Abstract
Brain injury profoundly affects global brain dynamics, and these changes are manifest in the electroencephalogram (EEG). Despite the heterogeneity of injury mechanisms and the modularity of brain function, there is a commonality of dynamical features that characterize the EEG along the gamut from coma to recovery. After severest injury, EEG activity is concentrated below 1 Hz. In minimally conscious state during wakefulness, there is a peak of activity in the 3–7 Hz range, often coherent across the brain, and often also activity in the beta (15–30 Hz) range. These spectral changes likely result from varying degrees of functional deafferentation at thalamic and cortical levels. EEG-based indices of brain dynamics that go beyond these simple spectral measures may provide further diagnostic information and physiologic insights.
Keywords: Brain injury, vegetative state, minimally conscious state, deafferentation, electroencephalography, spectral analysis
INTRODUCTION
Patients who survive severe brain injury are often left with a chronic disturbance of consciousness. The consequent suffering and disability has a major impact on the individual patient and their family. The aggregate burden to society is accentuated by two factors: traumatic brain injury primarily affects young people, and ongoing improvements in medical intensive care have increased survival rates, especially after very severe injuries. Over the last decade, it has become increasingly evident that even with a severe initial deficit, the outlook is not hopeless: many patients have a spontaneous late recovery (even after many years), and some treatment options show promise. Improved understanding of the physiologic basis and phenomenology of these disturbances therefore is crucial: to provide accurate diagnosis and prognostication, and to guide and assess potential treatments.
Determination of consciousness requires more than behavioral observation
In severe brain injury, making even basic diagnostic distinctions is challenging. The critical distinction between the vegetative state (VS) and the minimally conscious state (MCS) is the presence of at least some elements of consciousness, even if inconsistent (see Box 1 for definitions and characteristics of these states and related entities). Reliance on clinical observations to identify elements of consciousness is questionable[1] : it presumes an intact motor system, but severe damage to the motor system (or motor disability consequent to prolonged immobility) is common in this population. This puts a premium on methods of assessing brain function that do not rely on motor output [2–5].
One such approach is functional imaging. Functional magnetic resonance imaging (fMRI) studies have demonstrated that some VS and MCS patients can generate complex activations consistent with motor imagery, and even communicate via such signals [2,3,6], despite a lack of verbal or gestural communication systems. Translation of such methods to the electroencephalogram (EEG) has demonstrated that brain signals linked to motor imagery can be measured in brain-injured subjects using this modality as well [4]. However, fMRI and EEG measurements carried out over short periods of time are of limited value in patients with severe brain injuries, because of their marked and frequent fluctuations in state. Because of such state fluctuations, evidence of cognitive responses may be present at one time, and not at another [4]. Moreover, statistical methods that do not take state fluctuations of background activity into account may lead to false positive findings in EEG assessments of severely brain-injured subjects [7].
These considerations motivate augmenting behavioral observation with direct measures of brain activity that allow not only for assessment of interaction with the environment, but also of state and state fluctuations. The EEG is a particularly attractive modality for this purpose: it is non-invasive, it is relatively inexpensive, it allows for repeated or extended measurements at the bedside, and it can resolve dynamics at the timescale of neuronal activity. (For a comprehensive introduction to EEG, see [8]) Our review therefore focuses on EEG measures of brain activity, and an emerging framework for linking these measures to the neurophysiology of the normal and injured brain.
Why focus on global dynamics?
Since many cognitive and behavioral functions are modular and localized, an emphasis on global dynamics might at first seem puzzling. Our reasons for this focus are twofold. First, although brain injury often affects modular functions, these effects often depend idiosyncratically on the specific injury pattern (e.g., the vascular territory involved, or the location of the traumatic injury). In contrast, the effects of brain injury on arousal and attentional modulation are pervasive and general, and, as we suggest below, are likely to have an underlying pathophysiology that is independent of the mode or details of the injury. The second reason is that global deficits are arguably more significant for functional recovery: preservation of specific modular functions in the absence of intact arousal mechanisms is a devastating injury [9], while loss of a modular function may be susceptible to remediation via prosthetics and functional substitution.
