Broadening of Inhibitory Tuning Underlies Contrast-Dependent Sharpening of Orientation Selectivity in Mouse Visual Cortex (original) (raw)
Articles, Behavioral/Systems/Cognitive
Journal of Neuroscience 14 November 2012, 32 (46) 16466-16477; https://doi.org/10.1523/JNEUROSCI.3221-12.2012
Abstract
Orientation selectivity (OS) in the visual cortex has been found to be invariant to increases in stimulus contrast, a finding that cannot be accounted for by the original, purely excitatory Hubel and Wiesel model. This property of OS may be important for preserving the quality of perceived stimulus across a range of stimulus intensity. The synaptic mechanisms that can prevent a broadening of OS caused by contrast-dependent strengthening of excitatory inputs to cortical neurons remain unknown. Using in vivo loose-patch recordings, we found in excitatory neurons in layer 4 of mouse primary visual cortex (V1) that the spike response to the preferred orientation was elevated as contrast increased while that to the orthogonal orientation remained unchanged, resulting in an overall sharpening rather than a weakening of OS. Whole-cell voltage-clamp recordings further revealed that contrast increases resulted in a scaling up of excitatory conductance at all stimulus orientations. Inhibitory conductance was enhanced at a similar level as excitation for the preferred orientation, but at a significantly higher level for the orthogonal orientation. Modeling revealed that the resulting broadening of inhibitory tuning is critical for maintaining and sharpening OS at high contrast. Finally, two-photon imaging guided recordings from parvalbumin-positive (PV) inhibitory neurons revealed that the broadening of inhibition can be attributed to a contrast-dependent broadening of spike-response tuning of PV neurons. Together our results suggest that modulation of synaptic inhibition in the mouse V1 cortical circuit preserves the sharpness of response selectivity during changes of stimulus strength.
Introduction
Orientation selectivity (OS) in the visual cortex of several mammalian species has been found to be contrast invariant, as demonstrated by a constant tuning bandwidth in the face of increasing stimulus contrast (Movshon et al., 1978; Albrecht and Hamilton, 1982; Sclar and Freeman, 1982; Li and Creutzfeldt, 1984; Skottun et al., 1987; Alitto and Usrey, 2004; Niell and Stryker, 2008). Moreover, recent studies indicate that OS sometimes even exhibits a contrast-dependent sharpening (Alitto and Usrey, 2004; Johnson et al., 2008). These experimental observations contradict the prediction of a broadening of OS at high contrast by a purely feedforward excitatory circuit, caused by an increased drive from nonselective thalamocortical inputs (Hubel and Wiesel, 1962; Troyer et al., 1998; Ferster and Miller, 2000). Two mechanisms have been proposed to explain the contrast-dependent properties of OS. First, cortical inhibition among neurons with different orientation tuning or from untuned inhibitory neurons is used in theoretical network models to achieve contrast invariance (Somers et al., 1995; Troyer et al., 1998; Lauritzen and Miller, 2003). Second, evidence shows that the variability of visually evoked membrane potential responses from trial to trial and the dependence of this variability on contrast can account for contrast invariance (Anderson et al., 2000; Finn et al., 2007; Sadagopan and Ferster, 2012). According to the variability model, pure excitatory mechanisms explain contrast invariance. But this model does not rule out the possible role of inhibition. This is because the membrane potential response results from the integration of visually evoked excitatory and inhibitory conductances, and several intracellular recording studies demonstrate that there can be substantial temporal overlaps between these conductances (Borg-Graham et al., 1998; Liu et al., 2010; Tan et al., 2011; Li et al., 2012). In addition, there has been ample evidence from both extracellular and intracellular studies suggesting that cortical inhibition may play a role in sharpening OS (De Valois et al., 1982; Celebrini et al., 1993; Monier et al., 2003; Ringach et al., 2003; Mariño et al., 2005; Xing et al., 2011). To address whether and how cortical inhibition contributes to maintaining sharp OS in the face of increasing contrast, it is essential to elucidate the inhibitory response tuning at different contrasts, and the responses of inhibitory neurons themselves to different contrasts as a function of orientation. Such studies are still lacking.
Thanks to the availability of recording techniques to dissect synaptic inputs and of genetic tools to target inhibitory neurons, the mouse has now become an important model to understand the mechanisms for visual processing (Taniguchi et al., 2011). Mouse visual cortical neurons can be as sharply tuned for orientation as cat cells (Niell and Stryker, 2008; Liu et al., 2009; Tan et al., 2011). Our previous study of mouse simple cells at a relatively high contrast indicates that their OS is significantly sharpened by very broadly tuned inhibition (Liu et al., 2011). Here we report that excitatory and parvalbumin-positive (PV) inhibitory neurons undergo contrast-dependent sharpening and broadening of OS respectively, and that a broadening of inhibitory synaptic tuning contributes critically to maintaining sharp OS at high contrast.
Materials and Methods
Animal preparation.
All experimental procedures used in this study were approved by the Animal Care and Use Committee of the University of Southern California. Adult female wild-type C57BL/6 mice (2–3 months) were used for voltage-clamp recordings and some loose-patch recordings. For visually guided recordings from layer 4, the layer 4-specific Cre mouse line, Scnn1a-Tg3-Cre (The Jackson Laboratory), was crossed with the Ai9 reporter line, which contains the DIO-tdTomato at ROSA26 locus (The Jackson Laboratory). For recordings from PV neurons, the mice with PV neurons expressing tdTomato were obtained by crossing the PV-ires-Cre driver line (The Jackson Laboratory) with the Ai9 reporter line. Mice were sedated with an intraperitoneal injection of chlorprothixene (5 mg/kg) and then anesthetized with urethane (0.5 g/kg, i.p., at 10% w/v in saline), as previously described (Niell and Stryker, 2008; Liu et al., 2009). The animal's body temperature was maintained at ∼37.5°C by a heating pad (Harvard Apparatus). A tracheotomy was performed, and a small glass capillary tube was inserted to maintain a free airway. CSF draining was performed. The part of the skull and dura mater (∼1 × 1 mm) over the primary visual cortex (V1) was removed. An artificial CSF solution [ACSF, containing (in mm): 140 NaCl, 2.5 KCl, 2.5 CaCl2, 1.3 MgSO4, 1.0 NaH2PO4, 20 HEPES, 11 glucose, pH 7.4] was applied to the exposed cortical surface when necessary. The eyes were covered with ophthalmic lubricant ointment until recording, at which time the eyes were rinsed with saline and a thin layer of silicone oil (30,000 centistokes) was applied to prevent drying while allowing clear optical transmission. Eye movements and the receptive field drift of single units were negligible within the time window of our recordings (Mangini and Pearlman, 1980; Liu et al., 2010).
