Abstract
The behavioral state of a mammal impacts how the brain responds to visual stimuli as early as in the dorsolateral geniculate nucleus of the thalamus (dLGN), the primary relay of visual information to the cortex. A clear example of this is the markedly stronger response of dLGN neurons to higher temporal frequencies of the visual stimulus in alert as compared with quiescent animals. The dLGN receives strong feedback from the visual cortex, yet whether this feedback contributes to these state-dependent responses to visual stimuli is poorly understood. Here, we show that in male and female mice, silencing cortico-thalamic feedback profoundly reduces state-dependent differences in the response of dLGN neurons to visual stimuli. This holds true for dLGN responses to both temporal and spatial features of the visual stimulus. These results reveal that the state-dependent shift of the response to visual stimuli in an early stage of visual processing depends on cortico-thalamic feedback.
SIGNIFICANCE STATEMENT Brain state affects even the earliest stages of sensory processing. A clear example of this phenomenon is the change in thalamic responses to visual stimuli depending on whether the animal’s brain is in an alert or quiescent state. Despite the radical impact that brain state has on sensory processing, the underlying circuits are still poorly understood. Here, we show that both the temporal and spatial response properties of thalamic neurons to visual stimuli depend on the state of the animal and, crucially, that this state-dependent shift relies on the feedback projection from visual cortex to thalamus.
Introduction
While awake, animals shift between brain states: the alert state, when animals engage with sensorimotor behaviors, and a quiescent state (Steriade, 1997; O’Connor et al., 2002; Bezdudnaya et al., 2006; Hei et al., 2014). These shifts affect visual processing as early as the dorsolateral geniculate nucleus of the thalamus (dLGN). For example, in the alert state, dLGN neurons respond better to visual stimuli that change rapidly in time, i.e., containing high temporal frequencies, as compared with the quiescent state (Bezdudnaya et al., 2006; Stoelzel et al., 2017; Aydin et al., 2018). Numerous mechanisms have been proposed for these state-dependent shifts in visual processing (Shapley and Victor, 1978, 1981; McCormick, 1992; Fanselow et al., 2001; Eyding et al., 2003; Castro-Alamancos, 2004; Hirata et al., 2006; Ruiz et al., 2006; de Labra et al., 2007; Huguenard and McCormick, 2007; Briggs and Usrey, 2008; Liang et al., 2020; Schröder et al., 2020; Molnár et al., 2021), yet the contribution of the cortical feedback projections to the dLGN has not been established.
Visual cortex sends massive feedback projections to the dLGN via specific excitatory neurons located in layer 6 (Guillery, 1969). In fact, these projections outnumber the retinal input by an order of magnitude (Van Horn et al., 2000). Because visual cortex undergoes dramatic shifts in activity between the alert and quiescent states (Niell and Stryker, 2010; Lee et al., 2014), visual cortex, through its feedback to the thalamus, may well impact the visual responses of the dLGN in a state-dependent manner.
While many studies have addressed the role of cortico-thalamic feedback on visual responses in the dLGN (Destexhe, 2000; O’Connor et al., 2002; McAlonan et al., 2006, 2008; Andolina et al., 2007; Briggs and Usrey, 2011; Mease et al., 2014; Crandall et al., 2015; Denman and Contreras, 2015; Kirchgessner et al., 2020; Born et al., 2021), none of these studies tested whether cortico-thalamic feedback contributes to the differences in the visual response properties of the thalamus depending on the state of the animal.
Here, we use optogenetic approaches to rapidly and reversibly silence either visual cortex or the layer 6 cortico-thalamic neurons, while simultaneously recording from the dLGN and the hippocampus to record visual responses and to monitor brain state, respectively. Silencing feedback projections removed brain state-dependent differences in the temporal and spatial response properties of dLGN neurons, without affecting brain state. Therefore, feedback projections from visual cortex to the thalamus contribute to the state-dependent shifts in how the external world is represented even at this very early stage of sensory processing.
Materials and Methods
Animal protocols
All procedures were conducted in accordance with the National Institutes of Health guidelines and with the approval of the Committee on Animal Care at University of California San Diego (protocol S02160M) and University of California San Francisco (protocol AN131913). Animals were housed on a reverse light cycle in cages of five mice or less. At the time of electrophysiology, all animals were older than 3.5 weeks. Both male and female animals were used in an approximately equal ratio.
Mouse lines
vGat-ChR2 (The Jackson Laboratory stock number 014548), Ntsr1-Cre.
Viruses
AAV2/9.CAG.flex.Arch.GFP from the University of North Carolina viral vector core.
AAV2/1.CAG.flex.ChR2.GFP from the University of North Carolina viral vector core.
AAV2/9.hSyn1.flex.GtACR2.FusionRed prepared at Janelia Research Campus (titer used: 5*10̂11).
Animal surgery: awake recordings
We implanted a chronic head frame for awake electrophysiology recordings at least 5 d before the recording.
Head frame surgery
Animals were anesthetized with 2% isoflurane. After removing the hair on the head and sterilizing the skin, the skin on the top part of the skull was removed. A bone scraper and a scalpel blade were used to clean and score the surface of the skull. A bone screw was inserted bilaterally into each skull plate at 0.75 mm anterior and 2 mm lateral of bregma. Then, a thin layer of Vetbond was applied to the skull followed by the application of dental cement mixed with black paint to affix the head frame to the skull. The black dental cement covered all areas of the skull except primary visual cortex (V1) to prevent light for optogenetic stimulation from accessing other cortical areas. This dental cement was also used to build up a recording well for containing artificial CSF (ACSF) during in vivo electrophysiology. A single dose of 10% buprenorphine was administered, and we checked on the mice daily after the surgery.