A perspective on EEG analysis
As a measure of brain dynamics, the EEG is in some sense an embarrassment of riches: typical recordings provide signals with a bandwidth ranging over a broad frequency range (e.g., 1 Hz to 70 Hz), recorded at dozens or even hundreds of scalp locations, over a period of minutes to hours. Reducing these high-dimensional datasets to a small number of meaningful quantities is a critical challenge. The challenge is exacerbated by the presence of non-stationarities (i.e., the state changes mentioned above) and the many environmental and physiologic artifacts that contaminate clinical recordings – and the possibility that state changes and artifacts may be interrelated.
While there is no simple solution, we would like to suggest a set of guidelines. First, for identification of state changes and artifact, it is essential to inspect the raw signal itself, along with video images of the patient. Second, for dimensional reduction, there is an advantage to approaches that have only minimal dependence on specific physiologic models, and well-characterized statistical properties – spectral analysis (Fig. 1A) is a prime example [10–12], as we illustrate below. Finally, while statistical vetting is a necessity, such validation can be highly dependent on the statistical model [7]. Therefore, a physiologic or mechanistic interpretation of EEG observables provides important reassurance that a set of inferences is based on more than a chance association. With these considerations, this article reviews not just the phenomenology of EEG dynamics in the injured brain, but also summarizes current thinking about mechanism.
LARGE-SCALE EEG DYNAMICS IN STRUCTURAL BRAIN INJURIES
We begin by considering the phenomenology of global EEG dynamics in the severely injured brain that characterize and differentiate the states along the gamut from coma to normal function. We focus on the power spectrum and related measures[10–12], as this enables a link to the likely pathophysiological underpinnings, which we then describe. Finally, we consider other quantitative indices derived from the EEG that show promise as probes of global dynamics in severe brain injury.
Phenomenology
Although a wide variety of EEG patterns may appear with structural brain injuries and even in normal wake and sleep states, broad regularities are readily identifiable, particularly at the extremes of very severe injury and normal brain function [8,13]. Figure 1B illustrates typical EEG power spectra obtained from human subjects in coma, MCS, and normal wakefulness. In coma (Figure 1B1), power is concentrated at very low (<1Hz) frequencies; above 3 Hz, there is a gradual and nearly featureless decline. This example, taken from a patient in VS following a very severe anoxic injury, is representative of all EEG channels in this subject. Such power spectra (power concentrated below 1 Hz, and uniform across the scalp) are characteristic of patients with the most severe forms of structural injuries produced by trauma, hypoxia or other causes.
In contrast, an example EEG power spectrum during normal wakefulness contains a complex mix of frequencies (Figure 1B3). As is typical of the normal EEG power spectrum, there are peaks in the alpha band (8–12 Hz) and the beta band (15–30Hz). The relative and absolute sizes of these peaks normally vary with location (with alpha being more prominent over parietal and occipital areas, and beta more prominent over frontal areas), and also across subjects. Figure 1A1 is another example, in which the alpha peak is more prominent and the beta activity is nearly absent.
The EEG power spectrum in MCS following severe structural brain injury (Figure 1A2, 1B2, 1C1 left) reveals a third pattern: a strong peak in the theta (4–7 Hz) range, usually near 7 Hz (as in this example) but occasionally as low as 3 Hz, and present diffusely over the scalp. While theta rhythms can be present in normal subjects, they occur only in specific circumstances: either transiently in the frontal midline during effortful cognition, or more broadly over frontocentral EEG channels during drowsiness [8]. The diffuse spatial distribution of the theta rhythm in Figure 1B2, along with its presence during wakefulness, identify it as pathologic pattern, characteristic of MCS patients ([14],Forgacs et al., abstract, Society for Neuroscience, San Diego, November 2013).
Pathophysiologic mechanisms
Converging evidence from physiological and clinical studies suggests a linkage between the alterations in EEG dynamics seen in Figure 1B, along with other characteristic features of the EEG in severe brain injury, and the consequences of varying degrees of deafferentation and disconnection.
Low-frequency activity
The concentration of power below 1 Hz seen in VS (Figure 1B3) likely reflects total deafferentation of the cortex. Such slow oscillations are known to arise in two very different scenarios: total anatomical deafferentation in the feline `slab' model, in which all long-range white matters to a cortical region are transected [15], and the total functional deafferentation of deep anesthesia[16]. Similar patterns of slow oscillations are present in two other circumstances characterized by severe functional deafferentation: across structurally intact frontal-parietal cortices during temporal lobe seizures[17,18], and during normal slow-wave sleep, in which functional deafferentation results from disfacilitation of neocortical neurons[19].
