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Coalescence of Sleep Rhythms and Their Chronology in Corticothalamic Networks

Mircea Steriade and Florin Amzica
Laboratoire de Neurophysiologie, Faculté de Médicine,
Université Laval, Quebec G1K 7P4, Canada
Abstract
The cellular substrates of sleep oscillations have recently been investigated by means of multi-site, intracellular and extracellular recordings under anesthesia, and these data have been validated during natural sleep in cats and humans. Although various rhythms occurring during the state of resting sleep (spindle, 7-14 Hz; delta, 1-4 Hz; and slow oscillation, <1 Hz) are conventionally described by using their different frequencies, they are coalesced within complex wave-sequences due to the synchronizing power of the cortically generated slow oscillation (main peak around 0.7 Hz). In intracellular recordings from anesthetized animals, the slow oscillation is characterized by a biphasic sequence consisting of a prolonged hyperpolarization and depolarization. Basically similar patterns are observed by means of extracellular discharges and/or field potentials in naturally sleeping animals and humans. The depolarizing component of the slow oscillation is transferred to the thalamus where it contributes to the synchronization of spindles over widespread territories. The association between the depolarizing component of the slow oscillation and the subsequent sequence of spindle waves forms what is termed the K-complex. The slow oscillation also groups cortically generated delta waves. At variance with previous assumptions that the brain lies for the most part in the dark and a global inhibition occurs in resting sleep, cortical cells are quite active in this behavioral state. This unexpectedly rich activity raises the possibility that, during sleep, the brain is occupied to specify/reorganize circuits and to consolidate memory traces acquired during wakefulness.

Current Claim: During quiescent sleep, low- and high-frequency thalamic and cortical rhythms are grouped into complex wave-sequences due to the depolarizing component of a cortically generated slow oscillation.




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This paper is an attempt at revising the current thinking on the generation and synchronization of various oscillations that define the state of resting (non-REM) sleep at the EEG level. We present three main points. (A) A novel slow oscillation, described in intracellular recordings from cortical and thalamic neurons (Steriade et al., 1993a, 1993c, 1993d), has the virtue of grouping other sleep rhythms, spindles and delta, into complex wave-sequences. The slow oscillation has a frequency of about 0.6 to 1 Hz in ketamine-anesthetized as well as naturally sleeping animals (Steriade et al., 1996a, 1996b) and humans (Steriade et al., 1993c; Achermann and Borbély, 1997; Amzica and Steriade, 1997a). Instead of considering different sleep oscillatory types as generated within isolated networks, we envision the cerebral cortex and thalamus as a unified oscillatory machine in which the depolarizing component of the cortically generated slow oscillation drives thalamic reticular (RE) and thalamocortical (TC) cells to produce spindles (7-14 Hz) and a clock-like component of delta waves (1-4 Hz). The generation of slow oscillation within the neocortex has been demonstrated by its survival in cortex after thalamectomy (Steriade et al., 1993d), its disruption by disconnection of intracortical synaptic linkages (Amzica and Steriade, 1995b), and its absence in the thalamus of decorticated animals (Timofeev and Steriade, 1996). However, in intact animals the slow oscillation is reflected in the thalamus by both RE and TC cells. This contributes to the grouping of thalamically generated oscillations (spindles and clock-like delta). (B) The combination of the excitatory component of the slow oscillation with spindles leads to the appearance of sleep K-complexes in both cats and humans (Amzica and Steriade, 1997a, 1997b). (C) The orderly appearance of various rhythms throughout the state of resting sleep, under the umbrella of the slow oscillation, is associated with a progressive increase in the corticothalamic coherence of sleep rhythms.
Why is it important to study the neuronal substrates underlying spontaneous brain rhythms even if their functional significance is far from being elucidated? Although different EEG oscillatory types were described by British and Eastern European investigators more than a century ago, their cellular bases have only been revealed during the past 10 to 15 years. Since the mid-1980s, the apparent chaos of EEG waves has been reduced to a few basic cellular operations that shed light on the origin and mechanisms generating various EEG grapho-elements. Our reductionistic attempt provides explanations of the mechanisms underlying brain rhythms and may ultimately shed light on the functional role played by these oscillations. To give just one example: some still describe different types of EEG sleep spindles, with lower or higher frequencies, while intracellular data allow us to understand that these supposedly different types are attributable to a single event, namely, the duration of hyperpolarization-rebound sequence in TC neurons. The hyperpolarization de-inactivates a low-threshold Ca2+-mediated current, underlying postinihibitory rebound spike-bursts that are transferred to cortical areas (Steriade and Llinás, 1988). If the hyperpolarization is of about 70 msec, the spindle frequency is about 14-15 Hz; if the hyperpolarization is longer because its progenitors, GABAergic RE neurons, fire longer spike-bursts, the frequency is lower. Understanding that the spindle oscillation is due to rhythmic inhibitory postsynaptic potentials (IPSPs) generated by RE neurons (Steriade et al., 1985; Bal et al., 1995) may explain one of their functional roles, which is the blockade of synaptic transmission through the thalamus (Steriade et al., 1969; Timofeev et al., 1996), thus deafferenting the cortex from the outside world and allowing a peaceful sleep. Similar examples may be taken from the study of other brain oscillations defining resting sleep.