Electrophysiology in dLGN and V1
Before recording, we briefly anesthetized the mice to drill away the dental cement covering the skull, as previously described (Reinhold et al., 2015), to thin the skull over V1, and to make two small craniotomies (each ∼50 μm in diameter) over V1 and over the dorsal lateral geniculate nucleus (dLGN). We thinned the skull over V1 until it was transparent when coated in ACSF. We targeted the V1 recording to ∼3.75 mm posterior and 2.5 mm lateral of bregma, and we targeted the dLGN recording to ∼1.8 mm posterior and 2 mm lateral of bregma, and 2.4–3 mm beneath pia, measuring visual responses to help target the recording sites in visual thalamus. For these recordings, we placed the V1 and dLGN electrodes in the brain before allowing the animal to wake up from anesthesia.
Marking recording track in visual thalamus
The electrode placed in visual thalamus was coated with DiI to label the recording track, as previously described (Reinhold et al., 2015). Recording sites in thalamus were then verified postmortem (see below Verification of thalamic recording sites).
Recording the primary somatosensory cortex (S1) local field potential (LFP)
We measured the LFP in primary somatosensory cortex (S1), with a 16-channel linear extracellular array from a site ∼250 μm beneath the pia.
Animal surgery: viral injections
Pup injections of ArchT into Ntsr1-Cre visual cortex
We injected AAV2/9.CAG.flex.Arch.GFP into the left visual cortex of neonatal mouse pups between postnatal days 0 and 2, as previously described (Reinhold et al., 2015). We did not record from these animals before postnatal day 30.
Adult injections of GtACR2 into Ntsr1-Cre visual cortex
We performed three craniotomies per mouse in the left hemisphere only. The craniotomies were located at (1) [0.4 mm anterior of lambdoid suture, 2.35 mm lateral of midline], (2) [0.4 mm anterior of lambdoid suture, 2.85 mm lateral of midline], and (3) [1.2 mm anterior of lambdoid suture, 2.6 mm lateral of midline]. Within each craniotomy we performed one injection of 150 nl at each of two depths: 700 and 450 μm. The injection speed was 30 nl/min. Recordings were done at two weeks postinjection because of virus toxicity observed at 3+ weeks.
Postmortem histology
Animals were not perfused, but brains were fixed in 4% paraformaldehyde (PFA) in PBS for two nights at 4°C. Brains were then transferred to 30% sucrose for 2 d before sectioning on a freezing microtome. Sections were 50 μm thick. We then mounted the sections with a mounting medium containing DAPI. Sections were imaged using a fluorescent microscope.
Verification of thalamic recording sites
Electrophysiology recording tracks targeted to thalamus were marked with DiI at the time of the recording (see above Marking recording track in visual thalamus). Penetration of the dLGN was confirmed postmortem. We discarded the data from mice in which we observed a recording track outside of dLGN.
Habituating mice to recording set-up
Before recording, we placed each mouse on a circular treadmill in the head-fix set-up for 30–60 min each day for 3–5 d. Once the mouse appeared comfortable in the head-fix, we proceeded with recordings. Visual stimuli consisting of drifting gratings were presented during habituation sessions.
Measuring running
We attached a rotary encoder to the circular treadmill to measure the animal’s running speed and direction.
Extracellular electrophysiology
At each recording site in visual cortex or dLGN, we used either (1) a 16-channel linear NeuroNexus silicon probe (A series), with either 50- or 25-μm spacing between linearly arranged electrode sites; or (2) a 32-channel linear NeuroNexus silicon probe with 20-μm spacing between linearly arranged electrode sites. The 50-μm spacing in the 16-channel linear probe enabled simultaneous recordings from all V1 layers. We used the 25-μm spacing to specifically target deeper V1 layers. Recording electrodes were connected to a 10× or 20× preamplifying head-stage from AM Systems (Plexon adapter). The dLGN recording was then amplified 200× using the AM Systems 3500 amplifier. The V1 recording was amplified 500× using the AM Systems 3600 amplifier. Both extracellular voltage traces were filtered between 0.1 Hz and 10 kHz at the amplification step. A National Instruments Data Acquisition device was used to digitize the analog voltage signals, before these signals were acquired and displayed in MATLAB (custom software by S. Olsen and K. Reinhold, as in Reinhold et al., 2015).
Visual stimulation
Two types of visual stimulation were used:
Drifting gratings
Sinusoidal drifting gratings were oriented patterns of periodically varying luminance (i.e., black and white bars with graded transitions). Spatial frequency and temporal frequency (i.e., drift speed) were varied for the drifting gratings. Unless otherwise specified, figures show an average of responses across spatial frequencies 0.02, 0.03, 0.04, 0.06, and 0.08 cycles per degree (cpd) and a temporal frequency of 3 Hz. For drifting gratings, we used an LCD computer monitor for display (γ-corrected, mean luminance 50 cd/m2, refresh rate 60 Hz) at a distance of 25 cm from the eye contralateral to the V1 recording site. MATLAB’s Psychophysics Toolbox was used to display the drifting gratings. Unless otherwise specified, drifting grating contrast was 100%, and the mean luminance of the drifting grating was matched to the gray interstimulus blank screen.
Full-field flicker
By positioning a blue light-emitting diode (LED) in front of a lens (5×, 0.15 NA), we placed an ∼1/2-inch homogeneous beam over the eye of the mouse contralateral to the recording sites. There was no spatial structure to this beam. We flickered this LED at varying temporal frequencies between 1 and 60 Hz. Unless otherwise specified, the contrast of this flicker was 100%, varying between 0 and 25 mW (∼3.5 mW/cm2). The luminance varied sinusoidally in time.
Measuring spontaneous activity
We measured spontaneous activity during the presentation of an unchanging blank gray screen on the computer monitor (see above Visual stimulation).
