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Research ArticleNew Research, Neuronal Excitability

Balancing Extrasynaptic Excitation and Synaptic Inhibition within Olfactory Bulb Glomeruli

David H. Gire, Joseph D. Zak, Jennifer N. Bourne, Noah B. Goodson and Nathan E. Schoppa
eNeuro 25 July 2019, 6 (4) ENEURO.0247-19.2019; DOI: https://doi.org/10.1523/ENEURO.0247-19.2019
David H. Gire
1Department of Physiology and Biophysics, University of Colorado School of Medicine, Aurora, CO 80045
2Neuroscience Graduate Program, University of Colorado School of Medicine, Aurora, CO 80045
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Joseph D. Zak
1Department of Physiology and Biophysics, University of Colorado School of Medicine, Aurora, CO 80045
2Neuroscience Graduate Program, University of Colorado School of Medicine, Aurora, CO 80045
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Jennifer N. Bourne
1Department of Physiology and Biophysics, University of Colorado School of Medicine, Aurora, CO 80045
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Noah B. Goodson
2Neuroscience Graduate Program, University of Colorado School of Medicine, Aurora, CO 80045
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Nathan E. Schoppa
1Department of Physiology and Biophysics, University of Colorado School of Medicine, Aurora, CO 80045
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  • Figure 1.
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    Figure 1.

    Tests of spillover hypothesis based on PG cell-MC pair recordings. A1, Simplified circuitry at a glomerulus: OSN axons contact eTCs (black lines), which in turn send glutamatergic extrasynaptic signals to MCs (gray arrow). eTCs and MCs can excite GABAergic PG cells at dendrodendritic synapses, which feedback inhibition onto these cells (red lines). The OSN-to-eTC-to-MC feedforward pathway occurs in parallel with the direct OSN-to-MC pathway (left). A2, The spillover hypothesis: glutamate released at an eTC-to-PG cell synapse activates extrasynaptic receptors on nearby MC apical dendrites. B, Example whole-cell current recordings in a same-glomerulus PG cell-MC pair (Vhold = –77 mV in both cells) used to test the spillover hypothesis. Shown are currents evoked by OSN stimulation (40 µA) in a single response-trial (B1; PG cell in red, MC in blue), a fluorescent image of the pair (B2; glomerulus demarcated by dashed oval), five superimposed trials for the PG cell on a less expanded scale (B3), detected rapid EPSCs in the PG cell and time-locked MC currents (B4; expanded and normalized in inset), and a plot showing the correlation between individual PG cell and MC current events (B5; correlation coefficient = 0.43, p = 0.0010). Boxed region in B1 shows two examples of current deflections in the MC that were time-locked to rapid EPSCs in the PG cell. Open arrowheads in B3 point to bursts of EPSCs in the PG cell that delineate the cell as the subtype that receives direct input from eTCs (Shao et al., 2009). C, Summary of correlation coefficients obtained across all PG cell-MC pair recordings, plotted as a function of the mean MC current in the same experiment (r = 0.78, p = 0.008). Plot combines data from our standard recordings (n = 7; black circles) as well as three recordings in TTx (see D, gray circles). D, Spontaneous currents in a PG cell-MC pair recorded in TTx (1 µM), consistent with spillover at single release sites. The bottom trace at right reflects the average of shuffled events collected from the MC. Averages reflect 22 events.

  • Figure 2.
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    Figure 2.

    Spillover-mediated currents are due to glutamate release from eTCs. A, Recording from an eTC-MC pair showing MC currents (blue; at Vhold = –77 mV) evoked by single eTC spikes (black; in LCA mode). Raw traces (left) and averages (n = 94) are shown. Note the amplitude and kinetic similarities to MC currents recorded in the PG cell-MC pairs (Fig. 1B4). B, Comparison of the magnitude (B1) and kinetic properties (B2; 20%-to-80% rise-time and half-width) of MC currents recorded in eTC-MC pairs (n = 9) versus PG cell-MC pairs (n = 8 for B1, n = 7 for B2). Lines in B1 reflect mean ± SEM. Integrated charge values were multiplied by –1. C, Current events collected from a triple-cell recording that included a same-glomerulus eTC, PG cell, and MC. In the expanded and normalized average traces (boxed inset), it is clear that the PG cell and MC currents both had 1- to 2-ms onset delays after the eTC spike, indicating that the eTC was the source of the currents.

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    Figure 3.