The aim of the present paper is to reveal the cellular substrates of sleep oscillations and to propose some avenues to understand their functions.



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Data reported in this paper result from intracellular recordings (in some cases dual simultaneous impalements of cortical neurons or cortical and thalamic neurons) in conjunction with multi-site extracellular recordings in acutely prepared cats under different types of anesthesia (mainly ketamine-xylazine) or from multi-site extracellular recordings during natural wake and sleep states in chronically implanted cats (see technical details in Steriade et al., 1996a, 1996b). The intrinsic properties and input-output organization of different cortical and thalamic neuronal types were defined by standard electrophysiological procedures (depolarizing and hyperpolarizing current pulses at different levels of membrane potential - Vm, antidromic and orthodromic responses) and the morphological features of recorded neurons were known by intracellular staining with Lucifer yellow or Neurobiotin (see Steriade et al., 1993c; Contreras and Steriade, 1995). The results from intracellular recordings are based on neurons with resting Vm more negative than -55 mV and overshooting action potentials. Different analyses used to assess the synchronization processes were cross-correlograms, measures of synchrony coefficient, wave-triggered excitatory postsynaptic potentials (EPSPs), spike-triggered-averages, first-spike-analysis, and sequential field correlations as visualized by three-dimensional surfaces and contour maps (see Steriade and Amzica, 1994; Amzica and Steriade, 1995a, 1995b).


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Figure 7
Coalescence of three types of sleep rhythms grouped by the cortical slow oscillation
For didactic purposes, three types of oscillations are usually described as characterizing the state of resting sleep: spindles (7-14 Hz), delta (1-4 Hz) and slow oscillation (below 1 Hz, usually 0.6 to 1 Hz). However, in brain-intact animals and humans, the sleep oscillations are not seen in isolation but they are grouped by the recently discovered slow oscillation. Figure 1 shows that the intracellularly recorded slow oscillation (0.8-0.9 Hz) progressively develops in conjunction with the increased synchronization of EEG field potentials. This development is associated with steeper slopes of both depolarizing and hyperpolarizing components of the slow oscillation (compare 1 to 2 in bottom panels). The depolarizing components of the slow oscillation, reflected as a sharp depth-negative field potential (Figs. 1 and 2A), give rise to corticothalamic volleys that, by driving thalamic neurons, induce brief sequences of spindle waves consisting of rhythmic IPSPs in TC cells. The amplitudes of spindle-related IPSPs in TC cells, which increase under steady depolarization (Fig. 2B), are induced by spike-bursts in GABAergic RE cells that, in turn, are driven by the depolarizing component of the cortical slow oscillation (Steriade et al., 1993a; Contreras and Steriade, 1995). Distinctly from the waxing-and-waning pattern of spindle oscillations in the decorticated animals or under barbiturate anesthesia when cortical neurons display reduced spontaneous activities, the spindles triggered by the corticothalamic volley of the slow oscillation under ketamine-xylazine anesthesia are shorter and display an exclusively waning pattern (Fig. 2A-B). This is due to the fact that the synchronous excitation of corticothalamic neurons during the slow oscillation entrain, right from the start, a great population of neurons implicated in the genesis of spindles within a thalamic territory, thus explaining the absence of an initial waxing process (Contreras and Steriade, 1996).
The coalescence of the slow and spindle oscillations is especially visible during light sleep. The evolution of sleep rhythms, with their progressively increased amplitudes from the end of waking state toward the end of deep resting sleep, is illustrated by means of multi-site recordings in Fig. 3 which shows that, in naturally sleeping animals, the slow oscillation dominates brain electrical activity throughout the state of resting sleep. During light sleep, every cycle of the slow oscillation generally leads to a sequence of spindle waves, on one, another, or all cortical leads. As shown above (Fig. 2), this is due to the synaptic engagement of thalamic neurons implicated in spindle genesis. Notably, though deep sleep displays less spindles, toward the end of deep sleep, just before EEG activation occurs in REM sleep, spindles recover their power, as during the initial stages of resting sleep (Fig. 3). This can be explained by the voltage-dependency of sleep rhythms in TC cells. Indeed, at the single-cell level, spindles occur at the resting Vm of TC neurons, whereas, at more hyperpolarized levels, spindles are progressively replaced by intrinsically generated, clock-like delta potentials (Steriade et al., 1991; Nuñez et al., 1992). These intracellular data from anesthetized preparations found support in results obtained in naturally sleeping animals, showing that thalamic spindles are maximal at sleep onset and decrease thereafter, whereas thalamic delta waves increase gradually during resting sleep (Lancel et al., 1992). Thus, with increasing hyperpolarization of TC cells during resting sleep, due to the progressive diminished firing rates of cholinergic and other types of brainstem-thalamic activating neurons (reviewed in Steriade and McCarley, 1990), the incidence and amplitude of spindles are largely diminished during deep sleep stages. On the other hand, the reappearance of spindles toward the end of resting sleep (see Fig. 3) is attributable to a relative depolarization of TC cells, due to the increased firing rates of brainstem-thalamic reticular neurons that display precursor-increased rates of spontaneous firing, 30 to 60 s before the onset of REM sleep (Steriade et al., 1990).