Although sleep and anesthesia share some features, they are very distinct in origin and mechanism. A much closer functional relationship exists, however, between anesthesia and the altered consciousness produced by brain injuries[20]. Because anesthesia is readily controlled, it provides for unique insights into the physiologic processes underlying global brain dynamics.
Within the context of anesthetic coma induced by propofol, the slow oscillation has recently been the subject of a detailed study that included multi-unit recordings from humans[21]. This work revealed unexpected local and global dynamical structure in neuronal firing patterns within each slow oscillation of the EEG. Specifically, at a scale of <4mm, neuronal populations can show spiking activity that fluctuates between silence and rates typically encountered during wakefulness. These fluctuations are sharply gated by the slow oscillation. Moreover, they appear asynchronously across the cortex, suggesting functional isolation.
Propofol anesthesia is also associated with another dynamical feature: a spectral power peak centered at ~11Hz over frontocentral EEG channels, that is coherent (i.e., synchronous) across the brain [22]. Computational modeling suggests that this rhythm may arise via a dual mechanism that silences the typical dominant posterior ~10Hz (alpha) rhythm of normal wakefulness and produces an `anteriorized' alpha-range oscillation via thalamic nuclei projecting to the frontal lobe [23].
Recent work [24] indicates that these dynamics seen in propofol anesthesia underlie another pathologic EEG pattern seen in coma, namely, burst suppression. The burst suppression pattern, seen in patients with severe structural or anoxic brain injury, consists of alternation between periods of electrical silence and periods of apparently irregular high-voltage activity, each lasting several seconds. Ching et al. [24] showed that the spectral characteristics of the bursts match those of propofol-associated activity, namely, a globally coherent oscillation at ~11 Hz along with slow wave oscillations that are asynchronous across the brain [25]. The electrically silent periods that alternate with this activity appear to be linked to failure of ATP production across populations of neurons [24].
Theta-range activity
In states that are intermediate between that of coma and normal wakefulness, a variety of spectral features are observed. The most common is a peak in theta power (Figure 1A2, 1B2, 1C1 left), which has been identified in patients with both global (S Williams et al, [14]) and focal [26] structural brain injuries, and is characteristic of MCS during wakefulness.
Two mechanisms are known to be capable of producing strong power in the theta range after severe or moderate deafferentation at the level of the neocortex and thalamus. The first is cellular: in the setting of deafferentation present in neocortical slice preparations, layer V pyramidal cells have intrinsic membrane oscillations at approximately 7 Hz. The second is circuit-based: deafferentation of the thalamus from its cortical inputs leads to bursting in the wakeful state [27] and increased theta power in the EEG [28,29]. These mechanisms have distinguishing characteristics. The circuit mechanism is likely to be associated with a lesser degree of deafferentation, and the thalamic bursting component is expected to produce 15–30Hz (beta) power in the EEG. In the cellular mechanism, likely to be operative in the presence of more severe deafferentation, weak coupling of intrinsically oscillating neurons is expected to produce long-range synchronization of theta activity [30] manifest in a theta-range peak in coherence (as in Figure 1C1 right). The presence of theta-range as well as beta-range peaks in the examples of Figure 1A2 and 1B2 suggests a contribution from both mechanisms.
Models
The power spectral features that are present in the normal wake and sleep EEG can be captured by mathematical and computational models. Neural mass models [31–36] are especially appropriate for this purpose, as they seek to account for overall qualitative features of EEG dynamics without requiring fine-grained anatomical detail, but approaches postulating specific neuronal connectivities [24] have also proven successful.
Neural mass models can form the basis of both for “forward” and “inverse” approaches. In forward approaches, models are constructed based on a simplified description of brain connectivity, and the analytic behavior of the model is investigated to determine whether this caricature provides a useful framework for understanding brain dynamics. The simplification may consist of a continuum approximation to the whole brain [37], or, models that emphasize the connectivities of specific brain areas or populations. The series of models developed by Robinson and colleagues[34]exemplifies the latter approach: it focuses on the interactions of four populations: corticothalamic layer V neurons, cortical inhibitory neurons, thalamic reticular neurons, and thalamic relay neurons. With each of these populations modeled as separate “masses,” the model accounts for the typical spectral power distributions found in normal wakefulness, the sleep stages, theta-dominated drowsiness and burst suppression, and in addition accounts for the spatial coherence structure of the normal EEG during wakefulness[38]. These models thus serve as a foundation for formalizing the linkage between the physiology of neuronal populations and the dynamics that can be observed in the EEG.