In vivo electrophysiology.
The pia was prepenetrated with a broken pipette under visual guidance before recording experiments. Whole-cell voltage-clamp recordings were performed with an Axopatch 200B (Molecular Devices). The patch pipette had a tip opening of ∼2 μm (4.5–6 MΩ impedance). The Cs+-based intrapipette solution used for voltage-clamp recordings contained the following (in mm): 125 Cs-gluconate, 5 TEA-Cl, 4 MgATP, 0.3 GTP, 8 phosphocreatine, 10 HEPES, 10 EGTA, 2 CsCl, 1 QX-314, 0.75 MK-801, pH 7.25. The K+-based intrapipette solution used for current-clamp recordings contained the following (in mm): 130 K-gluconate, 2 KCl, 1 CaCl2, 4 MgATP, 0.3 GTP, 8 phosphocreatine, 10 HEPES, 11 EGTA, pH 7.25. The pipette capacitance and whole-cell capacitance were compensated completely, and series resistance (25–50 MΩ) was compensated by 50–60% (100 μs lag). A 12 mV junction potential was corrected. Signals were filtered at 2 kHz for the voltage-clamp recording and 5 kHz for the current-clamp recording, and sampled at 10 kHz. The evoked excitatory and inhibitory currents were resolved by clamping the cell at −70 and 0 mV, respectively. As discussed previously (Liu et al., 2010), our whole-cell recording method highly biases sampling toward pyramidal neurons. For cell-attached recordings, glass electrodes containing ACSF were used. A 100–250 MΩ seal was formed on the targeted neuron. The pipette capacitance was completely compensated. Spikes were recorded in the voltage-clamp mode, with a command potential applied to achieve a zero baseline current. The spike signal was filtered at 10 kHz and sampled at 20 kHz. The blindly recorded neurons assigned to layer 4 in this study had a cortical depth ranging from 375 to 520 μm, which was predicted from the travel distance of the pipette in the tissue. The layer assignment was reasonably precise for three reasons. First, the quantification of the layer 4 location using visual cortical slices of the layer 4-specific reporter mice, Scnn1a-Tg3-Cre tdTomato, demonstrated that the upper and lower boundaries of layer 4 were at 374 ± 14 μm and 510 ± 16 μm (mean ± SD, n = 3 brains, 15 locations) beneath the pial surface, respectively. This was confirmed by Nissl staining (data not shown). Second, the use of a high-magnification objective (40×) on our custom-built microscope enabled a precise identification of the cortical surface. In addition, the application of prepenetration greatly reduced the dimpling of the cortical surface in our experiments. Third, under two-photon imaging and with the use of a dye-filled pipette, we quantified the deviation of the predicted depth from the actual depth. At a depth of 350–465 μm, there was a small systematic error of predicted depths (14 ± 5 μm, mean ± SD, n = 10 brains). This systematic error was applied to correct the predicted depth. The identified excitatory neurons had a trough-to-peak interval of 0.89 ± 0.09 ms (mean ± SD, see Fig. 1A, inset) in their spike waveforms.
In vivo two-photon imaging guided recording.
Two-photon imaging was performed with a custom-built imaging system as previously described (Liu et al., 2009). A mode-locked Ti:sapphire laser (MaiTai Broadband, Spectra-Physics) was tuned at 890 nm with the output power at 60–300 mW for imaging fluorescently labeled neurons in layer 4, adjusted according to the cell's fluorescence level. The glass electrode, with ∼1 μm tip opening and 8–10 MΩ impedance, was filled with ACSF containing 0.15 mm calcein (Invitrogen). The pipette capacitance was completely compensated. The pipette tip was navigated in the cortex and patched onto a fluorescent soma as previously described (Liu et al., 2009). After confirming a successful targeting, the positive pressure in the pipette (∼10 mbar) was then released and a negative pressure (20–150 mbar) was applied to form a loose seal (with 80–200 MΩ resistance), which was maintained throughout the course of the recording. The depth of the patched cell could be directly determined under the two-photon microscope. The depth of the recorded PV neurons in this study ranged from 350 to 465 μm beneath the pia. The recorded PV neurons all exhibited narrow spike waveforms, with an average through-to-peak interval of 0.30 ± 0.04 ms.
Visual stimulation.
Stimuli were created using Matlab with Psychophysics Toolbox and displayed with a gamma-corrected LCD monitor (refresh rate, 75 Hz; maximum luminance, 280 cd/m2) placed 0.25 m away from the right eye. The center of the monitor was placed at 45° azimuth, 0° elevation, and it covered ±35° horizontally and ±27° vertically of the mouse visual field. Recordings were mostly made in the monocular zone of the V1. Spontaneous activity was recorded when a uniform gray background was applied. To measure orientation tuning, drifting sinusoidal gratings (2 Hz, 0.04 cycle/degree) of 12 directions (30° step) and different contrasts were applied in a random sequence. A stationary grating of one orientation was first presented on the full screen for 1.8 s before it drifted for 1.5 s (3 cycles). The grating stopped drifting for 500 ms before another grating pattern appeared. The 12 patterns were presented in a random sequence. Ten sets of stimuli were applied to each cell, with the sequence different between sets. The maximum contrast for the drifting gratings achieved by the monitor was ∼95% (near 100%).