Spindling is not the only sleep rhythm that is modulated and grouped by the cortical slow oscillation. (A) The intrinsically generated delta rhythm of TC cells is influenced by the slow oscillation because the rhythmic depolarizing corticothalamic drives increase the membrane conductance of TC cells and prevent the interplay between a hyperpolarization-activated cation current (Ih) and a calcium current de-inactivated by membrane hyperpolarization (It), thus periodically dampening the slow oscillation (see Fig. 10A in Steriade et al., 1993a; and Box 1 in Steriade et al., 1994). However, as corticothalamic volleys also drive GABAergic RE neurons, singly delta-oscillating TC cells may be synchronized because RE cells set their Vm at the adequate level where delta rhythm is generated (Steriade et al., 1991). (B) The other component of delta waves, that is generated intracortically after thalamectomy (see above), has not yet been systematically studied at the intracellular level to shed light on its neuronal substrate(s). One possibility is that the frequency band of 1-4 Hz in the power spectrum during late stages of resting sleep results, at least partially, from the shape of the depth-negative (depolarizing) component of the slow oscillation (0.3-0.4 s), which represents the K-complex (Amzica and Steriade, 1997a, 1997b). Anyway, typical delta waves, at a frequency of 2-4 Hz, generated by both regular-spiking and intrinsically bursting cortical neurons, are grouped within sequences recurring with the slow rhythm (see Fig. 3 in Steriade et al., 1993d). And, in human sleep EEG, sequential mean amplitudes of delta waves show their periodic recurrence with the rhythm of slow oscillation (Steriade et al., 1993c). That delta and slow oscillation represent two distinct phenomena was recently demonstrated by Achermann and Borbély (1997) who showed differences in the dynamics between the slow and the delta oscillations, as the latter declines in activity from the first to the second non-REM sleep episode, whereas the former does not. The current confusion in the literature between delta oscillation and delta waves is probably due to the fact that the presence of a peak in power spectrum may result from an oscillation with the frequency of the peak and/or a frequent occurrence of waves with a duration and shape that would contribute to that particular peak.

We investigated the synchronization of slow oscillation in naturally sleeping animals by using the wavelet procedure that detects waveforms similar in shape with a preset pattern. Thus, the original EEG trace is digitally filtered and tranformed into a new time series (signal) that conserves from the original only the relevant wavelets (Amzica and Steriade, 1997a). In order to match K-complexes (see below), we used Daubechies' wavelets (Daubechies, 1988). Figure 4 shows that the intracortical as well as corticothalamic synchronization of the slow oscillation is most obvious during deep sleep and is best expressed among areas across the same gyrus (areas 5 and 7) or among cortical areas and related thalamic nuclei (area 7 and rostral intralaminar nuclei). However, synchronization is also seen between morphologically distant and functionally different cortical fields (motor area 4 and visual area 18).

