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Dynamic causal modeling

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Dynamic causal modeling (DCM) is a Bayesian model comparison procedure for comparing models of how data were generated. Dynamic causal models are formulated in terms of stochastic or ordinary differential equations (i.e., nonlinear state-space models in continuous time). These equations model the dynamics of hidden states in the nodes of a probabilistic graphical model, where conditional dependencies are parameterized in terms of directed effective connectivity.

DCM was initially developed for identifying models of neural dynamics, estimating their parameters and comparing their evidence.[1]. DCM allows one to test competing models of interactions among neural populations (effective connectivity) using functional neuroimaging data e.g., functional magnetic resonance imaging (fMRI), magnetoencephalography (MEG) or electroencephalography (EEG).

Procedure

DCM is usually used to estimate the coupling among brain regions and the changes in coupling due to experimental changes (e.g., time or context). The basic idea is to construct reasonably realistic models of interacting brain regions. These models are then supplemented with a forward model of how the hidden states of each brain region (e.g., neuronal activity) give rise to the measured responses. This enables the best model(s) and their parameters (i.e. effective connectivity) to be identified from observed data. Bayesian model comparison is used to compare models based on their evidence, which can then be characterised in terms of parameters (e.g. connection strengths).

DCM studies typically involve the following stages [2]:

  1. Experimental design. Specific hypotheses are formulated and a neuroimaging experiment is conducted.
  2. Data preparation. The acquired data are pre-processed (e.g., to select relevant data features and remove confounds).
  3. Model specification. One or more forward models (DCMs) are specified for each subject's data.
  4. Model estimation. The model(s) are fitted to the data to determine their evidence and parameters.
  5. Model comparison. The evidence for the data under each model is compared using Bayesian Model Comparison, at the single-subject level or at the group level, and the parameters of the model(s) are inspected.

The key steps are briefly reviewed below.

Experimental design

Functional neuroimaging experiments are typically either task-based or they examine brain activity at rest (resting state). In task-based experiments, brain responses are evoked by known deterministic inputs (experimentally controlled stimuli) that embody designed changes in sensory stimulation or cognitive set. These experimental or exogenous variables can change neural activity in one of two ways. First, they can elicit responses through direct influences on specific brain regions. This would include, for example, sensory evoked responses in the early visual cortex. The second class of inputs exerts their effects vicariously, through a modulation of the coupling among nodes, for example, the influence of attention on the processing of sensory information. These two types of input - driving and modulatory - are separately parameterized in DCM[1]. To enable efficient estimation of driving and modulatory effects, a 2x2 factorial experimental design is often used - with one factor serving as the driving input and the other as the modulatory input [2].

Resting state experiments have no experimental manipulations within the period of the neuroimaging recording. Instead, hypotheses are tested about the coupling of endogenous fluctuations in neuronal activity, or in the differences in connectivity between scans or subjects. The DCM framework includes models and procedures for analysing resting state data, described below.

Model specification

Dynamic Causal Models (DCMs) are nonlinear state-space dynamical systems in continuous time, parameterized in terms of directed effective connectivity between brain regions. Unlike Bayesian Networks, DCMs can be cyclic, and unlike Structural Equation modelling and Granger causality, DCM does not depend on the theory of Martingales; i.e., it does not assume that random fluctuations' are serially uncorrelated. All models in DCM have the following basic form:

The first line describes the change in neural activity with respect to time (i.e. ), which cannot be directly observed using non-invasive functional imaging modalities. The evolution of neural activity over time is controlled by a neural function with parameters and experimental inputs . The neural activity in turn causes the timeseries , written on the second line. The timesseries are generated via a observation function with parameters . Additive observation noise completes the observation model. usually, the key parameters of interest are the neural parameters which, for example, represent connection strengths that may change under different experimental conditions.

Specifying a DCM requires selecting a neural model and observation model and setting appropriate priors over the parameters - e.g. selecting which connections should be switched on or off.