Data analysis.
The data acquisition software was custom-developed with LabVIEW (National Instrument). Spikes evoked by drifting gratings were counted within a 70–1570 ms window after the start of drifting. The spontaneous firing rate was subtracted from the stimulus-evoked spike rate. The recorded synaptic responses were cycle-averaged, and then were smoothed by averaging within a 40 ms sliding window. The response levels for drifting sinusoidal gratings of two directions at the same orientation were averaged to obtain the orientation tuning curve between 0 and 180°, which was then fit with a Gaussian function R(θ) = A * exp(−0.5 * (θ − ϕ)2/σ2) + B, with ϕ the preferred orientation and σ the tuning width. The strength of orientation selectivity was quantified with a global measure of orientation selectivity index:
where θi is the angle of the moving direction of the grating and R(θi) is the response level at angle θi.
In voltage-clamp recordings, excitatory and inhibitory synaptic conductances were derived according to the following equation (Zhang et al., 2003; Tan et al., 2004; Liu et al., 2007; Wu et al., 2008): Δ_I_(t) = Ge(t)(V(t) − Ee) + Gi(t)(V(t) − Ei), where Δ_I(t)_ is the amplitude of synaptic current at a time point, Ge and Gi are the excitatory and inhibitory synaptic conductance respectively, V(t) is the membrane voltage, and _E_e (0 mV) and _E_i (−70 mV) are the reversal potentials. V(t) is corrected by V(t) = _V_h − _R_s * I(t), where _R_s was the effective series resistance and _V_h is the applied holding voltage.
The estimated membrane potential response based on the synaptic conductances was derived using a single-compartment neuron model (Somers et al., 1995; Troyer et al., 1998; Liu et al., 2010; Zhang et al., 2011):
where V_m(t_) is the membrane potential at time t, C the whole-cell capacitance, _G_r the resting leak conductance, and _E_r the resting membrane potential. C was measured during the experiment. _G_r and _E_r were calculated based on the baseline currents at two potentials.
Modeling.
The synaptic conductance evoked by a moving grating was simulated by fitting the average synaptic response waveform with a skew-normal function (Li et al., 2012), which yielded a better fit than sinusoidal functions or α functions (data not shown):
where φ and Φ are the standard normal probability density function and the cumulative distribution function respectively. ξ determines the location. The scale factor (ω) was set at 145 ms and the shape factor (α) at 1.5 for both excitatory and inhibitory conductances. To generate a relatively fast rising phase of the conductance change, the synaptic conductance was set as 0 if it was smaller than 10% of maximum. Because the phase difference between excitation and inhibition was 21 ± 15° (mean ± SD, n = 14), inhibition had a 25 ms delay relative to that of excitation (corresponding to a 18° phase difference). Varying the relative delay of inhibition from 5 to 50 ms did not qualitatively affect our conclusion (data not shown). To simulate responses to different orientations, while maintaining the temporal shape of the evoked conductance, the peak amplitude of the evoked conductance was varied according to the simulated tuning curve created based on the average synaptic tuning curve in our experimental data. The amplitudes of optimally evoked excitatory and inhibitory conductances were set based on the average experimental data (1.37 nS for excitation and 2.94 nS for inhibition at 25% contrast; 2.14 nS and 4.43 nS at near 100% contrast). The same conductance-based neuron model described earlier was used to simulate the membrane potential response generated by the integration of model synaptic conductances. _E_r was −65 mV. _E_e and _E_i were 0 mV and −75 mV, respectively. C was 20 pF. _G_r was calculated based on the equation _G_r = C * _G_m/_C_m, where _G_m, the specific membrane conductance, is 2e–5 S/cm2, and _C_m, the specific membrane capacitance, is 1e–6 F/cm2.
Results
Contrast-dependent sharpening of OS of excitatory neurons
To first understand contrast-dependent orientation tuning properties of mouse visual cortical neurons, we performed in vivo loose-patch recordings in the V1. Since contrast invariance is a prominent problem for layer 4 neurons receiving direct thalamic inputs (Ferster and Miller, 2000), we focused our study in layer 4. Taking advantage of a layer 4-specific Cre driver line, Scnn1a-Tg3-Cre (Madisen et al., 2010), we performed visually guided recordings from layer 4 neurons labeled by expressing a red fluorescence protein, tdTomato, under a two-photon microscope (see Materials and Methods). Spike responses of the patched neuron to drifting sinusoidal gratings of different contrasts ranging from 10% to near 100% were recorded, as shown by an example cell (Fig. 1A). The broad spike waveforms (Fig. 1A, inset) indicated that it was most likely an excitatory neuron (Liu et al., 2009). With contrast increasing, the spike response of the cell (as measured by the average spike rate within all stimulus cycles) to the preferred orientation increased drastically, while that to the orthogonal orientation did not (Fig. 1A,B). The tuning curve of evoked spike rate appeared sharper at 25% than at 10% contrast, as evidenced by the narrower tuning width. Higher than 25% contrast, the tuning width changed little. The plot of evoked spike rate at all testing contrasts shows that spike rate at the preferred orientation increased with increasing contrast, while that at the orthogonal orientation barely changed (Fig. 1C). The sharpness of tuning, as quantified with a global orientation selectivity index (gOSI, see Materials and Methods), was steadily increased from low to high contrast (Fig. 1D). Figure 1E shows the polar graph plots of responses of three example excitatory neurons recorded blindly in wild-type mice (see Materials and Methods). In general, they showed similar contrast-dependency as the cell in Figure 1A. The first two cells were sharply tuned. Their tuning sharpness was apparently stable between 25% and near 100% contrast. The third cell was only moderately tuned and had a higher response level compared with the first two. Nevertheless, its tuning shape was not dramatically changed by increasing contrast.