Photo-activation of cortical inhibitory interneurons to silence V1 excitatory cells
A blue LED (either 455 or 473 nm) coupled to an optical fiber with a 1-mm diameter was positioned just above the visual cortex, ipsilateral to the dLGN recording. The skull was thinned above V1 and coated in ACSF on the day of the electrophysiology experiment (see above, Animal surgery: awake recordings), allowing the blue light from the LED (25 mW total power) to penetrate the cortex. Because the vGat-ChR2 transgenic mouse line expresses ChR2 in vGat+ inhibitory interneurons in the cortex, blue light in cortex activates these inhibitory interneurons. The illumination of V1 inhibited putative excitatory neurons in cortex (Fig. 3A and as in Reinhold et al., 2015).
Photo-inhibition of Ntsr1+ neurons in visual cortex
ArchT
Either an amber LED (595 nm, 20 mW) coupled to an optical fiber with a 1-mm diameter or an amber laser (550 nm, 25 mW) coupled to a fiber with a 0.2-mm diameter was positioned just above the visual cortex, ipsilateral to the dLGN recording. The skull was thinned over V1, as described above (Electrophysiology in dLGN and V1). Illumination of visual cortex led to suppression of neurons in V1 (Fig. 7A). We included data from experiments using both the amber LED and the amber laser.
GtACR2
We used a blue LED (25 mW) coupled to an optical fiber with a 1-mm diameter to illuminate the visual cortex (Fig. 7E).
Blue light control
We used ambient blue light surrounding the mouse to mask sight of the blue LED used for optogenetic manipulation. Additionally, to test whether the blue light emitted by the optogenetic LED could affect the visual response directly (i.e., via the retina), in one mouse, we occluded the craniotomy with opaque Kwik-Cast during the recording, after verifying an effect of optogenetic cortical silencing on dLGN activity. The blue optogenetic LED remained positioned above the visual cortex but was unable to illuminate the cortex through the opaque Kwik-Cast. We tested whether turning on the LED in this case, in the absence of any optogenetic manipulation, had an effect on the visual response in dLGN. There was no effect (data not shown). Similarly, when using the amber LED/laser to inhibit ArchT-expressing Ntsr1+ neurons in cortical layer 6, we used ambient amber light surrounding the mouse to mask sight of the optogenetic amber LED/laser.
Data analysis: sorting single units
Multiunit activity
Multiunit activity was the high-pass-filtered electrophysiology signal (above 300 Hz).
Cluster selection
First, we clustered spike waveforms into clusters using UltraMegaSort (D. N. Hill, S. B. Mehta, and D. Kleinfeld) by dividing each linear array of 16 electrodes into four tetrodes (or 32 electrodes into eight tetrodes; four neighboring electrodes in each tetrode) and then clustering spikes based on the shape and size of spike waveforms on each tetrode. We selected well-isolated clusters with spike waveform amplitudes well above the spike detection threshold, which was set at 5.5 times the standard deviation of the high-frequency noise. We fit a Gaussian to the distribution of spike waveform amplitudes in each selected cluster and verified that >85% of the spikes in the cluster were above the spike detection threshold. Furthermore, we ensured that, within each cluster, there were fewer refractory period violations (i.e., cases when two spikes occurred within 1.5 ms of each other) than 1% of the number of total spikes.
Defining and clustering bursts
Relay neurons in the dLGN sometimes burst. These bursts include a few spikes from the same neuron, very close together in time (here we define a burst as two or more spikes with an interspike interval of <8 ms), and the amplitude of the spike waveform decreases for each spike in the burst, but the spike waveform shape does not change. Because UltraMegaSort uses spike amplitude to cluster the spikes, it is conceivable that smaller burst spikes from a dLGN unit might be clustered separately from the nonburst spikes and from the first spike in the burst. Our goal was to be sure that each single unit contained the burst as well as nonburst spikes from the neuron (for example, see Fig. 4B). Therefore, we used the following procedure to combine clusters of burst and nonburst spikes likely belonging to the same source, a single neuron. After selecting well-isolated clusters (see above Cluster selection), we inspected all pairwise combinations of these clusters and permanently combined the two clusters, e.g., cluster 1 and cluster 2, if the following conditions were met:
The average waveforms of cluster 1 across the tetrode scaled very precisely, as determined by-eye, onto the average waveforms of cluster 2 (i.e., same shapes of spike waveforms, although spike waveform sizes may differ).
If one cluster in the pair had smaller-sized spike waveforms, this cluster contained fewer spikes than the cluster with larger spike waveforms (because smaller spikes should only occur after the first large spike in a burst).
More than 5% of the spikes in the cluster with the smaller spike waveforms should immediately follow (i.e., occur within 10 ms of) a spike in the cluster with larger spike waveforms.
The combined cluster (composed of the cluster pair) contained fewer refractory period violations than 1% of the total number of spikes in the combined cluster.
We iterated this procedure on the clusters that emerged after a first round of combinations, and iterated again on the output of that round of combinations, and so forth, until all pairs of clusters meeting the above criteria had been combined and no more clusters could be combined according to these criteria. We inspected this final set of clusters by-eye and validated only the clusters with spike amplitude modes well above the spike detection threshold and with fewer refractory period violations than 1% of the total number of spikes in the cluster. These final, curated clusters were the single units used for further analysis.
Sorting cortical units
For extracellular units recorded in cortex, we sorted the spike waveform clusters as described above Cluster selection, but we did not further combine clusters to find the burst spikes.
Separating regular-spiking (RS) and fast-spiking (FS) units in cortex
We measured the half-width of a spike waveform at its half-maximum height. We separated the regular-spiking (putative excitatory) units and fast-spiking (putative inhibitory) units in the cortex as described in (Reinhold et al., 2015).
