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NEUROSCIENCE |
1 Institute of Basic Medical Sciences, Department of Physiology, University of Oslo, PO Box 1103 Blindern, N-0317 Oslo, Norway
2 Department of Biochemistry and Biophysics, Faculty of Natural Sciences, Vilnius University, Ciurlionio 21, 03101 Vilnius, Lithuania
| Abstract |
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(Received 2 March 2007;
accepted after revision 10 May 2007;
first published online 10 May 2007)
Corresponding author P. Heggelund: University of Oslo, Institute of Basic Medical Sciences, Department of Physiology, PO Box 1103 Blindern, N-0317 Oslo, Norway. Email: paul.heggelund{at}medisin.uio.no
| Introduction |
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The retinal input to TC neurons is mediated by both NMDA receptors (NMDA-Rs) and non-NMDA-Rs (Hartveit & Heggelund, 1990; Heggelund & Hartveit, 1990; Scharfman et al. 1990; Sillito et al. 1990a,b; Funke et al. 1991; Turner et al. 1994). In vivo studies have suggested that the NMDA-Rs play a particularly important role in this type of synapse (Heggelund & Hartveit, 1990; Sillito et al. 1990b). The non-NMDA-Rs are of the AMPA type (Kielland & Heggelund, 2001; Chen et al. 2002). AMPA receptors (AMPA-Rs) have approximately linear voltage dependence (Hestrin et al. 1990), their EPSCs have a fast rise-time, lasting for milliseconds (Turner et al. 1994), and they may elicit short-latency spikes which preserve the timing of the afferent spikes (Blitz & Regehr, 2003). NMDA-Rs have highly non-linear voltage dependence (Mayer et al. 1984; Nowak et al. 1984), their EPSCs have slower rise-time, lasting for tens of milliseconds (Turner et al. 1994), and they elicit longer-latency spikes with more variable timing with reference to afferent spikes (Blitz & Regehr, 2003). By repetitive stimulation, both the AMPA and NMDA components show synaptic depression due to presynaptic mechanisms, and different postsynaptic mechanisms: fast desensitization of AMPA-Rs and saturation of NMDA-Rs (Chen et al. 2002; Kielland & Heggelund, 2002).
Several lines of evidence are consistent with the hypothesis that the sustained firing of TC neurons during static visual stimulation depends on input mediated by NMDA-Rs. In vivo experiments (Hartveit & Heggelund, 1990; Heggelund & Hartveit, 1990; Funke et al. 1991) have shown that NMDA-R antagonists strongly attenuate the sustained response in TC neurons of the non-lagged class (Mastronarde, 1987a), whereas the effect on the initial transient response is less consistent. In the class of lagged cells (Mastronarde, 1987a), which lack the initial transient and only give a relatively sustained response, NMDA-R antagonists almost completely abolish the visual response (Heggelund & Hartveit, 1990). Consistent with this, the timing of spikes in lagged cells is considerably less precise with reference to spikes in the retinal afferents than the timing in non-lagged cells (Mastronarde, 1987b). In line with these findings, in vitro studies have demonstrated that sustained spike firing in TC neurons during train stimulation of retinal afferents largely depends on input mediated through NMDA-Rs (Turner et al. 1994; Blitz & Regehr, 2003).
The non-linear voltage dependence of the NMDA-Rs is due to a Mg2+ blockade that is pronounced at hyperpolarized membrane potentials but gradually relieved by increasing membrane depolarization (Mayer et al. 1984; Nowak et al. 1984). Accordingly, in states when the TC neurons become depolarized, the NMDA component during repetitive inputs might become more pronounced and could reach the threshold for spike generation through temporal summation of the EPSPs. Thus, modulation of the membrane potential that adjusts the effect of the NMDA component could be a key mechanism for regulation of the degree of sustained firing during visual stimulation in vivo, and during train stimulation in vitro. Depolarization in the intact animal might be evoked by modulatory input from state-related nuclei in the brainstem (McCormick, 1992; Steriade et al. 1997), excitatory feedback from cortex (Lindström & Wróbel, 1990; Turner & Salt, 1998; von Krosigk et al. 1999), and possibly also strong input from retina. However, the pronounced synaptic depression at the retinogeniculate synaptic transmission (Chen et al. 2002; Kielland & Heggelund, 2002), might prevent generation of a sufficiently strong NMDA component. This raises the question of how NMDA-R mediated EPSPs in TC neurons summates temporally during repetitive retinal input at different membrane potentials.