Figure 1.
Contrast-dependent changes of orientation selectivity of layer 4 excitatory neurons in mouse visual cortex. A, Spike responses of an example layer 4 neuron to drifting sinusoidal gratings of different contrasts (labeled on the top), recorded in a Scnn1a-Tg3-Cre tdTomato mouse. Each trace (1.5 s, 3 cycles) represents the poststimulus spike time histograms (PSTHs) from 10 trials for a particular stimulus. Calibration: 30 Hz, 100 ms. Blue arrows mark the preferred orientation. Bottom, Tuning curves of average spike rate within the three cycles. Bar, SD. Gaussian fits of the tuning curves are shown. Boxed inset, Top left, PSTH for spontaneous activity. Calibration: 3 Hz, 100 ms. Inset, Top right, Coronal section of the cortex showing specific labeling of neurons in layer 4 (left; scale bar, 200 μm), a two-photon image of the patched layer 4 cell (upper right; scale bar, 20 μm), and superimposed 50 individual spike waveforms of the cell (lower right). Note that the interval between the trough and the peak is relatively long (>0.5 ms). B, Superimposed fitted tuning curves at different contrasts. C, The average spike rates at the preferred and orthogonal orientations plotted against contrast for the same cell. D, gOSI plotted against contrast for the same cell. Black symbols, gOSI measured from average observed values. Gray symbols, Mean and SD of bootstrapped gOSIs (resamplings, 1000 times). E, Polar graph of evoked spike rate for another three example cells. The maximum axis value is labeled in the parentheses. The mean ± SD of bootstrapped gOSIs is shown for each cell. F, Average gOSI (normalized to the value at near 100% contrast) plotted against contrast. Left, gOSI based on spike rate within all cycles. Right, gOSI based on spike rate within the first cycle. Bar, SE; n = 15 cells. G, Average tuning width (normalized to value at near 100% contrast) plotted against contrast. *p < 0.05, paired t test, compared with near 100% contrast. H, Average evoked spike rate (normalized to the value of the preferred orientation at near 100% contrast) at the preferred and orthogonal orientations. Dash line, Contrast at which the increase in spike rate at the preferred orientation has reached half maximum. I, Percentage change in evoked spike rate (preferred and orthogonal orientation), gOSI, and tuning width from 25% to near 100% contrast. *p < 0.05; ***p < 0.001, paired t test. J, Plot of the mean of bootstrapped gOSIs at near 100% contrast versus that at 25% contrast for individual cells. Solid black, Cells that exhibit significant deviation from the identity line (bootstrap test, p < 0.01).
Data on layer 4 excitatory neurons either visually recorded in Scnn1a-Tg3-Cre mice (n = 5) or blindly recorded in wild-type mice (n = 10) were summarized (Fig. 1F,G). There appeared to be two phases for the change of gOSI: an initial phase in which gOSI increased quickly, and a later phase (>37.5% contrast) in which gOSI increased more slowly (Fig. 1F, left). The average tuning width was decreasing in the initial phase, whereas it was relatively stable in the second phase (Fig. 1G). Thus, overall, there is a sharpening of orientation tuning with increasing contrast. However, within a range of midcontrast to high contrast (37.5% to near 100%), the results are consistent with the notion of contrast invariance (i.e., tuning width being constant). There is a drastic difference in contrast-dependency between responses to the preferred and orthogonal orientations: the spike rate at the preferred orientation was elevated with increasing contrast with the half elevation point occurring at ∼30% contrast, whereas that at the orthogonal orientation was on average unchanged (Fig. 1H). Based on these results on spiking response, we chose to compare excitatory and inhibitory synaptic responses between contrast levels of 25% and near 100% in the later experiments. As summarized in Figure 1I, from 25% to near 100% contrast, the spike rate at the preferred orientation increased by 74 ± 18% (mean ± SD, p < 0.001, paired _t_ test), while that at the orthogonal orientation did not change significantly (−7 ± 15%, _p_ > 0.1, paired t test). This led to a 63 ± 18% increase in the value of gOSI (p < 0.001, paired t test). In the meantime, tuning width was slightly but significantly reduced (p < 0.05, paired t test). In the mouse visual cortex, a reduction in response over time (i.e., adaptation) was often observed (Tan et al., 2011; Li et al., 2012). To avoid potential confounds of changes of OS over time, we also analyzed the spike rate within the first cycle. As shown in Figure 1F (right), the analysis of the first cycle also revealed an increase in gOSI with increasing contrast. Furthermore, we performed bootstrap resamplings (1000 times) of evoked responses so as to overcome some random variation during one stimulus presentation (Efron and Tibshirani, 1993; Carandini et al., 1997). Figure 1J shows the mean of bootstrapped gOSIs at 25% and near 100% contrasts for individual cells. Sixty-seven percent of the cells exhibited a significant increase in gOSI at the high contrast (bootstrap, p < 0.01), while no cell exhibited a decrease in gOSI at the high contrast (Fig. 1J).
Contrast-dependent excitatory and inhibitory synaptic responses
To dissect visually evoked excitatory and inhibitory synaptic inputs, we performed whole-cell voltage-clamp recordings using a cesium-based internal solution (see Materials and Methods). As shown by two example cells (Fig. 2A,C,E,G), we recorded excitatory and inhibitory responses to gratings while clamping the cell's membrane potential at two different levels, −70 and 0 mV, respectively (Liu et al., 2010,2011). To quantify the strength of synaptic responses, we averaged response traces by trials and cycles, and then measured the peak amplitude after smoothing the response trace with a 40 ms sliding window for averaging. The values of this peak amplitude were used to plot the synaptic tuning curves (Fig. 2B,D,F,H). In both cells, excitatory and inhibitory responses at all orientations were strengthened with increasing contrast, so that the offsets of the synaptic tuning curves were elevated. While the excitatory response was similarly tuned (Fig. 2F) or became slightly more sharply tuned (Fig. 2B) at the high contrast, the inhibitory tuning on the other hand apparently broadened (Fig. 2D,H).