Finally, because the slow oscillation was first described intracellularly under different anesthetics, we had to validate the similarity of these cellular patterns to those observed extracellularly in chronically implanted, unanesthetized animals. Under both ketamine-xylazine anesthesia and natural sleep, the slow oscillation has a frequency of 0.6 to 1 Hz (Fig. 5A-B). Under anesthesia, the field potentials associated with this oscillation are prolonged depth-positive (hyperpolarizing) and depth-negative (depolarizing) components (Fig. 5A). Similar aspects are observed in natural resting sleep, when the depth-positive waves are accompanied by silenced firing, while depth-negative sharp deflections are associated with brisk firing (Fig. 5B). Surprisingly, because fast oscillations (generally 20-50 Hz) are conventionally associated with brain-activated states, similar fast oscillations also appear during resting sleep but are selectively obliterated during the depth-positive component of the slow oscillation (see inset in Fig. 5B). This demonstrates the voltage(depolarization)-dependency of fast oscillations.


The slow oscillation and K-complexes in human sleep
After preliminary data showing the presence of slow oscillation during natural sleep in humans (Steriade et al., 1993c), the human slow oscillation (<1 Hz) was recently reported in parallel studies from two laboratories (Achermann and Borbély, 1997; Amzica and Steriade, 1997a). Here, we document different aspects of the human slow sleep oscillation. (A) During stage 2, scalp recordings show a prevalent peak (0.8 Hz) within the frequency range of the slow oscillation as well as a minor mode around 15 Hz reflecting spindle waves (Fig. 6). The depth-negative components of the slow oscillation, followed or not by spindles, represent the K-complexes (bottom panels in Fig. 6). The frequency of K-complexes (peaks at 0.5 Hz in stage 2, 0.7 Hz in stages 3-4 of human sleep) is very similar, up to identity, to the frequency of the slow oscillation during natural sleep (see Fig. 2C in Amzica and Steriade, 1997a). (B) The power spectrum reveals a major peak around 1 Hz, that becomes evident from stage 2 and continues throughout resting sleep (top panel in Fig. 7). The slow oscillation is particularly abundant in fronto-parietal leads (bottom panel in Fig. 7).

These data invite human sleep researchers to consider the two types of oscillatory activities below 4 Hz (delta, 1-4 Hz; slow, <1 Hz) and, accordingly, to analyze their results by taking into account the distinctness of these two oscillations, as demonstrated by Achermann and Borbély (1997; see above).



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Figure 7
Cellular mechanisms of sleep oscillations
Sequences of spindle waves, recurring with a slow rhythm at about 0.3-0.5 Hz, occur during early sleep stages and are generated by interactions between RE and TC neurons (Steriade et al., 1993b; Bal et al., 1995). The pacemaking role of RE neurons was shown by abolition of spindles in TC systems after disconnection from RE nucleus (Steriade et al., 1985) and by preservation of spindles in the deafferented rostral pole of the RE nucleus (Steriade et al., 1987). Although spindles are generated in the thalamus after decortication (Morison and Bassett, 1945), corticothalamic volleys are important in triggering and synchronizing spindles throughout TC systems (Steriade et al., 1972; Contreras et al., 1996a, 1997).
Delta waves, usually regarded as a single type of EEG waves, consist of two components. The cortical one survives thalamectomy (Villablanca, 1974; Steriade et al., 1993d). The thalamic-generated delta oscillation is present after decortication (Curró Dossi et al., 1992), is stereotyped and clock-like, and its intrinsic-cell nature is due to the interplay of two hyperpolarization-activated currents of TC neurons, Ih and It (McCormick and Pape, 1990; Soltesz et al., 1991).

The basic features of the recently described slow oscillation (see Introduction) consist of a prolonged hyperpolarization (up to 1 s), associated with a depth-positive (surface-negative) EEG wave, followed by a long-lasting depolarization (up to 0.8 s), associated with a depth-negative (surface-positive) field potential. These sequences recur periodically, with a rhythm of 0.6 to 1 Hz. The long-lasting depolarization consists of EPSPs, fast prepotentials (FPPs) and fast IPSPs reflecting the action of synaptically coupled GABAergic local-circuit cells; in addition, the depolarizing component is made up of both NMDA-mediated synaptic excitatory events and a voltage-dependent persistent Na+ current, as the depolarizing envelope is shortened by adminstration of ketamine, an NMDA blocker, or intracellular injection of QX-314, a blocker of Na+ currents (Steriade et al., 1993c). The prolonged hyperpolarization results from a series of factors; among them, disfacilitation in cortical networks is probably the most important (Contreras et al., 1996b).