To address this question, we made whole-cell recordings in current clamp and studied how responses of TC neurons to train stimulation of retinal afferents varied depending on the holding potential of the neuron. We used train stimuli with frequencies characteristic for responses of retinal ganglion cells to visual stimuli in vivo (Balkema & Pinto, 1982; Stone & Pinto, 1992). The response of the TC neurons to afferent stimulation is determined by several other factors beside the retinogeniculate synaptic input, like intrinsic conductances of the TC cell, inhibitory inputs, excitatory cortical feedback, and modulatory brainstem input (McCormick, 1992; Steriade et al. 1997). In the present study we were interested in properties of the retinogeniculate synaptic transmission, which is a basic factor in determining responses of TC neurons. We therefore used a preparation in which other inputs were eliminated or pharmacologically blocked. The separate NMDA and AMPA components of the retinogeniculate inputs were isolated pharmacologically. We found that the isolated NMDA component gave an increasing depolarization through temporal summation of EPSPs during train stimulation, despite the synaptic depression. This depolarization could provide sustained firing of the neuron with a frequency that depended on the holding potential. The isolated AMPA component was rather ineffective for spike generation. When the pulse train was delivered without immediately preceding synaptic input, the AMPA component could elicit short-latency spiking at the beginning of the train. However, when a few pulses of lower frequency, typical for maintained firing of retinal ganglion cells in vivo (Balkema & Pinto, 1982; Stone & Pinto, 1992), preceded this pulse train, sufficient depression was generated to abolish the initial spiking. Together with the depolarization evoked by the NMDA component, the AMPA component contributed significantly to spike generation, and the AMPA component was necessary for precise timing of the spikes with respect to the timing of the afferent pulses. The relationship between the degree of NMDA-R mediated sustained firing and the holding potential demonstrated that the degree of sustained response would be very sensitive for state-dependent regulations of the membrane potential of the TC neuron. We suggest that regulation of the sustained response through the level of the membrane potential is a key mechanism for regulation of the strength of input to cortex depending on states like arousal, attention and vigilance, a regulation that can be controlled from both cortex and the brainstem.
| Methods |
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4°C in artificial cerebrospinal fluid (ACSF) containing (mM): 125 NaCl, 25 NaHCO3, 2.5 KCl, 2 CaCl2, 1.25 NaH2PO4, 1 MgCl2, 25 D-glucose, and bubbled with 5% CO295% O2. Brain slices of LGN were cut from the block at a thickness of 250 µm, in a semiparasagittal plane, as previously described (Turner & Salt, 1998), using a vibroslicer (Sigmann Electronics, Hüffenhardt, Germany). The slices were stored submerged in ACSF at 30°C until recording, and were used within 4 h.
During experiments, slices were kept submerged in a small chamber (volume,
1.5 ml). The chamber was perfused with ACSF at the rate of 3 ml min1 at a temperature of 36°C using an inline heater. In all experiments picrotoxin (50 µM; Sigma-Aldrich, St Louis, MO, USA) was added to the perfusion solution to block GABAA synaptic inputs. CGP54626 hydrochloride (5 µM; Tocris Bioscience, Bristol, UK) was added to block GABAB effects elicited by repetitive stimulation of retinal afferents (Soltesz & Crunelli, 1992). A selective GABAC receptors antagonist was not added because in the feed-forward inhibitory loop, which could be activated by our stimulation of retinal afferents, all IPSPs seems to be blocked by GABAA and GABAB antagonists (Perreault et al. 2003; Blitz & Regehr, 2005). We added 2,3-dioxo-6-nitro-1,2,3,4-tetrahydrobenzo[f]quinoxaline-7-sulphonamine disodium salt (NBQX; 10 µM; Tocris Bioscience, Bristol, UK) and (RS)-3-2-carboxypiperazin-4-yl-propyl-1-phosphonic acid (CPP; 1015 µM; Tocris Bioscience, Bristol, UK) to the perfusion solution, as indicated, to block AMPA and NMDA receptors, respectively. We used NBQX to block AMPA-Rs. Although NBQX is a non-NMDA-R antagonist that blocks kainate receptors in addition to AMPA receptors (Sheardown et al. 1990), it has been shown that the non-NMDA receptors at the retinogeniculate synapses are of the AMPA type (Kielland & Heggelund, 2001; Chen et al. 2002).
Whole cell current-clamp recordings were made from TC neurons in LGN. The cells were visualized with differential interference contrast microscopy using infrared light. TC neurons were distinguished from local interneurons by their morphological (rounded soma and three or more primary dendrites; Zhu et al. 1999) and physiological characteristics (lower input resistance and shorter membrane time constant; Perreault et al. 2003). Recordings were obtained with borosilicate glass electrodes (46 M
) filled with (mM): 115 potassium gluconate, 20 KCl, 10 Hepes, 2MgCl2, 2 MgATP, 2 Na2ATP, 0.3 GTP. The pH was adjusted to 7.3 with KOH. In some of the experiments, as indicated, 2-[(2,6-dimethylphenol)amino]-N,N,N-trimethyl-2-ox-oethanaminium chloride (QX 222; 46 mM; Tocris Bioscience, Bristol, UK) was included in the intracellular solution to block Na+ action potentials. The electrical signals were amplified and low-pass filtered at 10 kHz with an Axoclamp 2A amplifier (Molecular Devices, Palo Alto, CA, USA) and Pulse software (HEKA Elektronik, Lambrecht, Germany). Bridge-balance circuitry was used to compensate for electrode resistance. Capacitance neutralization was used to compensate for membrane capacitance. Compensations and series resistances (< 20 M
) were checked periodically throughout the experiment. Data were digitized at 10 kHz with an ITC-18 interface (Instrutech, Port Washington, NY, USA).