Figure 2.
Excitatory and inhibitory synaptic responses revealed by voltage-clamp recordings. A, Average traces of excitatory responses of an example cell at 25% and near 100% contrast. Red dash lines, Pretrigger baseline. B, Response tuning curve at 25% (top) and near 100% (middle) contrast for the same cell. Bottom, Normalized response tuning curve at 25% (dash) and near 100% (solid) contrast. C, D, Inhibitory responses and tuning curves for the same cell. E–H, Synaptic responses and tuning curves for another example cell. Data are presented in a similar manner. Calibrations: A, 100 pA; C, 200 pA; E, 50 pA; G, 150 pA; 200 ms.
We recorded excitatory responses from 26 neurons. In 14 of these cells, recording was maintained long enough so that inhibitory responses were also completely examined. The summarized results show that from 25% to near 100% contrast, excitation and inhibition were increased markedly by >50% (Fig. 3A). The relative increase of excitation was similar between the preferred and orthogonal responses, suggesting a nearly multiplicative change of excitatory input across orientations. The relative increase of inhibition at the preferred orientation was similar to that of excitation, but the relative increase of inhibition at the orthogonal orientation was much greater (Fig. 3A). Due to these unbalanced increases in excitation and inhibition, the E/I ratio at the orthogonal orientation was significantly decreased (Fig. 3B), along side a reduction of inhibitory tuning selectivity (Fig. 3C). Meanwhile, excitatory tuning selectivity tended to be slightly enhanced (Fig. 3C). A similar conclusion on a reduced inhibitory tuning selectivity could be made when the peak amplitude during the first cycle was measured (Fig. 3D,E,F), or when the average conductance was measured (for inhibition, gOSI was 0.11 ± 0.02 at 25% contrast, 0.05 ± 0.01 at near 100% contrast, mean ± SE, p < 0.01, paired _t_ test; for excitation, gOSI was 0.06 ± 0.03 at 25% contrast, 0.08 ± 0.03 at near 100% contrast, _p_ > 0.05). Nine of the 14 recorded cells exhibited a significant decrease in inhibitory tuning selectivity (Fig. 3G). As a result, at near 100% contrast inhibitory tuning selectivity was significantly lower than excitatory tuning selectivity in 9 of 14 cells (Fig. 3H, right). Despite the changes in synaptic strength and selectivity, there was no significant change in preferred orientation for either spike or excitatory response (Fig. 3I,J), nor in similarity between preferred orientations of excitation and inhibition (Fig. 3K).
Figure 3.
Contrast-dependent changes of synaptic inputs to excitatory neurons. A, Percentage change in response level at the preferred and orthogonal orientations, quantified by the peak amplitude of the cycle-averaged response waveform. Bar, SE; n = 14. **p < 0.01, ***p < 0.001, paired t test. B, E/I ratio for the two orientations at different contrasts. **p < 0.01, paired t test. C, gOSIs of excitation (red, n = 26) and inhibition (blue, n = 14) at 25% and near 100% contrast. Data points for the same cell are connected with a line. ***p < 0.001, paired t test. D–F, Summary results based on quantifications of the peak amplitude within the first stimulus cycle. Data are presented in the same way as in A–C. G, Plot of the mean of bootstrapped gOSIs at near 100% contrast versus that at 25% contrast for individual cells. For inhibition, dark blue indicates cells that exhibit significant deviation from the identity line (p < 0.01). H, Plot of the mean of bootstrapped gOSIs for inhibition versus that for excitation to the same cell. Left, At 25% contrast. Right, At near 100% contrast. Solid black, Cells that exhibit significant deviation from the identity line (p < 0.01). I, Preferred orientation of spike response at near 100% contrast versus that at 25%. J, Preferred orientation of excitation at near 100% contrast versus that at 25%. K, Preferred orientation of inhibition versus that of excitation.
An inhibitory synaptic mechanism underlying contrast-dependent sharpening of OS
Both an increase in excitatory selectivity and a decrease in inhibitory selectivity can lead to an elevation of gOSI of spiking response. Considering the magnitude of the respective change in excitatory and inhibitory tuning (Fig. 3C,F), it can be predicted that the reduced inhibitory tuning selectivity would play a major role. To confirm this point, we simulated contrast-dependent membrane potential responses with a conductance-based integrate-and-fire neuron model, using parameter values (e.g., synaptic strength and synaptic tuning profile) as observed in our experiments. We first averaged the normalized synaptic tuning curves of all the cells. Again, the summary shows that the average excitatory tuning curve barely changed at the high contrast, whereas the average inhibitory tuning curve significantly broadened (Fig. 4A). We simulated waveforms of visually evoked synaptic conductances (in 1 cycle) with a skew normal function (Fig. 4B, top), with the inhibitory response delayed relative to the excitatory response by 25 ms (see Materials and Methods). The membrane potential response was then derived by feeding the simulated synaptic conductances into the neuron model (Fig. 4B, bottom). To simulate synaptic tuning curves for the model, the average recorded synaptic tuning curves were fitted with Gaussian functions (Fig. 4C). For simplicity, the excitatory tuning curves at the low and high contrasts were chosen to be the same. As shown in Figure 4D, the tuning curve of the derived postsynaptic membrane potential response (PSP) was sharper when the synaptic amplitudes and tuning profiles at near 100% contrast (red) were used in the model, compared with those at 25% contrast (solid black). The sharper tuning was due to a much larger elevation of PSP response at the preferred than orthogonal orientation (Fig. 4D). This simulation result is largely consistent with our experimental observation that with contrast increases the spiking response was markedly increased at the preferred orientation but remained unchanged at the orthogonal (Fig. 1H). The sharpening of PSP response can be primarily attributed to the increased broadness of inhibitory tuning, because strengthening the excitatory and inhibitory inputs normally while artificially retaining the initial inhibitory tuning profile (as at 25% contrast) resulted in even weaker tuning of PSP response (Fig. 4D, dashed curve). This result in fact supports the prediction from our previous modeling work that a balanced increase of excitation and inhibition would result in a weakening of tuning selectivity of PSP response and that a broadening of inhibition might be required to counteract this effect (Liu et al., 2011).