Functional MRI

DCM for fMRI neural circuit
The neural model in DCM for fMRI. z1 and z2 are the mean levels of activity in each region. Parameters A are the effective connectivity, B is the modulation of connectivity by a specific experimental condition and C is the driving input.

The neural model in DCM for fMRI is a Taylor approximation that captures the gross causal influences between brain regions and their change due to experimental inputs (see picture). This is coupled with a detailed biophysical model of the generation of the BOLD response and the MRI signal[1], based on the Balloon model of Buxton et al.[3] and supplemented for use with neurovascular coupling and MRI data [4][5]. Additions to the neural model enable the inclusion of interactions between excitatory and inhibitory neural populations [6] and non-linear influences of neural populations on the coupling between other populations[7].

Support for resting state analysis was first introduced in Stochastic DCM[8], which estimates both neural fluctuations and connectivity parameters in the time domain using a procedure called Generalized Filtering. A faster and more accurate solution for resting state data was subsequently introduced which operates in the frequency domain, called DCM for Cross-Spectral Densities (CSD) [9][10]. Both of these can be applied to large-scale brain networks by constraining the connectivity parameters based on the functional connectivity[11][12]. Another recent development for resting state analysis is Regression DCM[13] implemented in the Tapas software collection (see Software implementations). Regression DCM operates in the frequency domain, but linearizes the model under certain simplifications, such as having a fixed (canonical) haemodynamic response function. The enables rapid estimation of models, enabling application to large-scale brain networks.

Models of the cortical column used in EEG/MEG/LFP analysis. Self-connections on each population are present but not shown for clarity. Left: DCM for ERP. Right: Canonical Microcircuit (CMC). 1=spiny stellate cells (layer IV), 2=inhibitory interneurons, 3=(deep) pyramidal cells and 4=superficial pyramidal cells.

EEG / MEG

DCM for EEG and MEG data use more biologically detailed neural models than fMRI, as the higher temporal resolution of these measurement techniques provides access to richer neural dynamics. These can be classed into physiological models, which recapitulate neural circuity, and phenomenological models, which focus on reproducing particular data features. The physiological models can be further subdivided into two classes. Conductance-based models derive from the equivalent circuit representation of the cell membrane developed by Hodgkin and Huxley in the 1950s[14] . Convolution models were introduced by Wilson & Cowan[15] and Freeman [16] in the 1970s and involve a convolution of pre-synaptic input by a synaptic kernel function. The specific models used in DCM are as follows:

  • Physiological models:
    • Convolution models:
      • DCM for evoked responses (DCM for ERP)[17][18]. This is a biologically plausible neural mass model, extending earlier work by Jansen and Rit[19]. It emulates the activity of a cortical area using three neuronal sub-populations (see picture), each of which rests on two operators. The first operator transforms the pre-synaptic firing rate into a Post-Synaptic Potential (PSP), by convolving a synaptic response function (kernel) by the pre-synaptic input. The second operator, a sigmoid function, transforms the membrane potential into a firing rate of action potentials.
      • DCM for LFP (Local Field Potentials)[20]. Extends DCM for ERP by adding the effects of specific ion channels on spike generation.
      • Canonical Microcircuit (CMC)[21]. Used to address hypotheses about laminar-specific ascending and descending signals in the brain, which underpin the predictive coding account of brain function. The single pyramidal cell population from DCM for ERP is split into deep and superficial populations (see picture). A version of the CMC has been applied to model multi-modal MEG and fMRI data[22].
      • Neural Field Model (NFM)[23]. Extends the models above into the spatial domain, modelling continuous changes in current across the cortical sheet.
    • Conductance models:
      • Neural Mass Model (NMM) and Mean-field model (MFM)[24][25]. These have the same arrangement of neural populations as DCM for ERP, above, but are based on the Morris-Lecar model of the barnacle muscle fibre [26], which in turn derives from the Hodgin and Huxley model of the giant squid axon[14]. They enable inference about ligand-gated excitatory (Na+) and inhibitory (Cl-) ion flow, mediated through fast glutamatergic and GABAergic receptors. Whereas DCM for fMRI and the convolution models represent the activity of each neural population by a single number - its mean activity - the conductance models include the full density (probability distribution) of activity across the population. The 'mean-field assumption' used in the MFM version of the model has the density of one population's activity depending only on the mean of other neural populations. A subsequent extension to the MFM model added voltage-gated NMDA ion channels[27].
  • Phenomenological models:
    • DCM for phase coupling[28]. Models the interaction of brain regions as Weakly Coupled Oscillators (WCOs), in which the rate of change of phase of one oscillator is related to the phase differences between itself and other oscillators.