Excitatory postsynaptic potentials (EPSPs) in TC neurons were evoked by electrical stimulation of retinogeniculate fibres with bipolar electrodes, using 100 µs-long current pulses. For each neuron the current strength was increased to a value (10200 µA) at which it evoked an action potential to a single pulse at a holding potential of 55 mV, and kept at this value throughout the recordings from a given neuron. Stimulus protocols were pulse trains of 10 pulses at 50, 80 or 100 Hz, which are in the range of spike firing of mouse retinal ganglion cells to visual stimuli in vivo (Balkema & Pinto, 1982; Stone & Pinto, 1992). The membrane potential of the neurons was adjusted to different steady state values in the range between 60 and 45 mV by constant current injection through the recording electrode. For each experimental condition, responses to 510 repetitive stimulus presentations were recorded with 20 s intervals between presentations (30 s for experiments with three-parted stimulus trains). Spike latency was calculated as time from stimulus pulse to peak of action potential.
Offline data analyses were made with Igor Pro (Wave Metrics, Lake Oswego, OR, USA). Statistical analyses were performed with Igor Pro and Statistica (StatSoft, Inc., Tulsa, OK, USA). Results are given as means ± S.E.M. The statistical difference between groups was determined using the Friedman ANOVA test.
| Results |
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(mean, m
= 198, S.D.
= 40.7 M
, n
= 42), and the time constant varied between 22.4 and 45.7 ms (m
= 32.9, S.D.
= 6.9 ms, n
= 42); values that are within the range for TC neurons (Perreault et al. 2003). The resting membrane potential of the cells in the control condition without afferent stimulation varied across cells from 68 to 55 mV (m
=
63.9 mV, S.D.
= 3.2, n
= 46). The membrane potential of the neurons was adjusted to different values in the range between 60 and 45 mV by constant current injection through the recording electrode. We studied changes of response patterns across these different holding potentials. Firing pattern at different holding potentials
The firing pattern to train stimulation changed with the setting of holding potential with respect to both the number of spikes and to which pulses in the train that elicited a spike. The typical variation of firing pattern is illustrated by the traces in Fig. 1. At 75 mV, as expected, the pattern was dominated by a short-latency low-threshold calcium potential, and the elicited action potentials lacked precise timing with respect to the single pulses in the stimulus train, consistent with previous findings (Blitz & Regehr, 2003). At normal resting potential (60 mV), only the first one to three pulses of the train generated a spike. At the more depolarized holding potentials, spikes were generated also in the later part of the train, with increasing number as the holding potential was shifted to more depolarized levels.
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To study the contribution of the AMPA component we blocked the NMDA-Rs by adding the selective antagonist CPP to the bath solution. At a holding potential of 50 mV, this abolished all spikes except those to the very first pulses of the train (Fig. 2B). To study the contribution of the NMDA component, we blocked AMPA-Rs by application of NBQX. This selectively abolished the spikes at the beginning of the stimulation with less marked effects on the number of spikes in the later part of the train (Fig. 2D). This is consistent with previous in vivo and in vitro experiments suggesting that the NMDA component is necessary for firing during the later parts of a stimulus (Salt, 1987; Hartveit & Heggelund, 1990; Heggelund & Hartveit, 1990; Funke et al. 1991; Zhang & Kelly, 2001; Blitz & Regehr, 2003).
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Temporal summation of EPSPs at different holding potentials
The firing patterns shown in Fig. 2 suggest that the temporal summation of EPSPs during the train stimulus is markedly different for the AMPA and NMDA components. We determined the temporal summation of EPSPs of the two components separately, and studied how they changed with variation of the holding potential. To determine the summation without distortions from action potentials and the subsequent after-hyperpolarization, we blocked the voltage-dependent sodium channels by adding QX222 to the intracellular solution (n = 27). The NMDA component was studied in 17 neurons, the AMPA component in 10 neurons.
The temporal summation of the EPSPs of the NMDA component gave gradually increasing depolarization during the stimulus trains at all holding potentials, despite the synaptic depression of the NMDA-R (Chen et al. 2002; Kielland & Heggelund, 2002). This is illustrated by the example in Fig. 3A. The black traces show the summation of the isolated NMDA component. The grey traces show the summation of EPSPs mediated by both AMPA and NMDA components in the control condition before wash-in of NBQX. Clearly, the single EPSPs elicited by the NMDA component had a relatively long duration compared with the interpulse intervals at 50 Hz. However, the increment of depolarization from one EPSP to the next decreased during the pulse train such that the sum gradually levelled out towards a plateau as expected from increasing synaptic depression during the pulse train. It is evident from the traces that the neuron would reach the threshold for spike firing at different parts of the pulse train depending on the underlying membrane potential.
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The depolarization elicited by the NMDA and AMPA components complemented each other, such that at the beginning of the train when the NMDA component was weak, the AMPA component was strong, and in the subsequent parts when the AMPA component declined, the NMDA component increased. Thus, the combination of the two components (grey traces in Fig. 3) provided strong depolarization throughout the pulse train.