Data analysis: separating the alert and quiescent brain states
A 16-site or 32-site linear extracellular recording electrode was placed at a depth such that the top channel on this electrode would sit in the ventral part of hippocampus and the bottom channels on this electrode would penetrate dLGN (see above, Extracellular electrophysiology). Thus, we could measure the local field potential (LFP) from the hippocampus and record single units in dLGN simultaneously. We measured the theta power in the hippocampal LFP to distinguish the alert and quiescent brain states. We used the mtspecgramc function in Chronux (Bokil et al., 2010) to measure the theta power of the hippocampal LFP. We defined the theta power as the power between 5 and 7 Hz minus the power at 2 and 4 Hz, as previously shown (Bezdudnaya et al., 2006). We calculated the power in each of these frequency bands over 0.8-s-long time windows by passing the following parameters to Chronux: movingwin = [0.8 0.2] and params.tapers = [3 5], to specify a time window of 0.8 s with a step size of 0.2 s and a time-bandwidth product of three with five tapers. Finally, we normalized the power spectrum by its sum across all frequencies at each time point to focus the analysis on the relative power in different frequency bands. For each experiment, we plotted a histogram of the theta power averaged across trials in the experiment. Note that silencing cortex does not change the theta power in hippocampus (see Fig. 3B); thus, we included time windows when the blue LED was illuminating cortex. We inspected this bimodally distributed histogram of theta power (Fig. 1B, scatter plot) and selected, by-eye, the theta power threshold that seemed to best divide the two modes in the histogram. We classified trials with an average theta power above this threshold as “alert” and trials with an average theta power below this threshold as “quiescent.” The mice were often but not always running in the alert state. For example, in Figure 1, each trial lasted for 14.5 s, and, of the trials classified as alert, 86% of these theta trials showed running. Here, “running” means that the mouse ran continuously for at least 1 s. When calculating the fraction of time spent in each brain state, we smoothed the theta power using 4-s bins.
Data analysis: measuring cortical synchronization
We recorded the LFP in V1 using an extracellular electrode (see above Extracellular electrophysiology). We then calculated the cortical synchronization as the low-frequency LFP power (0.5–6 Hz) minus the high-frequency LFP power (30–80 Hz). We used the mtspecgramc function in Chronux to measure the power over 0.8-s-long time windows and passed this function the following parameters: movingwin = [0.8 0.2] and params.tapers = [3 5], to specify a time window of 0.8 s with a step size of 0.2 s and a time-bandwidth product of three with five tapers. We normalized the power spectrum at each time point by its sum across all frequencies.
Data analysis: units of LFP power spectrum, hippocampus theta, and cortex synchronization
In general, the units of the power spectrum of the LFP are V2 Hz−1. However, in the cases of hippocampus theta and cortex synchronization, we normalized the power spectrum by its sum across all frequencies at each time point, to focus on the relative power across different frequency bands. Therefore, these are normalized measures.
Data analysis: quantifying power of the F1 response
F1 response to full-field flicker at varying temporal frequencies
We presented full-field visual flicker at frequencies between 1 and 60 Hz. The stimulus structure was the following: 1 s of mean-luminance baseline (no flicker), 2 s of full-field flicker modulated sinusoidally in time, then another 2 s of mean-luminance baseline. We calculated the unit’s trial-averaged peri-stimulus time histogram (PSTH), a binned count of spikes per second, as the unit’s response. We measured the F1 response to this full-field flicker using the mtspectrumpb function in Chronux (Bokil et al., 2010) over the full 2 s of the time-varying visual stimulus. We passed the following parameters to mtspectrumpb: params.tapers = [0.9 2 0], to specify a bandwidth of 0.9, a time window of 2 s and three tapers. We measured the F1 response as the power in the response frequency matching the stimulus temporal frequency. We averaged the PSTH of the unit’s spiking before taking the power.
F2 response
In Figure 2 D,E, we measured the F2 response as the power at the response frequency equivalent to two times the stimulus temporal frequency.
F1 response to drifting gratings
We measured the power of a single unit’s F1 response to a drifting grating visual stimulus with a fundamental temporal frequency of 3 Hz as follows. We calculated the unit’s trial-averaged PSTH, a binned count of spikes per second, as the unit’s response. We then used the mtspecgrampb function in Chronux (Bokil et al., 2010) to measure the power at 3 Hz in that unit’s response. We averaged the PSTH of the unit’s spiking before taking the power. Unless otherwise noted, we measured the power at 3 Hz over a time window of 1 s. We then stepped this 1-s-long time window along the PSTH, at intervals of 0.05 s, to get a smoothly varying F1 power over time. We passed the following parameters to Chronux: movingwin = [1 0.05] and params.tapers = [5 6] (note that the first number, 5, is the time-bandwidth product), specifying a time window of 1 s in steps of 0.05 s and six tapers. When we measured the response to a visual stimulus with a temporal frequency of 1 Hz, we used a 2-s time window for the power calculation (see above, F1 response to full-field flicker at varying temporal frequencies, for a discussion of the frequency response curves as in Fig. 1E). We present the F1 power as follows. In the figures, we show the raw F1 power of spiking activity in units of 1e5. An F1 power of 0.1 in units of 1e5 (i.e., 1e4) roughly corresponds to a PSTH with a 10 spikes per second peak-to-trough sinusoidal modulation at 3 Hz only; an F1 power of 4 in units of 1e5 corresponds roughly to a PSTH with a 20 spikes per second peak-to-trough sinusoidal modulation at 3 Hz; and an F1 power of 16 in units of 1e5 corresponds roughly to a PSTH with a 40 spikes per second peak-to-trough sinusoidal modulation at 3 Hz.