    Ultrastructural evidence for complexes that could support spillover. A, Electron micrographs (A1, A2; two images are four 50-nm sections apart) and three-dimensional reconstruction (A3) of an example complex that includes a DAB-labeled eTC dendrite (darkened in micrographs; light yellow in reconstruction) forming a synapse (green) onto a putative PG cell dendrite (blue). A glutamatergic dendrite that was assigned to be a putative MC (red; see main text) and glial processes (purple) are in close proximity. Note that the glial processes in the reconstruction appear to surround the dendrites. Inset in A1, Same image as in A1 but without the colors so that the synapse (green arrow) can be seen more clearly. Scale bars: 0.5 μm for micrographs, 0.1 μm for inset of A1. Scale cube in A3 = 0.5 µm3. B, Another example of a complex containing an eTC-to-PG cell synapse with adjacent glial process and putative MC dendrite. Note that in the reconstruction the putative MC dendrite runs behind the PG cell and eTC dendrites. Scale bars and cube as in A. C, Electron micrograph (C1) and reconstruction (C2) of a cluster of synapses (in red) from OSNs (green) onto a DAB-labeled eTC dendrite (light yellow in reconstruction). Note the absence of an adjacent putative MC dendrite. Inset in C1, Original image of the eTC dendrite showing one of the OSN synapses (red arrow) that is indicated by the white dashed box. Scale bars and cube as in A. D, Summary of analysis of 13 eTC-to-PG cell synapses and 39 OSN-to-eTC synapses (pooled results from analysis of two eTC fills in two bulb slices). The fraction out of the total with an adjacent putative MC dendrite (within 0.5 µm) was much higher for eTC-to-PG cell synapses.

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    Figure 4.

    Absence of spillover at glutamatergic axonal synapses in glomeruli. A, Model to be tested: glutamate released at axonal synapses onto eTC dendrites spills over and activates glutamate receptors on adjacent MC dendrites. B, Example whole-cell recording from an eTC-MC pair at the same glomerulus used to test for spillover at axonal synapses. Raw traces recorded without a stimulus (B1), an image of the pair (B2; collapsed in the z-axis), and examples and averages (n = 293) of detected sEPSCs in the eTC and time-locked MC currents (B3) are illustrated. The cell body of the eTC in this pair was just above the glomerulus to which the MC sent its apical dendrite. C, Plot relating the magnitude of the sEPSCs and associated MC currents for the experiment in B. Line reflects linear regression fit of the data (r = –0.012, p = 0.82). D, Summary of MC currents recorded in eTC-MC pairs (open squares) versus PG cell-MC pairs (filled circles), plotted as a function of the amplitude of the fast EPSC in the reference cell (either eTC or PG cell). Data were binned according to the magnitude of the fast EPSCs in 100-pA/ms increments. Note that, while the MC current in the PG cell-MC pairs clearly increased as a function of the magnitude of the PG cell EPSC (linear regression fit: r = 0.79, p = 5.6 × 10−5), no such relationship was observed in the eTC-MC pairs (r = 0.28, p = 0.31). The eTC-MC pair dataset includes four to five points each in the bins centered at 50, 150, and 250 pA. Each point in each bin reflects a single experiment; *p = 0.01 in Mann–Whitney U test comparing the MC current in the two cell-pair types. E, Electrophysiological evidence that the eTC and MC in B were affiliated with the same glomerulus. E1, Two response trials overlaid showing that OSN stimulation (38 µA; at arrow) evoked LLDs in both cells in trial 2, but not trial 1. E2, Summary plot of responses to OSN stimulation for the same experiment (49 trials) relating the magnitude of the delayed current in the two cells. Note the clustering of data points in the upper right, corresponding to cooccurring LLD events. Current magnitude measurements were obtained by integrating the current starting 50 ms after OSN stimulation to avoid the OSN-EPSC. Line reflects linear regression fit (r = 0.98, p < 1.0 × 10−6).

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    Figure 5.