For the neuron illustrated in Fig. 3A, the depolarization accumulated during the train by the NMDA component was largest at a holding potential of 60 mV, and decreased gradually as the holding potential was shifted to more depolarized level. However, this was not the case for all of the neurons tested (n = 10). For most of them the accumulated depolarization was about the same at all four holding potentials, as illustrated for three neurons in Fig. 4. However, the degree of accumulated depolarization at the end of the pulse train differed considerably from neuron to neuron in the range from 5.1 mV to 18.6 mV (m = 11.4 ± 0.6 mV).
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The rather large standard error at 60 mV could be due to a variable residual contribution of T-type calcium current that can occur at this membrane potential (Crunelli et al. 2005). This was confirmed for two neurons in which we found a minor reduction of the EPSP to the first pulse of the train in the control condition by application 0.5 mM Ni2+ (data not shown).
The finding that the increase of depolarization at the beginning of the response became faster at more depolarized holding potentials could be an effect of the non-linear voltage dependence of the NMDA-R. We therefore recorded NMDA-R mediated EPSPs to single stimulus pulses (n = 11). An example of traces from one neuron at the different holding potentials is shown in Fig. 5A. It shows that the rise time of the EPSP became faster with the more depolarized holding potentials. This corresponds to the increasing steepness of the initial response to the pulse trains, as described above. Moreover, the amplitude of the EPSPs increased as the holding potential was shifted to more depolarized levels despite the reduced driving potentials. This is consistent with the negative voltage dependence of the NMDA-R in this range of membrane potentials (Mayer et al. 1984; Nowak et al. 1984). The rise time determined from a single exponential fitted to the rising slope of the EPSPs, decreased from an average of 8.1 ± 0.5 ms at 60 mV to 4.9 ± 0.3 ms at 45 mV holding potential (P < 0.0001, d.f. = 3; n = 11). The amplitude of the EPSPs increased from an average of 5.3 ± 0.5 mV at 60 mV to 5.7 ± 0.6 mV at 45 mV holding potential (P < 0.008, d.f. = 3; n = 11).
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As illustrated in Figs 3A and 4, the increasing depolarization of the NMDA component during stimulus trains at 50 Hz was due to the long duration of the single EPSPs compared with the interpulse intervals. This suggests that the build-up of depolarization should be even stronger at shorter interpulse intervals. However, the synaptic depression of the NMDA-Rs increases with shortening of interpulse intervals, as well (Chen et al. 2002; Kielland & Heggelund, 2002) and this could counteract a stronger build-up of depolarization at higher stimulus frequencies.
Recordings of temporal summation of NMDA-R mediated EPSPs at different frequencies in the range of 50100 Hz demonstrated a substantial increase of depolarization with increasing stimulation frequency. This is shown for a representative neuron in Fig. 7A. The neuron was stimulated with trains at three different frequencies (50, 80 and 100 Hz) at a holding potential of 50 mV. Comparison of the depolarization developed by the NMDA component (black traces), and the combined contribution of this and the AMPA component (grey traces), shows that the NMDA component elicited the major depolarization at all frequencies. Moreover, the dominance of the NMDA component increased considerably with the increasing pulse frequency. Only at the beginning of the train, and in particular at the first pulse, did the AMPA component have a strong, dominant contribution. The average change in membrane potential generated by the NMDA component during the pulse train increased from 8.7 ± 0.8 mV at 50 Hz to 14.5 ± 1.7 mV at 100 Hz train stimulation (P < 0.003, d.f. = 2; n = 6) demonstrating that the summation of the EPSPs gave stronger depolarization at higher stimulus frequency despite the synaptic depression.
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Synaptic depression of the AMPA and NMDA components can be seen by comparing the size of the successive EPSPs in the traces in Figs 3, 4, 6 and 7 Quantitatively it was difficult to measure the magnitude of the depression for the NMDA component, because the amplitude of most EPSPs were still quite large when the next stimulus pulse was delivered. However, qualitative comparison of the traces for the AMPA and the NMDA components shows that the depression was stronger for the AMPA than for the NMDA component consistent with the fast desensitization of the AMPA-Rs (Chen et al. 2002; Kielland & Heggelund, 2002).
Firing pattern at different holding potentials
The temporal summation properties of the EPSPs of the AMPA and NMDA components, presented above, could explain the contributions of the two components to the firing patterns at the different holding potentials.
The typical firing pattern generated by the isolated NMDA component is illustrated by the traces in Fig. 8A. At 60 mV, the EPSPs showed the characteristic summation pattern for this component, but no spikes were elicited. As the holding potential was stepped up to more depolarized levels, spiking occurred first in the later parts of the train, and then also in the earlier parts. At the most depolarized holding potential (45 mV), the neuron fired spikes throughout the whole train. Thus, spike generation of the NMDA component is not limited to the later parts of a pulse train, but may occur even to the first pulse at sufficiently depolarized holding potentials. This was seen in all cells tested (n = 6). Clearly, the effect of the NMDA component on sustained spike firing will be highly sensitive to inputs from the brainstem or cortex that modulate the membrane potential of the neuron.