Power calculation before or after trial averaging
Unless otherwise specified, we measured the F1 power of the trial-averaged PSTH. However, we also measured the F1 power of each individual trial before averaging across trials to control for any change in eye position across trials, although rodents make more, not fewer, eye movements when running (Wallace et al., 2013), and this should, if anything, lower F1 amplitude during the alert as compared with the quiescent state, whereas we see higher F1 amplitude during the alert state. Also note that this method is more likely to pick up spontaneous low-frequency activity as spurious 3-Hz visually evoked signal. All results were qualitatively unchanged using either analysis approach (data not shown).
Data analysis: normalization of F1 power
In some cases, we present the F1 power across units normalized to a certain condition, for example, in Figure 1. First, we subtracted the baseline F1 power before the onset of the visual stimulus. Second, each unit’s F1 response was divided by its total power across all response frequencies between 0 and 250 Hz. Third, we normalized the response curve across all temporal or spatial frequencies to the average response within a certain condition (e.g., control condition). We always confirmed that effects shown in the normalized plot qualitatively matched the effects on the raw F1 power, and we always show the raw data in other plots as well as normalized data.
Data analysis: normalizing single-unit peri-stimulus time histogram (PSTH) of F1 power
Unless otherwise specified, the average PSTH of F1 power was presented as an average across all single units. Where specified as normalized, the PSTH of F1 power was divided by the average visually evoked F1 power (i.e., during the visual stimulus) in the control condition (no optogenetic manipulation), to show the fractional change as a result of the optogenetic manipulation. We normalized each single unit’s F1 power to its own visually evoked F1 power in control conditions after subtracting the baseline F1 power. Note that, in the case that a unit had a small visually evoked F1 response with respect to baseline, this normalization amplified noise. Thus, we chose to include only the most visually responsive units in the normalized PSTH. These were the units with the largest increase in F1 power with respect to baseline (see next section).
Data analysis: selecting visually responsive units
When we presented the raw, non-normalized data, we included all units recorded in dLGN. However, when we presented a normalized PSTH of F1 power, we selected only the visually responsive units, because including nonvisually responsive units in the normalized figure amplifies noise. To pick the visually responsive units, we chose a threshold F1 power and included all units with an F1 response greater than this. We chose a threshold to separate the top 25% of units with the largest F1 responses. These were the units deemed “visually responsive.” When we show figures including only visually responsive units, we always also show, somewhere else, the same experiment including all units recorded in dLGN (even units without a visual response). Thus, we always show both the result including all units as well as the result including only the visually responsive units. This occasionally produced differences in the exact magnitude of the effect but no change in the qualitative effect.
Data analysis: measuring the power spectrum of the S1 LFP
We measured the LFP in somatosensory cortex (S1) using an extracellular electrode (see above Recording the primary somatosensory cortex (S1) local field potential (LFP)). We calculated the power spectrum of the S1 LFP using the mtspectrumc function in Chronux. We passed the following parameters to this function: params.tapers = [3 5], specifying a time-bandwidth product of three and five tapers.
Data analysis: fraction burst spikes
To test whether the dLGN units that bursted more also showed a bigger effect of cortical silencing, we calculated the fraction of each unit’s spikes that occurred in bursts. For instance, a “fraction burst spikes” of 0.1 for a unit indicates that 10% of all its spikes occurred in bursts.
Data analysis: selecting putative Ntsr1+ single units
ArchT or GtACR2
We aimed to quantify the fraction of Ntsr1+ units in cortex suppressed by the ArchT or GtACR2 optogenetic manipulation. Because we injected Cre-dependent ArchT or Cre-dependent GtACR2 into layer 6 of the visual cortex of the Ntsr1-Cre line, we expected a fraction of Ntsr1+ neurons to express ArchT or GtACR2 and therefore be suppressed by illumination with amber/blue light. However, an alternate source of suppression of cortical neurons needed to be considered: our data showed that suppressing cortical feedback onto thalamus led to a decrease in thalamic spontaneous activity, which is expected to lead to a decrease in cortical spontaneous activity (Reinhold et al., 2015). Thus, cortical units suppressed by illumination with amber light were likely to include both directly suppressed ArchT-expressing or GtACR2-expressing Ntsr1+ units and cortical units driven by thalamic input. To study this, we considered the ArchT experiments. To identify the directly suppressed ArchT-expressing Ntsr1+ units, we noted that these units should be suppressed before dLGN spontaneous activity was suppressed. We measured the time course of suppression of spontaneous activity in dLGN and found that its onset was delayed by 35 ms with respect to the onset of the amber LED directed at cortex (Fig. 7C,D). Hence, we searched for units in the deep layers of cortex that were suppressed within the first 35 ms of the onset of the amber LED. These units represented putative ArchT-expressing Ntsr1+ neurons. (We used the same criterion for selecting GtACR2-expressing, putative Ntsr1+ units in visual cortex.)
For recordings in visual cortex in the Ntsr1-Cre mice, we positioned the 16-channel recording electrode in V1 such that the bottom-most channels on the electrode array were ventral to cortex (i.e., no spiking), and the electrode was placed at an angle of ∼40° from the tangent to the pia. We then measured putative layer 6 as the bottom-most 400 μm on the angled recording electrode, with respect to the deepest well-isolated single unit. Accounting for the electrode angle, this represents the bottom-most 250 μm of cortex, consistent with the size of layer 6 in the mouse.
Single units were classified as putative ArchT-expressing or GtACR2-expressing if they met the following criteria:
Recorded in putative layer 6.
Regular-spiking (see above Separating regular-spiking (RS) and fast-spiking (FS) units in cortex).
Mean firing rate significantly suppressed within the first 35 ms of the onset of the amber/blue LED (p-value < 0.05 according to Wilcoxon rank-sum).
