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Articles, Systems/Circuits

Inferring Cortical Variability from Local Field Potentials

Yuwei Cui, Liu D. Liu, James M. McFarland, Christopher C. Pack and Daniel A. Butts
Journal of Neuroscience 6 April 2016, 36 (14) 4121-4135; DOI: https://doi.org/10.1523/JNEUROSCI.2502-15.2016
Yuwei Cui
1Department of Biology and Program in Neuroscience and Cognitive Science, University of Maryland, College Park, Maryland 20815, and
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Liu D. Liu
2Montréal Neurological Institute, McGill University, Montréal, Quebec H3A 2B4, Canada
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James M. McFarland
1Department of Biology and Program in Neuroscience and Cognitive Science, University of Maryland, College Park, Maryland 20815, and
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Christopher C. Pack
2Montréal Neurological Institute, McGill University, Montréal, Quebec H3A 2B4, Canada
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Daniel A. Butts
1Department of Biology and Program in Neuroscience and Cognitive Science, University of Maryland, College Park, Maryland 20815, and
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  • Figure 1.
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    Figure 1.

    Response variability of MT neurons. A, The responses of two MT neurons to repeated presentations of a continuously varying optic flow stimulus, with four example frames from a section of the repeated stimulus segment (top). The peristimulus time histograms (PSTHs, bottom, black) are compared with the firing rate predictions of the stimulus-processing model (red), labeled with the fraction of stimulus-locked response explained by the model [predictive power (PP)]. B, Spike rasters of the same neurons as in A, from which the PSTHs are generated. The shaded areas mark epochs where data are excluded from analysis due to periods when eye position was outside the fixation window. C, Model schematic illustrating the main components of the stimulus-processing model: the stimulus composed is first processed locally by direction- and speed-selective local subunits, and then gets pooled across space separately by Exc (left), Sup (middle), and NS-Sup (right) components. Red and blue arrows (left) indicate direction selectivity for the Exc and Sup terms. Finally, a spiking nonlinearity is applied to this signal to transform it into a firing rate prediction (bottom). D, The distribution of the stimulus-locked rate variation across MT neurons (n = 108, mean = 45.9 ± 25.9%; see Materials and Methods). The black arrows indicate the location of the two example neurons in A (stimulus-locked variance = 16.5% and 96.4%).

  • Figure 2.
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    Figure 2.

    Predicting MT responses from the stimulus and inferred network activity. A, Time–frequency analysis of the LFPs. Left, LFP signals and spiking activity were recorded with a 16-channel multielectrode array and used as inputs to a model that predicts a given single unit on the array (described below). Middle, To illustrate how each LFP was processed for use in the model, we show an LFP segment bandpassed in the gamma (30–70 Hz), alpha (8–12 Hz), and delta (1–4 Hz) bands. Right, To process each LFP for input to our model, we use a continuous wavelet transform to decompose the LFP signal into its amplitude and phase in each frequency band. To demonstrate how phase relates to a given bandpassed signal, the delta phase is shown below the delta band-filtered LFP (bottom middle); with times that phase is 180° (blue arrows) corresponding to local minima in the bandpassed signal. B, The phase-locking strength measured across frequency band and depth for an example neuron (top), demonstrating sensitivity in the delta and gamma bands. The phase-locking strength of simulated spikes generated by the LFP model (bottom) is nearly identical, demonstrating how the localized model components in D combine with correlations between LFP band and depth to result in empirical phase-locking measurements. C, Schematic of the LFP model, which includes a stimulus-processing component (from Fig. 1B), and the LFP-based component. D, Example LFP model component. Model weights (left) and preferred phases (right) are displayed as a function of both frequency bands (horizontal axis) and cortical depth (vertical axis). Phase values are depicted by hue, with the color brightness representing the corresponding weights to emphasize frequency bands and depths that are most important. E, To determine the effect of simultaneously fitting multiple model components, we measured the ratio of model weights for single-electrode LFP models fit with and without the stimulus-processing model. This shows that LFP models fit without the stimulus-processing component typically have much larger weights in low-frequency bands (<4 Hz, *p < 0.001, n = 108).

  • Figure 3.
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    Figure 3.

    Dramatic improvement of model performance with the inclusion of the LFP component. A, LLx values calculated for stimulus-processing models (left), and models that included either the LFP from the same electrode (middle) or all electrodes (right), for all neurons in the study. LLx values were calculated at both 25 ms (left) and 5 ms (right) time resolution. To demonstrate the relative performance of each model across all neurons, we also normalized each LLx value by that of the best model for that neuron (introduced below), and thus no model median reaches the (dashed) unity line here. The inclusion of the LFP component yields a more than threefold improvement in performance over the stimulus-processing model at 25 ms resolution (approximately the time course of the stimulus-locked rate). When considered at a higher time resolution (5 ms), the LFP model yields a median fivefold performance improvement, due to information about finer spike timing gained from the gamma-band LFP. B, The total variance of predicted firing rates from different models, normalized by the measured variance (left) or the variance of the best model for that neuron (right). C, Model performance improvement is tightly correlated with the increase in the variance of model outputs (r = 0.984, p < 10−67). D, Improvements in model performance were greater for neurons that were less stimulus locked (r = −0.64, p < 10−10).

  • Figure 4.
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    Figure 4.