Model estimation

Model inversion or estimation is implemented in DCM using variational Bayes under the Laplace approximation[29]. It provides two useful quantities. The log marginal likelihood or model evidence is the probability of observing of the data under the given model. This cannot be calculated explicitly and in DCM it is approximated by a quantity called the negative variational free energy , referred to in machine learning as the Evidence Lower Bound (ELBO). Hypotheses are tested by comparing the evidence for different models based on their free energy, a procedure called Bayesian model comparison.

Model estimation also provides estimates of the parameters , for example the connection strengths, which maximise the free energy. Where models differ only in their priors, Bayesian Model Reduction can be used to rapidly the derive the evidence and parameters for nested or reduced models.

Model comparison

Neuroimaging studies typically investigate effects which are conserved at the group level, or which differ between subjects. There are two predominant approaches for group-level analysis: random effects Bayesian Model Selection (BMS)[30] and Parametric Empirical Bayes (PEB)[31]. Random effects BMS posits that subjects differ in terms of which model generated their data - e.g. drawing a random subject from the population, there might be a 25% chance that their brain is structured like model 1 and a 75% chance that it is structured like model 2. The analysis pipeline for the BMS approach procedure follows a series of steps:

  1. Specify and estimate multiple DCMs per subject, where each DCM (or set of DCMs) embodies a hypothesis.
  2. Perform random effects BMS to estimate the proportion of subjects whose data were generated by each model
  3. Calculate the average connectivity parameters across models using Bayesian Model Averaging. This average is weighted by the posterior probability for each model. This means that models with greater probability contribute more to the average than models with lower probability.

Alternatively, one can use a parametric empirical Bayes (PEB) approach[31] is a hierarchical model over parameters (connection strengths). It eschews the notion of different models at the level of individual subjects, and posits that people differ in the (continuous) strength of their individual connections. The PEB approach separates sources of variability in connection strengths across subjects into hypothesised covariates and uninteresting between-subject variability (random effects). The PEB procedure is as follows:

  1. Specify a single 'full' DCM per subject, which contains all connectivity parameters of interest.
  2. Specify a Bayesian General Linear Model to model the parameters (the full posterior density) from all subjects at the group level.
  3. Test hypotheses by comparing the full group-level model to reduced group-level models where certain combinations of connections have been switched off.

Validation

Developments in DCM have been validated using different approaches:

  • Face validity establishes whether the parameters of a model can be recovered from simulated data. This is usually performed alongside the development of each new model (E.g. [1][7]).
  • Construct validity assesses consistency with other analytical methods. For example, DCM has been compared with Structural Equation Modelling [32] and other neurobiological computational models [33].
  • Predictive validity assesses the ability to predict known or expected effects. This has included testing against iEEG / EEG / stimulation [34][35][36][37] and against known pharmacological treatments [38][39].

Limitations / drawbacks

DCM is a hypothesis-driven approach for investigating the interactions among pre-defined regions of interest. It is not ideally suited for exploratory analyses[2]. Although methods have been implemented for automatically searching over reduced models (Bayesian Model Reduction) and for modelling large-scale brain networks[12], these methods require an explicit specification of model space. in neuroimaging, other approaches such as psycho-physical interactions (PPI) analysis may be more appropriate for discovering key nodes for DCM.