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To study the precision of spike timing with respect to timing of pulses in the train stimuli, we determined the latency of a spike from the nearest preceding pulse. Results for the NMDA and the AMPA component are presented in the histograms in Fig. 8A and B, respectively. Each histogram is based on the response to 10 stimulus presentations. The histograms in Fig. 8A present results for the isolated NMDA component. The results demonstrate that the blockade of AMPA-Rs eliminated the precisely timed spikes, and that the latencies of the elicited spikes were widely scattered. In the control condition at 50 mV (Fig. 8A, upper histogram with grey bars) the mean latency of the spikes was 4.2 ± 0.2 ms, and the coefficient of variation was 0.29. The latency at the same membrane potential for the isolated NMDA component had a mean of 9.8 ± 0.6 ms, and a variation coefficient of 0.49. There was no apparent change in the variability related to the holding potential. At 45 mV about the same mean latency (9.4 ms ± 0.4) and variation coefficient (0.41) was found despite the fact that at 45 mV the number of spikes was about the same as number of stimulus pulses. Similar results were obtained for all neurons tested with pulse trains at 50 Hz (n = 4). Tests with pulse trains of higher frequencies (80 and 100 Hz) also showed similar wide scatter of spike latencies as shown by the histograms in Fig. 9A and B. The results demonstrate that the single EPSPs mediated by the NMDA component did not trigger a precisely timed spike. Rather the level of depolarization built up by the temporal summation of this component generated a firing pattern in many respects similar to what is seen by a current step. This is illustrated in Fig. 9 where the firing patterns to an 80 Hz and a 100 Hz pulse train are compared to the firing pattern elicited by current steps through the recording electrodes. The response patterns to the train stimuli and to the current steps were characterized by the long latency from the start of the stimulus to the first spike, and a slightly accelerating firing rate.
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Role of the AMPA component in preserving precise spike timing at the synaptic relay
The role of the AMPA component in determining precise timing of spikes during the pulse train was not restricted to the spikes elicited by the first few stimulus pulses. This appears from the histograms in Fig. 8A by comparison of the distributions of spike latencies for the isolated NMDA component (histograms with black bars), with the distributions in the control condition when both AMPA and NMDA components were present (histogram with grey bars). The number of poorly timed spikes was considerably lower in the control condition than in the condition in which the AMPA-Rs were blocked. Accordingly, the AMPA component contributed to precise timing of the spikes even during the later part of the train, although the isolated AMPA component then was insufficient for spike generation. This is consistent with the interpretation that the NMDA component provides current that counteracts the rapid depression of the AMPA-Rs and keeps the neuron depolarized at a level closer to the threshold for action potential generation. When this level is high enough, the relatively weak but precisely timed EPSP of the AMPA component may be sufficient to trigger a spike, and thereby determine the precise timing of the spike.
Effects of frequency changes in the stimulus train
In the results presented above the stimulus trains were delivered without immediately preceding synaptic input. However, in vivo there is continuous synaptic input to TC neurons due to maintained activity in the retinal ganglion cells, and this presumably induces a sustained synaptic depression at the retinogeniculate synapses. Thus, when there is a sudden increase in the retinal input to a TC neuron in vivo, caused by for instance a visual stimulus flashed on its receptive field, the response is weakened by a sustained synaptic depression not present in our conditions with sudden onset of input. To study effects of preceding input activity on the response to pulse trains used in the experiments presented in the previous sections, we used (n = 10) a three-part stimulus train, the first part with 20 Hz pulses (typical frequency of maintained activity of retinal ganglion cells in vivo; Balkema & Pinto, 1982; Stone & Pinto, 1992), the second part with 50 Hz pulses, and the final part with 20 Hz pulses. The final part was introduced to observe after-effects of the 50 Hz train.
Effects of the immediately preceding input activity on the summation of EPSPs at different holding potentials are illustrated by results from two neurons in Fig. 10. Responses to the three-part stimulus train are shown by the black traces; the grey traces show control responses when only the 50 Hz train was given. Figure 10A shows results from a neuron for which the NMDA component was studied. The most pronounced effect of the preceding 20 Hz stimulation was the quite pronounced depolarization of the membrane potential during this first part of the three-part stimulus. However, we found no marked effects of the preceding stimulus pulses on the response to the 50 Hz train apart from a slightly increased depolarization to the first stimulus pulse. The response to the final 20 Hz pulses demonstrated a rather slow decay of the effects after the 50 Hz train. Figure 10B shows results from a neuron for which the AMPA component was studied. For this component the preceding 20 Hz stimulation induced a pronounced depression of the EPSP amplitudes at the beginning of the 50 Hz train, as predicted, and a fast decay of the effects after the 50 Hz train.
