Ca²⁺ influx during STDP induction.

At glutamatergic synapses, positive and negative spike-timing intervals lead to long-term potentiation and depression, respectively, resulting in an asymmetric spike-timing window (Markram et al., 1997 ; Bi and Poo, 1998 , 2001 ; Debanne et al., 1998 ; Zhang et al., 1998 ). In contrast, the spike-timing window for GABAergic synapses is symmetric, with coincident activity (within ±15 ms) resulting in decreased inhibition, independent of the spike- timing order (Woodin et al., 2003 ). This likely accounts for the non- significant differences in Ca²⁺-influx between positive and negative spike-timing intervals. However, the present study only examined spike-timing intervals of <5 ms; whether the results are similar for intervals >5 ms remains to be determined.

We identified a significant difference in the resting membrane potentials between depolarizing and hyperpolarizing synapses. This difference may result from our ability to identify GABAergic synapses where E_Cl sits close to the resting membrane potential; if E_Cl ≈ resting membrane potential there would be no driving force for Cl⁻ and thus we did not characterize a synapse electrophysiologically. This may have biased our selection of synapses for those with larger driving forces; depolarizing synapses would be more likely to be found onto neurons with relatively hyperpolarized resting membrane potentials, and hyperpolarizing synapses would be common onto neurons with relatively depolarized resting membrane potentials.

Following acute neuronal trauma (van den Pol et al., 1996 ; Toyoda et al., 2003 ), oxygen-glucose deprivation (Galeffi et al., 2004 ), and seizure activity (Galanopoulou, 2007 ), there is a depolarization of E_Cl which renders GABAergic transmission depolarizing (Fiumelli and Woodin, 2007 ; Kahle et al., 2008 ). Based on our present results, this switch in the polarity of GABAergic transmission increases the amount of Ca²⁺ influx during subsequent neuronal activity. In fact, the magnitude of the E_Cl depolarization following neuronal insults is so large it often renders GABAergic transmission excitatory (Kahle et al., 2008 ), which should produce even larger Ca²⁺ influxes than those observed in the present study. This may be particularly relevant given that the large Ca²⁺ influxes resulting from neuronal injury contribute to cell death (Bano and Nicotera, 2007 ).

Taken together, a model emerges where postsynaptic Ca²⁺ influx is required for STDP induction at GABAergic synapses, and where the magnitude of this influx is regulated by the GABAergic transmission itself. Further work will be need to elucidate both how the Ca²⁺ influx in turn regulates E_Cl, and how the Ca²⁺ influx is regulated when GABAergic and glutamatergic STDP are induced simultaneously.

Conflict of Interest Statement

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Acknowledgments

This work was supported by a Natural Sciences and Engineering Research Council of Canada (NSERC) Discover Grant to Melanie A Woodin, and a NSERC Fellowship to Trevor Balena.

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