The variational Bayesian methods used for model estimation are based on the on the Laplace assumption that the posterior over parameters is Gaussian. This approximation can fail in the context of highly non-linear models, where local minima can preclude the free energy from serving as a tight bound on log model evidence. Sampling approaches provide the gold standard, however are time consuming to run. These have been used to validate the variational approximations in DCM [40]

Software implementations

DCM is implemented in the Statistical Parametric Mapping software package, which serves as the canonical or reference implementation (http://www.fil.ion.ucl.ac.uk/spm/software/spm12/). It has been re-implemented and developed in the Tapas software collection (https://www.tnu.ethz.ch/en/software/tapas.html) and the VBA toolbox (http://mbb-team.github.io/VBA-toolbox/).

Further reading

References

Category:Neuroimaging

Expanded the Dynamic Causal Modelling page to a full article

  1. ^ a b c d Friston, K.J.; Harrison, L.; Penny, W. (2003-08). "Dynamic causal modelling". NeuroImage. 19 (4): 1273–1302. doi:10.1016/s1053-8119(03)00202-7. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  2. ^ a b c d Stephan, K.E.; Penny, W.D.; Moran, R.J.; den Ouden, H.E.M.; Daunizeau, J.; Friston, K.J. (2010-02). "Ten simple rules for dynamic causal modeling". NeuroImage. 49 (4): 3099–3109. doi:10.1016/j.neuroimage.2009.11.015. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  3. ^ Buxton, Richard B.; Wong, Eric C.; Frank, Lawrence R. (1998-06). "Dynamics of blood flow and oxygenation changes during brain activation: The balloon model". Magnetic Resonance in Medicine. 39 (6): 855–864. doi:10.1002/mrm.1910390602. ISSN 0740-3194. {{cite journal}}: Check date values in: |date= (help)
  4. ^ Friston, K.J.; Mechelli, A.; Turner, R.; Price, C.J. (2000-10). "Nonlinear Responses in fMRI: The Balloon Model, Volterra Kernels, and Other Hemodynamics". NeuroImage. 12 (4): 466–477. doi:10.1006/nimg.2000.0630. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  5. ^ Stephan, Klaas Enno; Weiskopf, Nikolaus; Drysdale, Peter M.; Robinson, Peter A.; Friston, Karl J. (2007-11). "Comparing hemodynamic models with DCM". NeuroImage. 38 (3): 387–401. doi:10.1016/j.neuroimage.2007.07.040. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  6. ^ Marreiros, A.C.; Kiebel, S.J.; Friston, K.J. (2008-01). "Dynamic causal modelling for fMRI: A two-state model". NeuroImage. 39 (1): 269–278. doi:10.1016/j.neuroimage.2007.08.019. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  7. ^ a b Stephan, Klaas Enno; Kasper, Lars; Harrison, Lee M.; Daunizeau, Jean; den Ouden, Hanneke E.M.; Breakspear, Michael; Friston, Karl J. (2008-08). "Nonlinear dynamic causal models for fMRI". NeuroImage. 42 (2): 649–662. doi:10.1016/j.neuroimage.2008.04.262. ISSN 1053-8119. PMC 2636907. PMID 18565765. {{cite journal}}: Check date values in: |date= (help)
  8. ^ "Generalised filtering and stochastic DCM for fMRI". NeuroImage. 58 (2): 442–457. 2011-09-15. doi:10.1016/j.neuroimage.2011.01.085. ISSN 1053-8119.