Or mean firing rate suppressed (p-value < 0.2 according to Wilcoxon rank-sum) within the first 35 ms of the onset of the amber/blue LED and firing rate still suppressed (including n.s. units) throughout visual stimulation (vs dLGN activity, which is not clearly suppressed during visual stimulation).
We found 25 out of 157 putative layer 6 regular-spiking units that met these criteria for the ArchT experiments. Because the Ntsr1+ neurons are ∼60% of the total neurons in cortical layer 6 (Bortone et al., 2014), our results suggest that ∼25% of the Ntsr1+ neurons expressed ArchT and were directly inhibited by illumination with amber light. (Note that, given these criteria, chance would predict that we see only 11.5% of putative layer 6 regular-spiking units that meet the criteria.) Importantly, the putative ArchT-expressing Ntsr1+ units were suppressed even before we observed any suppression of spontaneous activity in dLGN.
Data analysis: difference in baseline firing rate of dLGN neurons across mouse lines
The average spontaneous firing rate of dLGN neurons in the Ntsr1-Cre mouse line (in the alert brain state, average: 5.4 Hz, SEM: 0.46 Hz, n = 144 units) was lower than in the vGat-ChR mouse line (in alert brain state, average: 7.3 Hz, SEM: 0.34 Hz, n = 377 units). This was a significant difference quantified using the Wilcoxon rank-sum test (p-value = 0.0029). Despite this, we observed the same effect of suppressing cortico-thalamic feedback on dLGN visually evoked activity in both mouse lines.
Data analysis: defining preferred and nonpreferred spatial frequencies (Fig. 10E,F)
To test how cortico-thalamic feedback affects the representation of spatial frequency in dLGN, we presented the spatial frequencies 0.02, 0.03, 0.04, and 0.08 cycles per degree. We then identified the preferred and nonpreferred spatial frequencies for each dLGN neuron by measuring the F1 power (visually evoked and baseline-subtracted, i.e., over the entire duration of the visual stimulus minus the F1 power in the 4 s preceding the visual stimulus) in response to each spatial frequency and ordered these responses from highest (preferred) to lowest (nonpreferred). We selected one preferred spatial frequency and one nonpreferred spatial frequency for each neuron. For plots during the quiescent state, we identified the preferred and nonpreferred spatial frequencies based on the response in the alert brain state during cortical silencing. For plots during the alert brain state, we identified the preferred and nonpreferred spatial frequencies based on the response in the quiescent brain state during cortical silencing. (Thus, we avoid any issues of regression to the mean. For example, if we had chosen the preferred and nonpreferred visual stimuli based on the responses in control, we would expect, by chance, the selectivity/tuning to be less strong during cortical silencing, by definition, as a result of regression to the mean. However, our approach, using an independent measurement to select preferred and nonpreferred visual stimuli, avoids this confound.) Therefore, we can compare spatial frequency selectivity with and without cortical silencing.
Data analysis: selectivity index and selectivity ratio for spatial frequency tuning
We present two metrics capturing spatial frequency tuning in the dLGN, the selectivity ratio and the selectivity index (Fig. 10E,F). We defined the selectivity ratio as the average visually evoked and baseline-subtracted F1 power in response to the preferred spatial frequency divided by this average in response to the nonpreferred spatial frequency. We defined the selectivity index as the difference of the preferred response and the nonpreferred response divided by the sum of the preferred response and the nonpreferred response. We ran the statistical tests on the selectivity index metric to avoid “divide by 0” issues, but we also present the selectivity ratio for intuition about the effect size.
Results
Defining alert and quiescent brain states
We measured global brain states in awake mice that were head-fixed yet free to spontaneously run or rest on a circular treadmill (Materials and Methods; Reinhold et al., 2015). We defined brain state by the presence or absence of hippocampal theta oscillations in the local field potential (LFP) recorded just ventral of the hippocampus, consistent with previous descriptions (Bezdudnaya et al., 2006). The power of the theta frequency band (5–7 Hz) was bimodally distributed and inversely correlated with the power of low-frequency oscillations (0.5–6 Hz) simultaneously recorded in visual cortex (Fig. 1A–C). We refer to periods of high power in the hippocampal theta frequency band as “alert state,” a brain state that has been linked to running, enhanced alertness and high sensorimotor engagement (Green and Arduini, 1954; Buzsáki, 2002). Conversely, periods of low power in the hippocampal theta frequency band, generally associated with reduced alertness to external sensory stimulation (Kandel and Buzsáki, 1997; Swadlow and Gusev, 2001; Bezdudnaya et al., 2006; Bereshpolova et al., 2011), are here referred to as “quiescent state.” During the alert state, the mice were mostly but not always running (Fig. 1B; in 86% of alert trials, the mouse was running), while during the quiescent state the mice were almost never running (the mice ran in <4% of trials classified as quiescent). The alert and quiescent states alternated every 9.5 s on average (9.5 ± 13.0 s, mean ± SD) and lasted on average 7.6 and 11.7 s, respectively (alert: 7.6 ± 6.4 s, mean ± SD, quiescent: 11.7 ± 18.3 s, mean ± SD).
Contribution of visual cortex to brain state dependence of thalamic responses to visual stimuli
To determine how brain state impacts the response of dLGN neurons to temporal features of the visual stimulus, we recorded from these neurons using multisite extracellular probes. The dLGN recording sites were labeled with a fluorescent dye and validated ex vivo (Materials and Methods). To hold the spatial structure of the visual stimulus constant while varying the temporal frequency, we presented a visual stimulus called full-field flicker, the sinusoidal modulation of full-field luminance at temporal frequencies between 1 and 60 Hz (Materials and Methods), to the eye contralateral to the recorded hemisphere.