Building on the Robinson framework, Drover et al. [39] developed a neural mass model of a reduced corticothalamic system consisting of two sets of cortical populations linked at the thalamic level. The rationale for considering a two-cortical-region model is the hypothesis that one of the functions of the intralaminar thalamus is to set up patterns of cortical interactions that are appropriate to specific behaviors [40]. Such interactions typically link a sensory and a motor area, with one region driving the other, depending on task demands. When this linkage was modeled as the result of a partially shared reticular nucleus (i.e., shared inhibition), the resulting dynamics demonstrated transitions between several modes of corticocortical coupling: one mode in which the two cortical regions were both active and synchronized, and two modes in which one cortical region dominates and drives the other. When the linkage consisted of shared excitation (e.g., via a partially shared thalamic relay nucleus), only the synchronous mode was present. In a pilot study that examined the EEG of a patient with severe chronic brain injury and a reproducible behavioral improvement with zolpidem[14,41], the authors found that this behavioral improvement was associated with an increase in the number of mode transitions involving frontal brain regions, which correlated with an increase in metabolic activity as measured by PET scans.
This modeling study provides a rationale for examining not only standard (time-averaged) spectra and coherences, but how they fluctuate in time[14], as the latter may be an indirect indicator of thalamic activity that cannot be directly observed in the EEG. The model's predictions of the power spectra and coherences of EEG activity were derived from a standard linearized analysis at the fixed points of the neural mass model. But importantly, the predictions about their fluctuations over time – the spectrograms and coherograms – were derived from examining the stability of the fixed points of the neural mass model, and how these fixed points relate to each other. Thus, the nonlinear nature of the neural mass model played a crucial role in this analysis.
Neural mass models also form the starting point for “inverse” approaches, such as dynamic causal modeling [35,42]. Here, a series of candidate neural mass models are constructed, based on hypotheses concerning the relevant anatomical connectivity. The mass model is then augmented by a biophysical or hemodynamic model that couples the neural mass variables to the observables (i.e., the EEG or the BOLD response). Finally, a model selection procedure (the “inversion”) is used to determine which candidate connectivity model is most likely to account for the observed data.
This approach has recently been applied to the spectral changes in the EEG that underlie the transition to unconsciousness during propofol anesthesia[43]. Specifically, the investigators considered three models of increasing complexity: (i) connected anterior and posterior cortical masses, (ii) addition of a thalamic mass connected to both cortical masses, and (iii) subdivision of the thalamic mass into two parts, one connected to the anterior cortical mass and one connected to the posterior cortical mass. As described above, the transition to unconsciousness was associated with an increase in low-frequency activity in the delta- and alpha- bands. Bayesian model selection favored model (ii): a thalamic mass connected to an anterior and a posterior cortical mass. In the context of this model, propofol produced a selective loss of anterior-to-posterior cortical connectivity, with retention of posterior-to-anterior connectivity and thalamocortical connectivity, extending and refining the observations of Lewis et al.[25]. Thus, dynamic causal modeling goes beyond standard spectral analysis by seeking to identify the direction of functional connectivity and thereby make predictions about causality. As reviewed elsewhere [44], the strategy taken to extract directional information from the observed data signals relies on specific parametric features of a neural mass model, such as the expected propagation times between brain areas. This is in contrast to the information-theoretic approach of Granger causality analysis[45], which is fundamentally nonparametric. Note also that while the underlying neural mass models themselves are nonlinear, the nonlinearity is not crucial to these inferences – the model is studied in a linearized regime, and inferences are based on observed power spectra and coherences.
Other approaches to characterizing global dynamics
Other extensions of standard spectral characterizations -- bispectra, bicoherences, and their higher-order analogues -- focus on whether activity at one frequency is coupled to activity at another [10]. Phase-amplitude coupling is a specific kind of cross-frequency interaction that has attracted muchinterest, and for which specialized indices have been developed[46]. Applying these indices to EEG recordings during propofol induction of anesthesia, Mukamel et al. [47] identified state-dependent coupling of the amplitude of the alpha-range activity to the phase of the low-frequency activity.