  9. ^ Friston, Karl J.; Kahan, Joshua; Biswal, Bharat; Razi, Adeel (2014-07). "A DCM for resting state fMRI". NeuroImage. 94: 396–407. doi:10.1016/j.neuroimage.2013.12.009. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  10. ^ Razi, Adeel; Kahan, Joshua; Rees, Geraint; Friston, Karl J. (2015-02). "Construct validation of a DCM for resting state fMRI". NeuroImage. 106: 1–14. doi:10.1016/j.neuroimage.2014.11.027. ISSN 1053-8119. PMC 4295921. PMID 25463471. {{cite journal}}: Check date values in: |date= (help)
  11. ^ Seghier, Mohamed L.; Friston, Karl J. (2013-03). "Network discovery with large DCMs". NeuroImage. 68: 181–191. doi:10.1016/j.neuroimage.2012.12.005. ISSN 1053-8119. PMC 3566585. PMID 23246991. {{cite journal}}: Check date values in: |date= (help)
  12. ^ a b Razi, Adeel; Seghier, Mohamed L.; Zhou, Yuan; McColgan, Peter; Zeidman, Peter; Park, Hae-Jeong; Sporns, Olaf; Rees, Geraint; Friston, Karl J. (2017-10). "Large-scale DCMs for resting-state fMRI". Network Neuroscience. 1 (3): 222–241. doi:10.1162/netn_a_00015. ISSN 2472-1751. PMC 5796644. PMID 29400357. {{cite journal}}: Check date values in: |date= (help)
  13. ^ Frässle, Stefan; Lomakina, Ekaterina I.; Razi, Adeel; Friston, Karl J.; Buhmann, Joachim M.; Stephan, Klaas E. (2017-07). "Regression DCM for fMRI". NeuroImage. 155: 406–421. doi:10.1016/j.neuroimage.2017.02.090. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  14. ^ a b Hodgkin, A. L.; Huxley, A. F. (1952-04-28). "The components of membrane conductance in the giant axon ofLoligo". The Journal of Physiology. 116 (4): 473–496. doi:10.1113/jphysiol.1952.sp004718. ISSN 0022-3751.
  15. ^ Wilson, H. R.; Cowan, J. D. (1973-09). "A mathematical theory of the functional dynamics of cortical and thalamic nervous tissue". Kybernetik. 13 (2): 55–80. doi:10.1007/bf00288786. ISSN 0340-1200. {{cite journal}}: Check date values in: |date= (help)
  16. ^ "Mass Action in the Nervous System". 1975. doi:10.1016/c2009-0-03145-6. {{cite journal}}: Cite journal requires |journal= (help)
  17. ^ David, Olivier; Friston, Karl J. (2003-11). "A neural mass model for MEG/EEG:". NeuroImage. 20 (3): 1743–1755. doi:10.1016/j.neuroimage.2003.07.015. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  18. ^ Kiebel, Stefan J.; Garrido, Marta I.; Friston, Karl J. (2009-07-31), "Dynamic Causal Modeling for Evoked Responses", Brain Signal Analysis, The MIT Press, pp. 141–170, ISBN 9780262013086
  19. ^ Jansen, Ben H.; Rit, Vincent G. (1995-09-01). "Electroencephalogram and visual evoked potential generation in a mathematical model of coupled cortical columns". Biological Cybernetics. 73 (4): 357–366. doi:10.1007/s004220050191. ISSN 0340-1200.
  20. ^ Moran, R.J.; Kiebel, S.J.; Stephan, K.E.; Reilly, R.B.; Daunizeau, J.; Friston, K.J. (2007-09). "A neural mass model of spectral responses in electrophysiology". NeuroImage. 37 (3): 706–720. doi:10.1016/j.neuroimage.2007.05.032. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  21. ^ Bastos, Andre M.; Usrey, W. Martin; Adams, Rick A.; Mangun, George R.; Fries, Pascal; Friston, Karl J. (2012-11). "Canonical Microcircuits for Predictive Coding". Neuron. 76 (4): 695–711. doi:10.1016/j.neuron.2012.10.038. ISSN 0896-6273. {{cite journal}}: Check date values in: |date= (help); no-break space character in |first2= at position 3 (help); no-break space character in |first3= at position 5 (help); no-break space character in |first4= at position 7 (help); no-break space character in |first6= at position 5 (help); no-break space character in |first= at position 6 (help)