Figure 4.
A broadening of inhibitory tuning primarily contributes to the contrast-dependent sharpening of OS. A, Average normalized excitatory and inhibitory tuning curves at the two different contrasts (25% and near 100%). Bar, SE; n = 14. B, Top, Simulated excitatory and inhibitory synaptic conductance waveforms (1 cycle). Bottom, Membrane potential response generated by the integrate-and-fire neuron model when the evoked synaptic conductances shown on top were integrated. C, Tuning profiles of excitation and inhibition at 25 and 100% contrast applied in our model. Ge, excitation. Gi, inhibition. D, Tuning curves of PSP generated by our model. Black, 25% contrast. Red, 100% contrast. Dash, 100% contrast but with the inhibitory tuning profile prevented from broadening (i.e., it is the same as the one at 25% contrast). The applied strength of synaptic conductance at different contrasts was according to the tuning curve shown in C. Right, Normalized PSP tuning curves. E, Left, Average subthreshold _V_m responses of an example cell recorded under the current-clamp mode. Spikes were removed by a 15 ms median filter before averaging. Each trace is 1.5 s. Right, Polar graphs of evoke spike rate and peak depolarization voltage. F, gOSI of peak _V_m response at 25% and near 100% contrast. Data points for the same cell are connected with a line. **p < 0.01, paired t test; n = 8. G, Left, Average peak _V_m responses at the preferred and orthogonal orientations from our current-clamp recording results. n = 8. Right, _V_m responses derived by feeding the experimentally determined excitatory and inhibitory conductances into the neuron model. White column represents the _V_m response generated when the inhibitory tuning was prevented from broadening (i.e., the recorded inhibitory responses at near 100% contrast are scaled according to the average inhibitory tuning curve at 25% contrast). *p < 0.05; **p < 0.01, paired t test. n = 14.
To further confirm that a sharpening of PSP response occurs due to the contrast-dependent broadening of inhibition, we performed current-clamp recordings from layer 4 excitatory neurons, using a K+-gluconate-based internal solution (see Materials and Methods). The subthreshold membrane potential (_V_m) response was obtained after removing spikes with a median filter (Fig. 4E, left). Although the _V_m response was much more weakly tuned than the spiking response (Fig. 4E, right), we did observe that the gOSI of _V_m response significantly increased from 25% to near 100% contrast (Fig. 4F). In the meantime, the elevation of _V_m response from 25% to near 100% contrast was larger at the preferred than at the orthogonal orientation (Fig. 4G, left). Considering that the subthreshold membrane depolarization can be clipped by the spike threshold, the elevation of _V_m response at the preferred orientation may even be underestimated. Thus, as expected from the modeling result, the _V_m response was indeed sharpened at the high contrast. Furthermore, using the same neuron model, we derived PSP responses from experimentally determined excitatory and inhibitory conductances (Fig. 4G, right). For the PSP derived in this manner, the response elevation from the low to high contrast at the orthogonal orientation was indeed much smaller than that at the preferred. However, it was markedly increased if we forced the inhibitory tuning not to become broadened by scaling the recorded inhibitory responses at near 100% contrast according to the average inhibitory tuning curve at 25% contrast (Fig. 4G, right, white column). Together, our simulation data strongly suggest that the contrast-dependent broadening of inhibition plays a critical role in maintaining sharp orientation tuning at high contrast.
Contrast-dependent broadening of OS of inhibitory neurons
How does the inhibitory tuning become broadened at high contrast? One possibility is that the spiking response tuning of individual inhibitory neurons becomes broadened. PV fast-spiking neurons constitute the largest inhibitory neuron population in layer 4 (Kawaguchi and Kubota, 1997; Gonchar et al., 2007; Xu et al., 2010), yet contrast-dependent tuning properties of these neurons have not been characterized. We thus recorded from PV neurons by two-photon imaging-guided loose-patch recordings in the PV-Cre tdTomato transgenic mice (see Materials and Methods), and in two cases by identifying fast-spiking neurons in blind recordings (Liu et al., 2009). We found that PV neurons exhibited very different behaviors from excitatory neurons. As shown by an example cell in Figure 5A, the cell displayed relatively well tuned spiking responses at 10% contrast. However, the response tuning became more and more flattened with increasing contrast. At near 100% contrast, its tuning selectivity was almost completely lost (Fig. 5B). Different from excitatory neurons, the response level at both the preferred and orthogonal orientations increased robustly (Fig. 5C), resulting in an almost zero gOSI at the highest contrast (Fig. 5D). A weakening of tuning selectivity was also evident from the polar graphs for another two example PV cells (Fig. 5E). Summarized results for 13 PV neurons show that their tuning selectivity was monotonically decreasing with increasing contrast (Fig. 5F). Their spike responses at the preferred and orthogonal orientations were both elevated, but not in the same rate (Fig. 5G). The relative increase of spike rate was much higher at the orthogonal orientation than at the preferred, resulting in significantly reduced tuning selectivity at near 100% contrast (Fig. 5H). For individual cells, bootstrap test revealed that 10 of 13 cells exhibited a significant reduction in gOSI at the high contrast (Fig. 5I). Finally, consistent with previous reports (Ma et al., 2010; Atallah et al., 2012), PV neurons had significantly higher spontaneous and evoked firing rates than excitatory neurons (Fig. 5J). Together, our results strongly suggest that PV inhibitory neurons are not contrast invariant. The broadening of orientation tuning of these neurons likely contributes to the broadening of synaptic inhibition to excitatory cells.
Figure 5.