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| Discussion |
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TC neurons in LGN are normally influenced by many factors besides the glutamatergic input from retina that we studied, and one might ask to what extent our results apply to a more realistic in vivo situation. Other inputs modulate the activity pattern of the neurons in a state-dependent manner and change the firing pattern through GABAergic inputs. However, many of these influences, like most inputs from the brainstem, operate on a coarse time scale and exert their effects on various intrinsic conductances that induce relatively slow adjustments of the membrane potential (McCormick, 1992). The glutamatergic input from cortex seems, at least partly, to have similar effects. A single stimulus pulse to cortical afferents evokes just a minor EPSP in the TC neuron, but a train of pulses elicits EPSPs that summate to a more sustained depolarization (Lindström & Wróbel, 1990; Turner & Salt, 1998; von Krosigk et al. 1999). Intrinsic interneurons and neurons in the thalamic reticular nucleus, on the other hand, can sculpt the activity of TC neurons through fast GABAA inhibition. The interneurons generate a fast IPSP that follows the EPSP elicited by a spike in the retinal afferents (Lindström, 1982; Crunelli et al. 1987). This might slow down the build-up of depolarization through the NMDA component, but the degree of such slowdown could be rather limited since the duration of these IPSPs is considerably shorter than the duration of the NMDA-R mediated EPSPs. However, the interneurons and neurons in the thalamic reticular nucleus can provide inhibition also through GABAB receptors (Roy et al. 1984; Crunelli et al. 1988), and this could stop sustained firing and possibly induce burst firing in TC neurons by sufficiently long-lasting hyperpolarization (McCormick & Pape, 1990).
Responses of non-lagged TC neurons to an optimal visual stimulus flashed on the receptive field vary from predominantly transient to highly sustained. The transient/sustained behaviour is related to sleep states varying across non-REM sleep to drowsy or awake states (Coenen & Vendrik, 1972), and to changes in the EEG power spectrum from low frequency dominance to high frequency dominance (Funke & Eysel, 1992, 2000; Li et al. 1999). Several in vivo studies suggest that the sustained response is generated by the NMDA component of the sensory input (Salt, 1987; Hartveit & Heggelund, 1990; Heggelund & Hartveit, 1990; Funke et al. 1991; Zhang & Kelly, 2001), and the results from the present study suggest that the change to more sustained firing is caused by mechanisms that depolarize the neuron and bring the NMDA component of the retinal input toward the threshold for spike generation. Such changes in membrane potential might be elicited by several state-related mechanisms. The best characterized one is increased input from cholinergic and other activation related brainstem nuclei (Francesconi et al. 1988; Funke & Eysel, 1992; Humphrey & Saul, 1992; Funke et al. 1993; Hartveit & Heggelund, 1992, 1993, 1995; Hartveit et al. 1993; Fjeld et al. 2002) that depolarize TC neurons (Curró Dossi et al. 1991; Timofeev et al. 1996) by reducing the potassium current Ileak (McCormick & Pape, 1990; McCormick, 1992), in addition to other possible effects that might affect the amplitudes and temporal summation of EPSPs like membrane resistance and voltage-dependent conductances. The sustained depolarization of TC neurons generated by a pulse train in cortical afferents (Lindström & Wróbel, 1990; Turner & Salt, 1998; von Krosigk et al. 1999) may be an even more powerful mechanism for regulation of spike firing generated by the NMDA component.
State-dependent changes of response in TC neurons in LGN are usually related to a burst and a tonic mode, which are most clearly defined in vitro (Jahnsen & Llinas, 1984a,b; McCormick & Pape, 1990; McCormick, 1992). Burst mode occurs at membrane potentials hyperpolarized below about 60 mV and is characterized by rhythmic generation of low-threshold calcium bursts. Tonic mode occurs at depolarized membrane potentials above about 60 mV and is characterized by firing of single spikes. However, it is not clear how these two modes relate to responses of TC neurons to visual stimuli in vivo, and in particular, how they relate to the state-dependent changes from a mainly transient to a more sustained response to a visual spot stimulus. First, the in vivo studies were typically done by extracellular recording. Thus, the actual membrane potential of the neurons is unknown. Second, the transient-sustained changes are continuous (Funke & Eysel, 1992, 2000; Li et al. 1999) rather than being a shift between two discrete modes. Third, the visual response of TC neurons is basically similar to that of the retinal input and not considerably different as it would be if generated primarily by calcium bursts (Mastronarde, 1987a; Hartveit et al. 1993; Hartveit & Heggelund, 1995; Usrey et al. 1997; Fjeld et al. 2002). The response in TC neurons may be considerably weaker than the retinal input, particularly with respect to the sustained response component. The initial transient is generated in retina and is typically rather faithfully transferred to the LGN neuron (Hartveit et al. 1993; Hartveit & Heggelund, 1995; Fjeld et al. 2002). Following this transient there is typically at least some additional firing that is mainly single spike firing (e.g. Hubel & Wiesel, 1961; Coenen & Venderik, 1972). Even in conditions where the EEG power spectrum is dominated by low frequencies, there is some sustained firing (Coenen & Venderik, 1972; Livingstone & Hubel, 1981; Funke & Eysel, 2000), and this typically consists of single spikes rather than spike bursts (Coenen & Venderik, 1972; Livingstone & Hubel, 1981). Thus, the firing of TC neurons during optimal visual stimulation seems typically to occur in tonic mode. Possibly, the initial high-frequency transient response of the retinal input is sufficient to switch the neuron from a possible burst mode to the tonic mode. The changes we observed in the response to the train stimulation with variation of the holding potential, from just a few spikes at the beginning of the train to a more sustained firing throughout the train, occurred in a tonic mode. We suggest that the increasing sustained firing at more depolarized holding potentials, which shifted the NMDA component toward spike firing threshold, is related to in vivo changes along the transientsustained axis. This mechanism could play a key role in regulation of the impact of sensory input to cortex during different degrees of arousal, attention, and vigilance, and is a mechanism that can be controlled from both the brainstem and cortex.
