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. 2009 Jul;21(7):1797-862.
doi: 10.1162/neco.2009.06-08-799.

Discrete- and continuous-time probabilistic models and algorithms for inferring neuronal UP and DOWN states

Affiliations

Discrete- and continuous-time probabilistic models and algorithms for inferring neuronal UP and DOWN states

Zhe Chen et al. Neural Comput. 2009 Jul.

Abstract

UP and DOWN states, the periodic fluctuations between increased and decreased spiking activity of a neuronal population, are a fundamental feature of cortical circuits. Understanding UP-DOWN state dynamics is important for understanding how these circuits represent and transmit information in the brain. To date, limited work has been done on characterizing the stochastic properties of UP-DOWN state dynamics. We present a set of Markov and semi-Markov discrete- and continuous-time probability models for estimating UP and DOWN states from multiunit neural spiking activity. We model multiunit neural spiking activity as a stochastic point process, modulated by the hidden (UP and DOWN) states and the ensemble spiking history. We estimate jointly the hidden states and the model parameters by maximum likelihood using an expectation-maximization (EM) algorithm and a Monte Carlo EM algorithm that uses reversible-jump Markov chain Monte Carlo sampling in the E-step. We apply our models and algorithms in the analysis of both simulated multiunit spiking activity and actual multi- unit spiking activity recorded from primary somatosensory cortex in a behaving rat during slow-wave sleep. Our approach provides a statistical characterization of UP-DOWN state dynamics that can serve as a basis for verifying and refining mechanistic descriptions of this process.

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Figures

Figure 1
Figure 1
(a) The duration histograms of the UP (mean 0.96, median 0.67, support [0.1, 3], unit: second) and DOWN (mean 0.17, median 0.13, support [0.05, 1], unit: second) states of spiking data recorded from four behaving rats' visual cortex during SWS. Note that the statistics used in b are identical to those in (Ji & Wilson, 2007, Figure 2b). The y-axis in both plots shows the count statistics of all cortical UP and DOWN durations. (b) Censored versions of the log-normal and inverse gaussian pdfs for the UP (left panel) and DOWN (right panel) states. (c) Censored versions of the log-normal and inverse gaussian survival functions (1-cdf) for the UP (left panel) and DOWN (right panel) states. As comparison, the dashed lines in b and c show the holding time probability for an exponential distribution. Note that in the UP state, the holding time probability in both two-parameter distributions decays more slowly than that of the exponential distribution, whereas in the DOWN state, the holding time probability of exponential distribution decays more slowly than the others.
Figure 2
Figure 2
Synthetic data. (a) The simulated UP and DOWN hidden state process. (b) The simulated time-varying traces of conditional intensity function (CIF) λc(t) (c = 1, …, 4). (c) The four simulated spike trains. (d) The averaged firing rate across four spike trains (the solid gray curve corresponds to the temporally smoothed firing rate using a 30 ms width gaussian kernel).
Figure 3
Figure 3
A snapshot of UP and DOWN state estimation obtained from the discrete-time HMM for the simulated spike train data.
Figure 4
Figure 4
The fitted KS plots (top row) and autocorrelation plots (bottom row) for the four simulated spike trains from one Monte Carlo experiment (dotted and dashed lines in the plots indicate the 95% confidence bounds).
Figure 5
Figure 5
Snapshot illustrations of simulated synthetic spike trains and the estimated state posterior probability from the (a) HMM and (b) continuous-time semi-Markov model (b). The shaded area denotes the posterior probability of the hidden state being in an UP state. The estimation error rates (compared with the ground truth) in these two cases are 1.9% and 1.4%, respectively.
Figure 6
Figure 6
The estimation error comparison of different methods by varying the number of spike train observations (the statistics are computed based on five independent simulated trials). In all conditions, the spike trains are generated using the same conditions: μc = −3.6, αc = 7.2, and βc = 0.05.
Figure 7
Figure 7
A snapshot of recordings of cortical MUA, raw cortical EEG, cortical theta wave (4–8 Hz), cortical delta wave (2–4 Hz), raw hippocampal EEG, hippocampal ripple power (more than 100 Hz), hippocampal theta wave, and EMG.
Figure 8
Figure 8
Real-world MUA spike trains of eight tetrodes recorded from the primary somatosensory cortex of one rat (note that each tetrode might contain varying number of single cells). (a) A selected 5 s segment of the MUA spike trains during SWS and its UP and DOWN state classification via the threshold-based method (segmented by the thick solid line). (b) The hidden state estimation result obtained from the discrete-time HMM (used as the initial state for the continuous-time RJMCMC sampler). (c) The hidden state estimation obtained from the MCEM algorithm. In this example, the MCEM algorithm merged several neighboring sojourns that were decoded differently from the HMM.
Figure 9
Figure 9
Fitting the real-world sojourn-time duration length for the DOWN and UP states, where the UP or DOWN state classification is obtained from the discrete-time HMM estimation result. (Left panels) Histograms. (Right panels) Fitting the sojourn durations with exponential (for the DOWN state) and log-normal (for the UP state) distributions. If the sample data fit the tested probability density, the data points will approximately match the straight line in the plot.
Figure 10
Figure 10
Convergence plot of the simulated Markov chain. (a) Trajectory of the number of state jumps (inset: the trajectory within the first 1000 iterations). (b) Trajectory of the log likelihood in running the MCEM algorithm.
Figure 11
Figure 11
(Left panel) Estimated exponential decaying filters e−βcτ for the recorded spike trains shown in Figure 8. (Right panel) Estimated history dependence coefficients estimated for the eight spike trains (based on GLM fit using seven discrete windows of history spike counts: 1–5, 5–10, 10–15, 15–20, 20–30, 30–40, 40–50 ms). The estimated history-dependent firing coefficients exhibit an exponential-like decaying curve (for all eight spike trains).
Figure 12
Figure 12
Fitted KS plots of the real-world MUA spike trains (dotted lines along the diagonal indicate the 95% confidence bounds).
Figure 13
Figure 13
Autocorrelation plots for the real-world MUA spike trains (dashed lines indicate the 95% confidence bounds).
Figure 14
Figure 14
Cortical EEG averages (mean ± standard error of the mean, shown by trace width) triggered by the classified UP state start and end time stamps (for visualization purposes, the standard error of the mean in all plots is amplified by 10 times its original value). From top to bottom: Results from the threshold-based method, the HMM method, and the MCEM method. The start of the UP state is aligned with the K-complex signal that has a biphasic wave switching from a negative dip to a positive peak, which lasts about 200 ms.
Figure 15
Figure 15
Gaussian mixture clustering for the two firing features (log of duration and number of spikes per second). Here, the optimal number of mixtures is 3; the ellipses represent the two-dimensional gaussian shapes with different covariance structures.
Figure 16
Figure 16
Threshold-based method for estimating the median duration length of the UP and DOWN states (data from the same rat on a different day) in which two thresholds are chosen by grid search. The abscissa represents the gap threshold (in millisecond), and the ordinate represents the smoothed spike count threshold. The map's units are shown in seconds.

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