Contrast-dependent broadening of spike response tuning of PV inhibitory neurons. A, Poststimulus spike time histograms (PSTHs) for spike responses of an example PV neuron in layer 4. Calibrations: 30 Hz, 100 ms. Boxed inset, Top left, PSTH for spontaneous activity. Calibrations: 3 Hz, 150 ms. Inset, Top right, Two-photon image of the PV neuron (red) patched by the glass electrode (green), and superimposed 50 individual spike waveforms of the cell. Note that the interval between the trough and the peak is much shorter compared with excitatory neurons. Calibration: 15 μm. B, Superimposed fitted tuning curves at different contrasts. C, Evoked spike rates at the preferred and orthogonal orientations plotted against contrast for the same cell. D, gOSI plotted against contrast for the same cell. Gray shows the mean ± SD of bootstrapped gOSIs (resamplings, 1000 times). E, Polar graphs of evoked spike rate for another two PV neurons. F, Average gOSI (normalized to the value at the lowest contrast) plotted against contrast. Inset, Average gOSI (absolute value) at different contrasts. Bar, SE; n = 13. G, Average evoked spike rates (normalized to the value of preferred orientation at near 100% contrast) at the preferred and orthogonal orientations. Inset, Ratio of spike rate at the orthogonal versus preferred orientation. H, Percentage change in evoked spike rate and gOSI value from 25% to near 100% contrast. I, Plot of the mean of bootstrapped gOSIs at near 100% contrast versus that at 25% contrast for individual cells. Solid black, Cells that exhibit significant deviation from the identity line (bootstrap test, p < 0.01). J, Average evoked (at near 100% contrast) and spontaneous spike rate for excitatory and PV neurons. *p < 0.05, **p < 0.01, t test.
Trial-to-trial variability of synaptic responses
Previous studies in the cat have suggested that contrast-dependent changes in trial-to-trial variability is sufficient for generating contrast invariance without reliance on inhibition (Finn et al., 2007; Priebe and Ferster, 2008). Here we looked into this issue and found that the trial-to-trial variability of membrane potential responses was indeed reduced at the high contrast for both the preferred and orthogonal orientations (Fig. 6A,B). At the synaptic level, we found that the variability of excitatory responses significantly decreased at the high contrast (Fig. 6C,D), consistent with the notion of a reduced variability of thalamic inputs (Sadagopan and Ferster, 2012). The variability of inhibitory responses also tended to decline, although the level of reduction did not reach statistical significance (Fig. 6C,D). Thus, the change in variability of excitatory responses directly contributes to that of membrane potential responses. In addition to broadened inhibition, the reduced response variability can also contribute to preventing elevations of the null response, since it is equivalent to elevating the spike threshold (Finn et al., 2007; Priebe and Ferster, 2008).
Figure 6.
Trial-to-trial variability of synaptic responses. A, Average traces of membrane potential responses of an example cell at the preferred (Pref) and orthogonal (Orth) orientations. Shading indicates SD, which was calculated within a 40 ms sliding window. Red dash line, Baseline. Calibrations: 10 mV, 200 ms. B, Trial-to-trial variance of membrane potential responses at 25% and near 100% contrast for the preferred and orthogonal orientations. n = 8 cells. **p < 0.01; ***p < 0.001, paired t test. C, Average traces of excitatory (Exc) and inhibitory (Inh) responses of an example cell at the preferred and orthogonal orientations and at both 25% and near 100% contrasts, with SD indicated by the shading. Calibrations: Exc, 30 pA; Inh, 82 pA, 200 ms. D, Summary of trial-to-trial variance of synaptic responses. The maximum SD for each orientation was selected for this quantification. n = 14 cells. **p < 0.05; **p < 0.01, paired t test.
Discussion
Contrast invariance versus contrast-dependent sharpening of OS
Contrast invariance is traditionally defined as a constant orientation tuning width in the face of contrast increases. Meanwhile, it has been reported for ferret and a subset of primate visual cortical neurons that a global measure of OS (e.g., circular variance) exhibits contrast-dependent changes, which indicate an increased selectivity level at high contrast (Alitto and Usrey, 2004; Johnson et al., 2008). Our data on excitatory neuron tuning measured with gOSI are consistent with the results in these species in that tuning selectivity is enhanced with increasing contrast. The data on tuning width are also consistent with a previous report in the mouse V1 showing that tuning width is not significantly changed from midcontrast to high contrast (50–100%) (Niell and Stryker, 2008). For a broader range of contrasts, our data show that orientation tuning width is in fact reduced with increasing contrast. This general trend of decreasing tuning width, however, does not contradict the notion of contrast invariance at a mechanistic level. Tuning width being unchanged or reduced, the task the cortical circuits need to achieve is the same: to keep selectivity sharp at high contrast. The details of contrast-dependent changes of orientation tuning may depend on different species, cortical layers, or cell types studied. Our results showing that the spike rate of excitatory neurons at the orthogonal orientation is not enhanced with increasing contrast highlights the essence of the problem the visual cortex is commonly facing: how to prevent an elevation of the null response while there is certainly a large increase of excitatory drive at the null orientation.
Inhibitory contribution to contrast-dependent sharpening of OS
In our previous study of OS in layer 2/3 simple cells, we found that inhibitory input is more broadly tuned than excitatory input (Liu et al., 2011; Atallah et al., 2012). Such broader inhibition can significantly sharpen the tuning of output response compared with cotuned inhibition (Liu et al., 2011). We also found in our initial modeling work that simply scaling up excitation and inhibition in proportion would not lead to invariant tuning but a broadening of output response (Liu et al., 2011). We have thus hypothesized that differential contrast-dependent modulations of excitatory and inhibitory tuning might be necessary for achieving contrast invariance.