    Supralinear increase in extrasynaptic excitatory currents. A, Example whole-cell recordings from an eTC-MC pair illustrating MC current responses to different numbers of action potentials (APs) in the eTC. eTC spikes were evoked by direct depolarizing current pulses (500 pA, 25 ms). Note in the raw traces (A1; three superimposed trials) and averages (A2) that the total current associated with Iextra for more than or equal to two eTC spikes was much larger than linear summation of the current driven by one AP. In one of the trials in which the eTC spiked seven times in the same experiment (A3), the MC response included a distinct, much larger LLD event ∼150 ms after the onset of Iextra (note scale bar). B, Another eTC-MC pair recording in which the number of spikes in the eTC recorded in the LCA mode (B1; raw example trace) was related to Iextra in the MC (B2; averages). C, Summary of Iextra measurements from 12 pair recordings versus number of spikes in the eTC (N). Values, which reflect experiments in which the eTCs were in whole-cell (open squares) or LCA (open circles) patch modes, were normalized to the charge elicited by one eTC spike in the same pair. Note that nearly all points lie above the dashed line, which reflects linear summation of Iextra elicited by one eTC spike. Most pair recordings contributed multiple data points to the plot. D, Supralinearity indices SN measured across 12 pair-cell recordings separated by recording type for the eTC. A single value is plotted for each pair-cell recording, reflecting the average Iextra measured whenever the eTC fired at least two spikes (N ≥ 2). Asterisks: p ≤ 0.041 in comparison to SN≥2 = 1 (linear), paired t tests. Lines reflect mean ± SEM for each recording type. E1, Supralinearity indices SN (mean ± SEM) sorted by the number of spikes in the eTC. Each data point reflects 8–10 recordings obtained when the eTC was in either whole-cell or LCA patch mode. Superimposed line reflects fit of the individual SN values across all experiments, which yielded a significant correlation coefficient (0.37, p = 0.031). E2, Similar to part E1, except that values for the supralinearity indices were adjusted (yielding SN’) for the relative amount of glutamate released across different numbers of eTC spikes. Glutamate release was estimated from EPSCs recorded in eTC-PG cell pairs (Fig. 6); x-axis values reflect estimates of the amount of glutamate release following two, three, four, or five to seven eTC spikes, normalized to the single spike-evoked release in the same recording.

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    Figure 6.

    Sublinear increase in PG cell excitatory currents in eTC-PG cell pairs. A, Example recordings in an eTC-PG cell pair showing that spontaneous bursts of spikes in the eTC (recorded in LCA mode) were associated with strongly depressing rapid EPSCs in the PG cell. Three selected examples with varying number of eTC spikes are illustrated in A1. Analysis of 37 such bursts in this pair indicated that the degree of synaptic depression as reflected in the amplitude ratio of the first two EPSCs in the burst (Amp2/Amp1) was negatively correlated with the first EPSC amplitude (r = –0.63, p < 0.0001; A2) and positively correlated with the interval between the first two EPSCs (r = 0.44, p = 0.0058; A3). Both are consistent with a presynaptic vesicle depletion mechanism for depression. B, Summary of integrated current measurements from 10 eTC-PG cell pair recordings, demonstrating that the synaptic depression resulted in a sublinear increase in the excitatory current as a function of spike number in the eTC. Diagonal line reflects linearity. C, Example PG cell recording showing that the AMPA receptor allosteric modulator CTZ (100 µM) prolonged the EPSCs without altering the degree of depression. Selected EPSC bursts under each condition are illustrated in C1, while EPSC half-widths (C2) and amplitude ratios (Amp2/Amp1; C3) for the same experiment are also shown. The absence of an effect of CTZ on depression supported a presynaptic mechanism. D, Histograms summarizing CTZ effects on EPSC half-width (top) and the Amp2/Amp1 ratio (bottom) from five PG cell recordings; *p = 0.020 in paired t test. E, Estimates of the magnitude of slow currents in PG cells not directly associated with rapid EPSCs. PG cell currents, both under control conditions and in CTZ, were measured in a 100- to 200-ms window after the start of each eTC spike burst for bursts with more than or equal to four spikes lasting <100 ms. MC currents (reflecting Iextra) measured in the same manner are also plotted; n = 5 for each recording type; *p < 0.01 in paired t test comparison with zero current. F, Summary of absolute charge measurements as a function of eTC spike number for Iextra in MCs in the eTC-MC pairs (blue) and the PG cell current in the eTC-PG cell pairs (red). Each data point reflects mean ± SEM from 7–10 recordings; *p < 0.01 in Mann–Whitney U test, Bonferroni correction for multiple comparisons.

  • Figure 7.
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    Figure 7.