    Frequency and phase preferences of MT neurons. A, There is a diverse array of tuning captured by the LFP components of different neurons, shown for six examples, with the red arrow designating the depth of the unit being modeled. Model weights (left) and preferred phases (right) are displayed as a function of both frequency bands (horizontal axis) and cortical depth (vertical axis) in the same way as in Figure 2C. B, While the absolute depth of the unit could not be determined in our experiments, we aligned model weights relative to the depth of the unit being modeled, and averaged these weights across neurons. This shows that model weights from the gamma band (30–70 Hz) are mostly localized in depth, whereas weights from the delta band (1–4 Hz) are distributed across multiple channels (n = 93). C, The relative impact of each LFP frequency band on model performance was computed by fitting each LFP model while omitting a given band. The effect on normalized LLx is shown across all neurons (n = 93), showing that the removal of gamma (30–70 Hz) and delta (1–4 Hz) bands has the biggest impact on model performance. D, The consistency across neurons of phase preferences in each LFP band is demonstrated by a two-dimensional histograms of the preferred phase of each neuron in each frequency band from the single-electrode LFP model (n = 108).

  • Figure 5.
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    Figure 5.

    Modeling MT neuron response with multiunit activity. A, Example multiunit spiking activity (MUA, top) and the resulting population firing rate (PR; bottom) recorded from the multielectrode array, with the red box highlighting the single unit being modeled (which was excluded from the model). B, Schematic of the population rate model, which sum the output of PR-based and stimulus-processing components, passing the result through a spiking nonlinearity. The contribution of the PR was modeled using a linear temporal filter applied to the recent history of PR. C, Left, A typical PR filter, showing coupling between the example neuron and PR as a function of time lag (horizontal axis). Right, Average of all PR model components across the population of recorded neurons (n = 93). D, Left, The LLx of the PR and MUA models across the population of recorded neurons. Right, The same data, showing the normalized LLx across all neurons (as in Fig. 3), where the LLx of each model was normalized by the LLx of the best model for that neuron (see below). The normalized LLx is thus on the same scale as the LFP models considered earlier (Fig. 3), demonstrating that the PR-based models have less than half the performance of the LFP-based models. E, Schematic of the MUA model, where the MUA component replaces the PR component considered above (B). F, Left, A typical MUA model component, showing weights on MUA as a function of time lag (horizontal axis) and electrode depth (vertical axis) for the same neuron as the example in the top left panel in B. Right, Average of all MUA model components across the population of recorded neurons.

  • Figure 6.
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    Figure 6.

    Network inputs predict trial-to-trial variability. A, Schematic of the full model, which includes a stimulus-processing component, and two “network-based” components: the LFP and MUA components. B, The model performance of the range of models considered, using the cross-validated log-likelihood relative to the “full” Stim–LFP–MUA model (normalized LLx). This demonstrates that, while the addition of the MUA component can yield a nearly twofold improvement over the stimulus-processing (Stim) model, it has only a very small impact when added to the Stim–LFP model. C, The summed output of the three model components of the full model explains the spike response (red rasters) of the MT neuron on a trial-by-trial basis, as shown by the correspondence between observed spikes and model output. Colors are scaled such that blue is the most negative model output, and yellow is the most positive (arbitrary units). D, Spike raster across repeated trials (left), and the output of the three model components (right) across repeated trials of the same motion stimulus. The stimulus component output is identical across trials; the output of the LFP-dependent term is highly variable across trials, and the MUA component output has both stimulus-locked and trial-variable elements. The trial-averaged spike response and output of the three model components are shown on the bottom (black curve), together with an example trial in red. E, Variance of the model-predicted firing rate, normalized by the total amount of estimated firing-rate variance. F, The total variance of the model outputs are further separated into the contributions to the model firing rate of the stimulus-locked (left) and trial-variable (right) components, and are normalized by the corresponding measured stimulus-locked and estimated trial-variable variance. For example, the Stim model cannot predict any trial-variable variance (first column on right), while the full model (Stim–LFP–MUA, fourth column) predicts a median of 38% of the trial-variable variance of each neuron.

  • Figure 7.
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    Figure 7.

    LFP signals predict noise correlation. A, Examples demonstrating a range of measured noise correlations between pairs of MT neurons (left), which largely match the shape of the noise correlations predicted by the LFP models fit separately to each neuron in the pair (right, blue), compared with the predictions of the PR model (dashed red). B, The correlation coefficients between measured and predicted noise correlation functions demonstrate that the LFP models are capturing the shape of the noise correlation functions (median, r = 0.63 ± 0.04). The PR model has significantly worse performance (median, r = 0.56 ± 0.06, p < 0.05), whereas the combined PR plus LFP model does not perform significantly better than the LFP model (median, r = 0.67 ± 0.04, p = 0.60). C, Top, Simultaneously recorded pairs of neurons had a range of noise correlations (histogram shown across all pairs). Middle, bottom, The LFP model could predict these correlations on a neuron-by-neuron basis (middle, r = 0.77), again with the PR model not achieving as high performance (bottom, r = 0.50). D, The LFP model also could predict the dependence of noise correlation on relative depth: measured noise correlation (top) declines as a function of distance between MT neuron pairs, which is captured by the LFP model (bottom). Dashed lines show exponential fits to this relationship.

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The Journal of Neuroscience: 36 (14)
Journal of Neuroscience
Vol. 36, Issue 14
6 Apr 2016
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Inferring Cortical Variability from Local Field Potentials
Yuwei Cui, Liu D. Liu, James M. McFarland, Christopher C. Pack, Daniel A. Butts
Journal of Neuroscience 6 April 2016, 36 (14) 4121-4135; DOI: 10.1523/JNEUROSCI.2502-15.2016

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Inferring Cortical Variability from Local Field Potentials
Yuwei Cui, Liu D. Liu, James M. McFarland, Christopher C. Pack, Daniel A. Butts
Journal of Neuroscience 6 April 2016, 36 (14) 4121-4135; DOI: 10.1523/JNEUROSCI.2502-15.2016
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