In the current study, we have indeed observed that contrast changes modulate the two types of synaptic input in different manners. Excitatory responses evoked by different orientations are strengthened nearly multiplicatively, consistent with contrast-dependent increases in firing rate of thalamic neurons (Finn et al., 2007; Olsen et al., 2012). Inhibitory responses are also strengthened, but with a relatively greater level at the orthogonal orientation than at the preferred, resulting in a broadening of the inhibitory tuning. This can be attributed to a contrast-dependent broadening of spiking response tuning of individual inhibitory neurons, and additionally a potential increase in convergence of inhibitory neuron inputs, which remains to be investigated. Our modeling results indicate that the broadening of inhibition at high contrast largely limits the elevation of membrane potential response at the null orientation despite the greatly increased excitatory conductance. Otherwise, if inhibition is not broadened, the elevation of the null _V_m response would be similar to (or even greater than) that of the preferred response, leading to a reduced selectivity of output response (Fig. 4D, dash curve; Fig. 4G, white column). Thus, our data indicate that an inhibitory mechanism plays a critical role in preventing a significant elevation of the null response at high contrast.
Trial-to-trial variability of synaptic responses
Previous studies in the cat have shown that the trial-to-trial variability of membrane potential responses of simple cells is reduced with increasing contrast (Anderson et al., 2000). It can be attributed to a reduced variance of thalamic inputs, and is sufficient for accounting for the contrast invariance of simple cells (Finn et al., 2007; Priebe and Ferster, 2008; Sadagopan and Ferster, 2012). In the current study, we also observed a reduction of trial-to-trial variability of membrane potential responses, which can be directly attributed to a decrease in variability of excitatory responses. In addition, due to a saturating input–output transfer function as discussed in our previous study (Liu et al., 2011), an increase in excitatory conductance with a fixed variance would naturally result in a reduced variance of membrane potential response. Thus, two factors (increased excitatory conductance and increased variance of excitatory conductance) together can account for the reduced variability of membrane potential responses at high contrast. The observed changes in membrane potential response variability, however, cannot sufficiently explain the contrast-dependent changes in spike-response tuning in the current study. This is because, in the absence of inhibitory broadening, there would be a large increase in the null _V_m response (Fig. 4D,G). Reducing variability, which is equivalent to elevating the effective spike threshold, would be incapable of suppressing the null spike response while allowing a large increase in the preferred spike response, since it affects both responses at the same time. After the broadened inhibition largely limits the elevation of the null _V_m response, the reduction in variability can further contribute to suppressing the null spike response by elevating the spike threshold. This may explain why there is an increase in the null _V_m response at high contrast (Fig. 4G), whereas the null spike response is not changed (Fig. 1H). It should be noted that the level of inhibitory contribution to orientation selectivity may differ in different species.
Contrast-dependent broadening of orientation tuning of inhibitory neurons
An interesting observation in this study is that orientation tuning of PV inhibitory neurons becomes flattened as contrast increases. The largely untuned property of PV neurons at high contrast is consistent with observations from several previous studies that examined PV neurons at a fixed contrast (Kerlin et al., 2010; Ma et al., 2010; Hofer et al., 2011; Kuhlman et al., 2011; Zariwala et al., 2011; Atallah et al., 2012). In addition, the contrast-dependent changes of PV neuron tuning may provide an explanation for the discrepancy of PV neuron selectivity reported by different groups (e.g., Kerlin et al., 2010; Runyan et al., 2010), since different absolute contrasts may have been applied. Interestingly, the behavior of PV neurons in response to contrast increases (i.e., concurrent increases in firing rate at all orientations) is exactly what has been predicted for excitatory neurons by the original Hubel and Wiesel model, which did not take inhibition or variability into account (Ferster and Miller, 2000). In layer 4, PV neurons have been shown to receive thalamic input like excitatory neurons and to provide them with fast feedforward inhibition (Gibson et al., 1999; Gabernet et al., 2005; Cruikshank et al., 2007). Here, we propose that a simple thalamocortical circuit recruiting feedforward inhibition can explain both the contrast-dependent sharpening of excitatory neurons and the contrast-dependent broadening of PV inhibitory neurons (Fig. 7). In this circuit, PV neurons provide primary feedforward inhibition to the excitatory neuron of interest. The PV neurons and the excitatory neuron receive similar thalamic inputs, as evidenced by a similar preferred orientation between excitatory and inhibitory tuning across contrasts (Fig. 3K). With contrast increases, the thalamic inputs are strengthened, increasing excitatory drive onto both the PV neurons and the excitatory cell. As PV neurons receive relatively stronger thalamic input compared with excitatory cells (Gabernet et al., 2005; Cruikshank et al., 2010; Schiff and Reyes, 2012), the increase in excitatory drive onto PV neurons can easily lead to an elevation of their firing rate at all orientations due to the “iceberg” effect (Carandini and Ferster, 2000; Wehr and Zador, 2003; Zhang et al., 2003). The strengthened and broadened inhibitory input from PV neurons can then counteract the increased excitatory drive onto the excitatory cell, and maintain or even enhance the sharpness of orientation tuning of its output response. Such synaptic circuitry mechanism may also function in other sensory systems to achieve sharp tuning regardless of stimulus intensity.
Figure 7.
A simple model for contrast invariance of excitatory neurons and contrast variance of PV inhibitory neurons. The schematic orientation tuning curves of _V_m response for the PV neuron(s) and the excitatory (Ex) cell are shown. Gray, At a low contrast. Black, At a high contrast. Dotted gray line, Spike threshold. The PV neuron(s) exhibits a similar preferred orientation as the excitatory cell, since they receive a similar set of thalamic inputs.
Footnotes
- This work was supported by grants to H.W.T. from the United States National Institutes of Health (EY019049 and EY022478) and the Kirchgessner Foundation. We thank Dr. Kurt Zhang for his help on bootstrap analysis.
- Correspondence should be addressed to H.W. Tao,USC Keck School of Medicine, 1501 San Pablo Street, ZNI 439, Los Angeles, CA 90033. htao{at}usc.edu