    Tests of different mechanisms that could underlie the supralinear increase in extrasynaptic excitatory currents. A, Example eTC-MC pair recordings showing effects of the glial glutamate transporter blocker DL-TBOA (50 µM) on Iextra. Note that DL-TBOA enhanced Iextra when the eTC fired five spikes (left; averages of 12–15 bursts), but not when the eTC spiked only once (right; averages of 60). An increase that is selective for the multi-spike condition is inconsistent with glutamate transporter saturation being the cause of the supralinear increase in Iextra (see main text). B, Summary of the effect of DL-TBOA on Iextra separated by when the eTC spiked once (n = 5 pairs) versus two or more times (n = 6); *p = 0.0012 in unpaired t test comparing more than or equal to two- and one-spike datasets. Lines reflect mean ± SEM for the two conditions. C, Example recording of Iextra in MCs (averages of 12–15 trials) induced by eTC spike bursts (five spikes/burst) showing that the current was mostly blocked by the AMPA and NMDA receptor blockers, NBQX (10 µM) plus DL-AP5 (50 µM). This argued against the supralinear increase in Iextra being due to recruitment of a neurotransmitter other than glutamate. D, Effect of NQBX plus DL-AP5 as a function of the magnitude of Iextra elicited by more than or equal to two eTC spikes. Superimposed fitted line indicates lack of correlation (p = 0.25), providing further evidence against the largest Iextra signals being due to a non-glutamate neurotransmitter. Each of the eight data points reflects one eTC-MC pair recording. E, Test for recurrent excitation and asynchronous glutamate release. E1, Example analysis of a single burst event in an eTC-PG cell pair in the no-LLD condition. Note that each eTC spike had a single time-locked EPSC reflecting monosynaptic transmission, also evident in the derivative trace at bottom (horizontal dashed line = threshold). The absence of excess events argued against recurrent excitation or asynchronous glutamate release being the cause of the supralinear increase in Iextra. Box demarcates a burst event in the same recording in which there was a cooccurring LLD; in this example we counted 12 excess EPSCs in the PG cell. E2, Histogram reflecting latencies between eTC spikes and PG cell EPSCs in the no LLD-condition for the experiment in E1. Latencies of 0.5–3.5 ms (open bars) were considered to reflect monosynaptic transmission from the test eTC onto the PG cell. F, Distribution of the number of excess PG cell EPSCs per burst across five eTC-PG cell pair recordings under the no LLD-condition. Note that the large majority of burst events had no excess PG cell EPSCs.

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    Figure 8.

    Extrasynaptic excitation and synaptic inhibition in eTCs following OSN stimulation. A, Simplified circuit reflecting currents measured in a voltage-clamped eTC following stimulation of OSNs. Components include the monosynaptic OSN-EPSC, Iextra due to activation of other eTCs (OSN-to-eTC-to-eTC), and a polysynaptic inhibitory current (IGABA) due mainly to feedback inhibition from PG cells (OSN-to-eTC-to-PG cell-to-eTC). Not shown is a potential feedforward pathway of inhibition mediated by ∼30% of PG cells directly excited by OSNs (Shao et al., 2009). B, Example eTC current responses. B1, Overlaid trials (three each) of excitatory currents (at Vhold = –77 mV) and inhibitory currents (at Vhold = +28 mV) evoked by OSN stimulation at three intensities (2, 3, and 4 µA). The 3-µA data in boxed region best illustrate the current components defined in A. Note that at the lowest intensity (2 µA), inhibition was much larger than excitation and the OSN-EPSC was barely detectable. B2, Iextra (right) was isolated by fitting the rise and most of the decay of the OSN-EPSC in the composite current (left) with a sum of two exponentials, then subtracting the derived estimate of the OSN-EPSC. Average currents (five trials) at two stimulus intensities are illustrated. B3, Integrated extrasynaptic (Gextra) and GABAergic (GGABA) conductances as a function of OSN-EPSC amplitude for this experiment. Each point reflects mean of five trials. C, Example excitatory current in an eTC evoked by single spikes in another eTC (at arrow) in an eTC-eTC pair recording (average of 12 trials). D, Summary of Gextra and GGABA measurements across 21 eTC recordings, sorted by amplitude of the cooccurring OSN-EPSC. Solid lines reflect linear regression fits of data points (one per recording), constrained to pass through the origin, added here for illustrative purposes. Dashed lines reflect unity. E, Linear regression fits of OSN-EPSC amplitude versus Gextra/GGABA ratio measurements from 19 individual eTC recordings. Each eTC recording had at least three OSN stimulation intensities sampled (actual data points not shown). Note positive slopes in all but three experiments, indicating that the conductance ratios generally rose with increasing OSN input.

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Balancing Extrasynaptic Excitation and Synaptic Inhibition within Olfactory Bulb Glomeruli
David H. Gire, Joseph D. Zak, Jennifer N. Bourne, Noah B. Goodson, Nathan E. Schoppa
eNeuro 25 July 2019, 6 (4) ENEURO.0247-19.2019; DOI: 10.1523/ENEURO.0247-19.2019

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Balancing Extrasynaptic Excitation and Synaptic Inhibition within Olfactory Bulb Glomeruli
David H. Gire, Joseph D. Zak, Jennifer N. Bourne, Noah B. Goodson, Nathan E. Schoppa
eNeuro 25 July 2019, 6 (4) ENEURO.0247-19.2019; DOI: 10.1523/ENEURO.0247-19.2019
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Keywords

  • excitation inhibition balance
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