Possible significance of sleep rhythms
The frenzied activity of cortical neurons during the slow oscillation, occurring in natural sleep or deep anesthesia (see Figs. 1 and 5) during which consciousness is conventionally thought to be annihilated, prompts us to consider different roles played by the rhythmic bombardment of thalamic and cortical neurons upon their targets. Indeed, the deafferentation of thalamocortical networks produced by the spindle-related IPSPs in TC cells, with the consequence of obliterating incoming messages and thus disconnecting the brain from the outside world, is probably not the only effect of sleep oscillations. To begin with, whereas TC cells do not transmit ascending afferent signals to cortex during the hyperpolarizing phase of the slow oscillation because the EPSPs do not reach firing threshold, the internal dialogue of the brain (as tested by corticocortical and corticothalamic volleys) is not disrupted during this hyperpolarizing phase (Timofeev et al., 1996). The preservation, during resting sleep, of this form of internal communication is reminiscent of earlier data showing that callosally evoked discharges in precentral neurons of behaving monkeys are not diminished from waking to resting sleep and may even be enhanced (Steriade et al., 1974).

The state of resting sleep may subserve even more noble functions during different oscillatory activities of thalamic and cortical neurons. Rhythmic activation of cortical neurons, produced by repetitive spike-bursts of TC cells during sleep spindles, are hypothesized to reinforce and/or specify the circuitry, to stimulate dendrites to grow more spines, and to contribute to the consolidation of memory traces acquired during wakefulness (Steriade et al., 1993a). The idea of such plastic changes may be tested by using procedures of cellular conditioning and by lesioning different structures implicated in the production of sleep oscillations. For example, the effects of abolishing spindles in a hemisphere, after chemical lesioning of the RE nucleus (Steriade et al., 1985), may be investigated upon the time required for establishing conditioned responses in the ipsilateral cortex devoid of spindles. That spindles and their artificial model, augmenting responses evoked by low-frequency (10 Hz) repetitive volleys, are able to produce short-term plasticity was demonstrated even in the thalamus of decorticated animals (Steriade and Timofeev, 1997). In these experiments, intrathalamic stimulation at 10 Hz produced a progressive and persistent increase in slow depolarizing responses of TC cells, as well as to a persistent and prolonged decrease in the amplitudes of the IPSPs. Even more pronounced plastic changes are expected to occur with augmenting responses in an animal with intact cortex (Morison and Dempsey, 1943; Morin and Steriade, 1981; Castro-Alamancos and Connors, 1996) since augmenting does not lead to prolonged paroxysmal developments in decorticated animals but such transformations can occur in the presence of intact thalamocorticothalamic loops (unpublished data). After a series of repetitive responses in bursting thalamic neurons, evoked by cortical volleys at 10 Hz, the neurons spontaneously produced spike-bursts very similar to the shape and frequencies of those evoked stimuli (see Fig. 7 in Steriade, 1991). The "memory" of the circuit, presumably due to resonant frequencies in the thalamus and neocortex, may eventually lead to paroxysmal events, consisting of spike-wave seizures at 2-4 Hz (Steriade et al., 1976).

Thus, synapses within intracortical and thalamocortical circuits may be thought of as dynamically stabilized by internally generated, apparently "non-utilitarian" excitations during sleep oscillations (see Kavanau, 1994). The "rehearsal", in resting sleep, of information acquired during active behavior (Buzsáki, 1989; Wilson and McNaughton, 1994) is also revealed by the persistence, during periods of subsequent sleep, of intracortical and corticothalamic synchrony of fast (gamma) oscillations acquired during conditioning sessions (Amzica et al., 1997). All these data suggest that the re-expression of information during sleep may be related to memory consolidation.



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This work was supported by grants from the Medical Research Council of Canada and Human Frontier Science Program. F. Amzica is a postdoctoral fellow, partially supported by Fonds de Recherche en Santé du Québec. We thank D. Contreras and I. Timofeev for their collaboration in some unpublished experiments.


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