Graph-theoretic methods have also been advanced as a dimensional reduction tool that characterizes spatial characteristics of the EEG, in resting wakefulness [48] and in epilepsy [33], and, recently, in brain injury (T Nauvel et al., abstract, Society for Neuroscience, New Orleans, November 2012). Although preliminary, these findings suggest that graphical methods may be able to identify broad patterns characteristic of recovery from brain injury.
Examining EEG responses to stimulation provides an additional approach to understanding brain dynamics. Using methods of dynamic causal modeling and source localization, Boly et al.[49] studied the mismatch negativity response in patients in VS, MCS, and healthy controls. The dynamic causal model deduced from data from VS subjects was distinguished from the model deduced from data from MCS subjects and controls by a lack of feedback from an inferred frontal component to one in the temporal lobe. King et al.[50] examined single-trial EEG responses in VS, MCS, and confusional state (CS) patients, and found that multivariate pattern classifiers could distinguish among these states. Rosanova et al. and Ferrarelli et al.[51]showed that the dynamics of EEG responses to repetitive transcranial magnetic stimulation (TMS) showed a reliable and systematic dependence on the level of consciousness, across a range of states including VS, MCS, sleep states, locked-in-state (LIS), and normal subjects. At the extremes, patients in VS following structural brain injuries had TMS responses that were more local or had shorter timecourses and simpler dynamics than those recorded during dreaming, LIS, and normal wakefulness. Finally, Casali and colleagues[52] combined EEG measures of resting brain and responses to pulses of transcranial magnetic stimulation (TMS), to derive an index (based on algorithmic complexity) that correlated well with level of consciousness.
CONCLUSION
Severe brain injury often results in major disability, and its aggregate effects place a profound burden on the patient, family and society. Evaluation of the level of consciousness and cognitive abilities of patients is critical to prognostication, routine care, and clinical investigation. However, behavioral observation is unreliable, in large part because of the motor impairment often associated with brain injury. The EEG bypasses this potential confound. Its high temporal resolution allows for a focus on dynamics, and much progress has been made in identifying the basic features of large-scale brain dynamics that are common to different levels of injury and disorders of consciousness. To date, most of these efforts have focused on standard spectral measures (i.e., power spectra and coherences), and in linking these measures with pathophysiologic processes. Recent advances in the understanding of anesthetic-induced loss of consciousness, along with computational and mathematical modeling, suggest that other kinds of dynamical measures, sensitive to fluctuations and correlations among spectral features, may provide further diagnostic accuracy and mechanistic insight.
Highlights
EEG assays brain dynamics directly; behavioral observations rely on motor output.
In vegetative state, EEG power is largely confined to very low frequencies (<1 Hz).
In minimally conscious state, EEG power peaks in the 3–7 Hz range.
These findings likely reflect varying degrees of functional deafferentation.
Dynamical indices beyond spectral measures may also prove valuable.
Box 1.
Syndrome | Definition | Behavioral Characteristics |
---|---|---|
Coma | state of unarousable unresponsiveness | Eyes closed; motor function consists of reflex and postural responses only |
Vegetative State (VS) | state of intermittent arousal without evidence of consciousness | Spontaneous cycling through eyes-closed and eyes-open states, spontaneous eye and limb movements without evidence of goal-oriented behavior or sensory responsiveness |
Minimally Conscious State (MCS) | State of intermittent or inconsistent evidence of consciousness | Intermittent or inconsistent response to verbal command, verbal output, or object use; intermittent or inconsistent purposeful eye movements |
Confusional State (CS) | State of impaired consciousness with preserved functional object use or consistent communication | Disorientation; fluctuating levels of impairment; functional object use or consistent communication |
Locked in State (LIS) | State of complete or almost complete loss of motor output; not a disorder of consciousness | The misleading appearance of a disorder of consciousness due to lack of motor output; communication via brain-computer interface, EEG, functional brain imaging, autonomic responses, or subtle eye movements is possible |
ACKNOWLEDGEMENTS
This work was supported by NIH-NICHD HD51912 and the James S. McDonnell Foundation (NDS, PI). Some of the conceptual framework in this review was presented at the Society for Neuroscience Annual Meeting (2011), Drover, J.D., Conte, M.M., Goldfine, A.M., Voss, H.U., Victor, J.D., and Schiff, N.D. (2011) Are low frequency oscillations in the EEG of severely injured brains a marker for functional reserve of cortical neurons? (Abstract) Program No. 675.07. 2011
Footnotes
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