The firing of isolated putative dLGN relay neurons (n = 254 units from 5 mice) was modulated by the fundamental temporal frequency (F1) of the visual stimulus. For example, in response to a visual stimulus flickering at 4 Hz, the firing rate of dLGN neurons was modulated at 4 Hz. (44% of the visually modulated spikes were F1-modulated, 30% were F2-modulated, and <26% were modulated at other frequencies.) We defined the F1 response of a neuron as the amplitude of the F1 modulation of its firing rate in response to a range of stimulus frequencies. The F1 response of dLGN neurons was markedly different between the alert and quiescent states, consistent with results in other species (Bezdudnaya et al., 2006) and previous work (Aydin et al., 2018). Not only was the F1 response more pronounced during the alert state, but it also peaked at higher temporal frequencies (Fig. 1D,E, left-most panels; list of mice in Table 1). That is, in the alert state, the activity of dLGN neurons was more strongly driven by the temporal properties of the visual stimulus and followed higher frequencies, as compared with the quiescent state. Thus, the temporal response of mouse dLGN neurons to visual stimuli depends on brain state (for more example neurons and further quantification, see Fig. 2).
Does primary visual cortex (V1) contribute to the dependence of dLGN neurons’ responses to brain state? To address this question, we optogenetically silenced V1 using the vGat-ChR2 mouse line, in which the opsin is selectively expressed in GABAegic neurons (Olsen et al., 2012; Materials and Methods). V1 was silenced (Fig. 3A) for a brief period of time (3 s window beginning 0.5 s before the onset of the visual stimulus and continuing throughout the visual stimulus) during either the alert or quiescent state while presenting visual stimuli at various temporal frequencies. V1 illumination did not change brain state (Fig. 3B), as measured by the theta power of the LFP of hippocampal recordings, nor did it impact running behavior (switch from stationary to running or running to stationary in 20% of trials without V1 silencing and 16% of trials with V1 silencing, n.s., p-value = 0.22 from Wilcoxon sign-rank across sessions) consistent with previous studies (Resulaj et al., 2018). V1 illumination also did not affect the power of the LFP of nearby primary somatosensory cortex (Fig. 3C). Silencing V1 reduced spontaneous, nonvisually evoked dLGN activity in both the quiescent and alert states [quiescent state: (mean ± SEM) from 5.1 ± 0.24 to 3.9 ± 0.21 Hz, alert state: from 7.1 ± 0.32 to 4.9 ± 0.24 Hz, n = 377 units, 6 mice; Fig. 4A] and increased burst activity, also in both brain states (Fig. 4B–E). Strikingly, silencing V1 eliminated brain state differences in the visually evoked F1 response of dLGN neurons (Fig. 1D,E and more quantification in Fig. 2). V1 silencing strongly reduced the dLGN response to high frequencies (10–60 Hz) in the alert state while increasing the response to low frequencies (1–8 Hz) in the quiescent state (alert state: 41% decrease in the response to high stimulus frequencies, quiescent state: 39% increase in the response to low stimulus frequencies, n = 254 units from 5 mice; Fig. 2B,D,E for statistics). As a consequence, the F1 response in the alert and quiescent states became almost indistinguishable (Fig. 1E; also see Fig. 5 for a drifting grating visual stimulus). These results show that silencing V1, by reducing the F1 response to high frequencies in the alert state and enhancing the response to low frequencies in the quiescent state, effectively eliminates the visual response features that are unique to each brain state and leads to a response function that is intermediate between the quiescent and alert brain states. Thus, the state-dependent differences in the F1 response of the dLGN depend on V1.
Contribution of the cortico-thalamic feedback projection
To determine whether V1 impacts the F1 response of the dLGN via direct cortico-thalamic projections, we took advantage of a mouse line (Ntsr1-Cre) that selectively tags layer 6 cortical neurons that project back to the dLGN (Olsen et al., 2012; Bortone et al., 2014). To suppress this layer 6 population of neurons, we conditionally expressed either the inhibitory opsin GtACR2 or the inhibitory opsin ArchT (Materials and Methods). Consistent with V1 silencing, photo-suppression of these layer 6 cortico-thalamic neurons decreased spontaneous dLGN activity in both the quiescent and alert brain states, albeit to a lesser extent, likely because of the incomplete suppression of cortico-thalamic neurons [quiescent state (mean ± SEM): spontaneous dLGN activity from 3.9 ± 0.25 to 3.3 ± 0.23 Hz, alert state: from 5.4 ± 0.31 to 4.9 ± 0.30 Hz, n = 231 units, n = 7 mice, quiescent state: p < 10−6, alert state: p < 10−6 from paired Wilcoxon sign-rank test across units]. Importantly, however, for dLGN neurons showing a significant reduction of baseline activity on layer 6 silencing, the F1 response to low temporal frequencies in the quiescent brain state was enhanced, while the F1 response to high temporal frequencies in the alert brain state was suppressed (Fig. 6, alert state: 45% decrease to high stimulus frequencies, quiescent state: 143% increase to low stimulus frequencies, n = 43 units from four mice; spontaneous activity effects in Fig. 7; drifting gratings in Fig. 8; further quantification in Fig. 9). These data indicate that the state-dependent differences in the F1 response of the dLGN are mediated by V1 through cortico-thalamic layer 6 neurons.