Blitz & Regehr (2003) found that spikes at the beginning of a train stimulus are elicited by the AMPA component, whereas spikes in the later parts of the train are elicited by the NMDA component. Corresponding results have been found in other sensory nuclei (Salt, 1987; Zhang & Kelly, 2001). Other results have demonstrated that also early spike firing can be mediated by the NMDA component (Sanchez et al. 2007). The results of Blitz & Regehr (2003) were obtained at a holding potential of 55 mV. As shown by Fig. 8, we got similar results at this membrane potential. However, at more depolarized membrane potential, the NMDA component could elicit spikes throughout the pulse train, even to the first pulse in the train (Fig. 8A, 45 mV). This suggests that the apparent discrepancy between the previous studies could at least partly be due to a difference of membrane potential at which the firing pattern was studied. Moreover, we found strong stimulus induced depolarization mediated by the NMDA-Rs throughout the pulse train; even at the first pulse of the train. Thus, also at membrane potentials at which the NMDA component alone was insufficient to elicit early spikes, this component contributed with a substantial depolarization that together with the AMPA component could reach firing threshold.
The contribution of the NMDA component to retinogeniculate transmission in vivo is most likely even more pronounced than indicated by our data from responses to the pulse trains presented without immediately preceding synaptic input. Our data with the three-part stimulus train (Figs 10 and 11) demonstrated that stimulation with pulses in the frequency range of normal maintained firing of retinal ganglion cells in vivo immediately before a 50 Hz pulse train depressed the AMPA component to such extent that it failed to elicit spikes at all. This suggests that summation of AMPA-R and NMDA-R mediated EPSPs is necessary for spike generation even at the start of a sudden increase of retinal input, as presumably occurs at the onset of a visual stimulus. Moreover, the results from these experiments suggest that temporal summation of NMDA-R mediated EPSPs elicited by the maintained activity of retinal ganglion cells may generate a considerable depolarization of TC neurons that can contribute to keeping the neuron in a tonic mode.
Our results demonstrate that the latency of spikes elicited by the NMDA component was longer than the latency in the condition with both NMDA and AMPA components present, even in the condition when the NMDA component alone elicited a number of action potential equal to the number of pulses in the stimulus train (see histogram in Fig. 8 for 45 mV holding potential). This is consistent with the finding of Sanchez et al. (2007) for auditory responses in the inferior colliculus that the NMDA component is more important for spike generation in long-latency neurons than in short-latency neurons.
The lack of precise spike timing of the NMDA component combined with the precise spike timing of the AMPA component (Blitz & Regehr, 2003) does occasionally lead to a more irregular firing pattern including spike doublets (see the upper two traces in Fig. 1). In extracellular recordings such instances might be falsely regarded as burst related. However, the main result from our study concerning the combined effect of the AMPA and NMDA components on spike generation was a substantially increased fidelity of spike timing of the afferent input compared to the spike timing of the isolated NMDA component. This suggests that precise preservation of spike timing at the retinogeniculate relay (Mastronarde, 1987b; Reinagel & Reid, 2000, 2002) is due to an interplay between the AMPA and the NMDA components in which the NMDA component depolarizes the TC neuron toward the threshold for spike generation, and on top of that the typically small AMPA component may generate a precisely timed spikes. High preservation of timing at the retinogeniculate relay during visual stimulation in vivo was demonstrated by high cross-correlation of spike timing in pairs of non-lagged TC neurons and a connected retinal ganglion cell (Mastronarde, 1987b) suggesting that action potentials throughout the visual response are transmitted with preservation of precise timing. In lagged cells on the other hand, which have their functional input mediated through NMDA receptors (Heggelund & Hartveit, 1990), the cross-correlation was considerably lower (Mastronarde, 1987b). The preservation of precise spike timing may be essential for certain types of synaptic plasticity at the cortical level that is spike timing dependent (Schuett et al. 2001; Jacob et al. 2007).
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Blitz DM & Regehr WG (2003). Retinogeniculate synaptic properties controlling spike number and timing in relay neurons. J Neurophysiol 90, 24382450.
Blitz DM & Regehr WG (2005). Timing and specificity of feed-forward inhibition within the LGN. Neuron 45, 917928.[CrossRef][Medline]
Chen CF, Blitz DM & Regehr WG (2002). Contributions of receptor desensitization and saturation to plasticity at the retinogeniculate synapse. Neuron 33, 779788.[CrossRef][Medline]
Coenen AML & Vendrik AJH (1972). Determination of the transfer ratio of cat's geniculate neurons through quasi-intracellular recordings and the relation with the level of alertness. Exp Brain Res 14, 227242.[CrossRef][Medline]
Crunelli V, Haby M, Jassik-Gerschenfeld D, Leresche N & Pirchio M (1988). Cland K+-dependent inhibitory postsynaptic potentials evoked by interneurones of the rat lateral geniculate nucleus. J Physiol 399, 153176.