Impact of visual cortex on visual spatial frequency tuning in dLGN
We next investigated whether brain state also affects the response of the dLGN to varying spatial frequencies of the visual stimulus, and whether this also depends on cortico-thalamic feedback. We used drifting gratings presented on a computer monitor to the eye contralateral to the recorded hemisphere (Fig. 10A) and varied the spatial frequency of the gratings (0.02–0.08 cycles per degree) while holding the temporal frequency constant (3 Hz). The response of dLGN neurons was larger in the alert state compared with the quiescent state for frequencies around 0.03 cycles per degree (cpd; at 0.03 cpd: alert state response was 79% larger than quiescent state response) indicating that brain state also affects the spatial frequency response of these neurons. Strikingly, silencing visual cortex, again, abolished this difference (Fig. 10B,C). This was mainly because of an overall increase in the responses recorded in the quiescent state (silencing V1 in the quiescent state increased the dLGN response across the population of units by 174% at 0.02 cpd, 167% at 0.03 cpd, 118% at 0.04 cpd, and 70% at 0.08 cpd; silencing V1 in the alert state increased the response by 136% at 0.02 cpd, 24% at 0.03 cpd, 57% at 0.04 cpd, and 330% at 0.08 cpd; see Fig. 10D for distributions of all units; Fig. 10E,F shows that silencing cortex during the quiescent state recovered single units’ alert state selectivity to spatial frequency). Thus, silencing visual cortex in the quiescent state enhances the dLGN responses across all spatial frequencies, thereby matching responses in the alert state. Similarly, suppressing specifically layer 6 cortico-thalamic neurons enhanced the response of dLGN neurons at middle spatial frequencies (<0.08 cpd), particularly in the quiescent state (Fig. 11).
Discussion
The transmission of visual information from the retina to the cortex relies on an intermediary thalamic nucleus, the dLGN. The response properties of the dLGN to visual stimuli are highly dependent on the state of alertness of the animal (Bezdudnaya et al., 2006; Williamson et al., 2015; Stoelzel et al., 2017; Aydin et al., 2018; Liang et al., 2020; Hei et al., 2014). Our results indicate that a major component of this state dependence of dLGN responses requires the activity of visual cortex and, specifically, the feedback projections from cortex to thalamus. Indeed, when silencing visual cortex, the response properties of dLGN to visual stimuli are similar across states of alertness. In the temporal domain, this equalization of responses across states results from a reduction of the F1 response to high frequencies in the alert state and an enhancement, in the quiescent state, of the F1 response to low frequencies. As a consequence, upon cortical silencing, the temporal response properties of the dLGN are intermediate between the quiescent and alert brain states, regardless of the actual brain state of the animal (Fig. 1). In the spatial domain, the equalization of the responses between alert and quiescent states results from an enhancement, in the quiescent state during cortical silencing, of the response to middle frequencies (Fig. 10). Furthermore, silencing visual cortex reduces spontaneous activity in the dLGN regardless of brain state (Fig. 4A). Thus, in the absence of visual stimulation, the net effect of visual cortex onto dLGN neurons is excitatory regardless of brain state.
Is the impact of visual cortex on dLGN neurons’ activity permissive or instructive? It is reasonable to expect that the visual cortex may play a permissive role, such that removing the excitatory feedback from visual cortex may put dLGN neurons into a state that is less responsive, for example, to high temporal frequencies. This is supported by our data showing that silencing the visual cortex increased the bursting frequency of dLGN neurons regardless of brain state (Fig. 4E). This bursting of dLGN neurons, on removal of the excitatory drive from cortex, results from a combination of intrinsic and circuit properties that, together, may make dLGN neurons more likely to follow low frequency as compared with high frequency visual input (McCormick and Pape, 1990; McCormick and Huguenard, 1992; Contreras et al., 1996; Steriade, 1997). This may explain the shift from preferring higher to preferring lower temporal frequencies upon cortical silencing and, as a consequence, the equalization of responses across brain states.
Alternatively, or in addition, cortex may play an instructive role in determining the activity pattern of the dLGN. The response to high temporal frequencies of the dLGN may be amplified via the cortico-thalamic loop involving layer 6 feedback projections. In the alert state, cortex is responsive to the temporal properties of the stimulus, while in the quiescent state, cortex is dominated by its own internal activity (Steriade, 1997; Vinck et al., 2015; Clancy et al., 2019; Clayton et al., 2021; Nestvogel and McCormick, 2022). As a consequence, in the alert state, the cortical feedback may enhance visual responses in the dLGN, while in the quiescent state, the cortical feedback may actively disrupt dLGN neurons’ visual responses by adding a pattern of activity that is not matched to the visual stimulus.
Previous work has associated the brain state-dependent shift in visual responses in the dLGN with the cholinergic input from the brainstem/basal forebrain (Sillito et al., 1983; Steriade et al., 1990; von Krosigk et al., 1993; Erişir et al., 1997; Castro-Alamancos and Calcagnotto, 2001). Our work suggests that, upon cortical silencing, the cholinergic input alone is not sufficient to generate a robust state-dependent shift in visual responses. In other words, both the cholinergic input and the cortico-thalamic input might be necessary for the state-dependent shift in visual responses in the dLGN. This could be because, as explained above, cortical silencing may put dLGN neurons into a bursting mode that cannot be overcome by the cholinergic input alone.
Our identification of the contribution of cortical feedback brings us closer to understanding how the brain coordinates activity across cortex and thalamus to switch from an externally oriented brain state for sensory processing, in which the top-down feedback enhances the rapidly changing feed-forward sensory signal, to an internally oriented brain state, in which the top-down feedback suppresses the sensory response, possibly shifting the thalamus toward a representation of internal processes such as expectation, imagery or working memory.
Footnotes
This work was supported by National Institutes of Health Grants R01EY025668 and K99EY030415 (to A.R.) and by the Howard Hughes Medical Institute. We thank M. Mukundan and J. Evora for help with mouse husbandry.
The authors declare no competing financial interests.
- Correspondence should be addressed to Kimberly Reinhold at kimberly_reinhold{at}hms.harvard.edu
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