Crunelli V, Kelly JS, Leresche N & Pirchio M (1987). On the excitatory postsynaptic potential evoked by stimulation of the optic tract in the rat lateral geniculate-nucleus. J Physiol 384, 603618.
Crunelli V, Lightowler S & Pollard CE (1989). A T-type Ca2+ current underlies low-threshold Ca2+ potentials in cells of the cat and rat lateral geniculate nucleus. J Physiol 413, 543561.
Crunelli V, Tóth TI, Cope DW, Blethyn K & Hughes SW (2005). The window T-type calcium current in brain dynamics of different behavioural states. J Physiol 562, 121129.
Curró Dossi R, Paré D & Steriade M (1991). Short-lasting nicotinic and long-lasting muscarinic depolarizing responses of thalamocortical neurons to stimulation of mesopontine cholinergic nuclei. J Neurophysiol 65, 393406.
Deschênes M, Paradis M, Roy JP & Steriade M (1984). Electrophysiology of neurons of lateral thalamic nuclei in cat: resting properties and burst discharges. J Neurophys 51, 11961219.
Deschênes M, Roy JP & Steriade M (1982). Thalamic bursting mechanism, an inward slow current revealed by membrane hyperpolarization. Brain Res 239, 289293.[CrossRef][Medline]
Fjeld IT, Ruksenas O & Heggelund P (2002). Brainstem modulation of visual response properties of single cells in the dorsal lateral geniculate nucleus of cat. J Physiol 543, 541554.
Francesconi W, Müller CM & Singer W (1988). Cholinergic mechanisms in the reticular control of transmission in the cat lateral geniculate nucleus. J Neurophysiol 59, 16901718.
Funke K & Eysel UT (1992). EEG-dependent modulation of response dynamics of cat dLGN relay cells and the contribution of corticogeniculate feedback. Brain Res 573, 217227.[CrossRef][Medline]
Funke K & Eysel UT (2000). Quantitative aspects of the state-dependent co-variation of cat lateral geniculate and perigeniculate visual activity. Neuroreport 11, 10311037.[Medline]
Funke K, Eysel UT & Fitzgibbon T (1991). Retinogeniculate transmission by NMDA and non-NMDA receptors in the cat. Brain Res 547, 229238.[CrossRef][Medline]
Funke K, Pape H-C & Eysel UT (1993). Noradrenergic modulation of retinogeniculate transmission in the cat. J Physiol 463, 169191.
Hartveit E & Heggelund P (1990). Neurotransmitter receptors mediating excitatory input to cells in the cat lateral geniculate nucleus. II. Nonlagged cells. J Neurophysiol 63, 13611372.
Hartveit E & Heggelund P (1992). Brain-stem influence on visual response of lagged and nonlagged cells in the cat lateral geniculate nucleus. Vis Neurosci 10, 325339.
Hartveit E & Heggelund P (1993). The effect of acetylcholine on the visual response of lagged cells in the cat dorsal lateral geniculate nucleus. Exp Brain Res 95, 443449.[Medline]
Hartveit E & Heggelund P (1995). Brainstem modulation of signal transmission through the cat dorsal lateral geniculate nucleus. Exp Brain Res 103, 372384.[Medline]
Hartveit E, Ramberg SI & Heggelund P (1993). Brain stem modulation of spatial receptive field properties of single cells in the dorsal lateral geniculate nucleus of the cat. J Neurophysiol 70, 16441655.
Heggelund P & Hartveit E (1990). Neurotransmitter receptors mediating excitatory input to cells in the cat lateral geniculate nucleus. I. Lagged cells. J Neurophysiol 63, 13471360.
Hestrin S, Nicoll RA, Perkel DJ & Sah P (1990). Analysis of excitatory synaptic action in pyramidal cells using whole-cell recording from rat hippocampal slices. J Physiol 422, 203225.
Hirsch JC, Fourment A & Marc ME (1983). Sleep-related variations of membrane potential in the lateral geniculate body relay neurons of the cat. Brain Res 259, 308312.[CrossRef][Medline]
Hubel DH (1960). Single unit activity in lateral geniculate body and optic tract of unrestrained cats. J Physiol 150, 91104.
Hubel DH & Wiesel TN (1961). Integrative action in the cat's lateral geniculate body. J Physiol 155, 385398.
Humphrey AL & Saul AB (1992). Action of brain stem reticular afferents on lagged and nonlagged cells in the lateral geniculate nucleus. J Neurophysiol 68, 673691.
Jacob V, Brasier DJ, Erchova I, Feldman D & Shulz DE (2007). Spike timing-dependent synaptic depression in the in vivo barrel cortex of the rat. J Neurosci 27, 12711284.