  22. ^ Friston, K.J.; Preller, Katrin H.; Mathys, Chris; Cagnan, Hayriye; Heinzle, Jakob; Razi, Adeel; Zeidman, Peter (2017-02). "Dynamic causal modelling revisited". NeuroImage. doi:10.1016/j.neuroimage.2017.02.045. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  23. ^ Pinotsis, D.A.; Friston, K.J. (2011-03). "Neural fields, spectral responses and lateral connections". NeuroImage. 55 (1): 39–48. doi:10.1016/j.neuroimage.2010.11.081. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  24. ^ Marreiros, André C.; Daunizeau, Jean; Kiebel, Stefan J.; Friston, Karl J. (2008-08). "Population dynamics: Variance and the sigmoid activation function". NeuroImage. 42 (1): 147–157. doi:10.1016/j.neuroimage.2008.04.239. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  25. ^ Marreiros, André C.; Kiebel, Stefan J.; Daunizeau, Jean; Harrison, Lee M.; Friston, Karl J. (2009-02). "Population dynamics under the Laplace assumption". NeuroImage. 44 (3): 701–714. doi:10.1016/j.neuroimage.2008.10.008. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  26. ^ Morris, C.; Lecar, H. (1981-07). "Voltage oscillations in the barnacle giant muscle fiber". Biophysical Journal. 35 (1): 193–213. doi:10.1016/s0006-3495(81)84782-0. ISSN 0006-3495. {{cite journal}}: Check date values in: |date= (help)
  27. ^ Moran, Rosalyn J.; Stephan, Klaas E.; Dolan, Raymond J.; Friston, Karl J. (2011-04). "Consistent spectral predictors for dynamic causal models of steady-state responses". NeuroImage. 55 (4): 1694–1708. doi:10.1016/j.neuroimage.2011.01.012. ISSN 1053-8119. PMC 3093618. PMID 21238593. {{cite journal}}: Check date values in: |date= (help)
  28. ^ Penny, W.D.; Litvak, V.; Fuentemilla, L.; Duzel, E.; Friston, K. (2009-09). "Dynamic Causal Models for phase coupling". Journal of Neuroscience Methods. 183 (1): 19–30. doi:10.1016/j.jneumeth.2009.06.029. ISSN 0165-0270. {{cite journal}}: Check date values in: |date= (help)
  29. ^ Friston, K.; Mattout, J.; Trujillo-Barreto, N.; Ashburner, J.; Penny, W. (2007), "Variational Bayes under the Laplace approximation", Statistical Parametric Mapping, Elsevier, pp. 606–618, ISBN 9780123725608
  30. ^ Rigoux, L.; Stephan, K.E.; Friston, K.J.; Daunizeau, J. (2014-01). "Bayesian model selection for group studies — Revisited". NeuroImage. 84: 971–985. doi:10.1016/j.neuroimage.2013.08.065. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  31. ^ a b Friston, Karl J.; Litvak, Vladimir; Oswal, Ashwini; Razi, Adeel; Stephan, Klaas E.; van Wijk, Bernadette C.M.; Ziegler, Gabriel; Zeidman, Peter (2016-03). "Bayesian model reduction and empirical Bayes for group (DCM) studies". NeuroImage. 128: 413–431. doi:10.1016/j.neuroimage.2015.11.015. ISSN 1053-8119. PMC 4767224. PMID 26569570. {{cite journal}}: Check date values in: |date= (help)
  32. ^ Penny, W.D.; Stephan, K.E.; Mechelli, A.; Friston, K.J. (2004-01). "Modelling functional integration: a comparison of structural equation and dynamic causal models". NeuroImage. 23: S264 – S274. doi:10.1016/j.neuroimage.2004.07.041. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  33. ^ Lee, Lucy; Friston, Karl; Horwitz, Barry (2006-05). "Large-scale neural models and dynamic causal modelling". NeuroImage. 30 (4): 1243–1254. doi:10.1016/j.neuroimage.2005.11.007. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  34. ^ David, Olivier; Guillemain, Isabelle; Saillet, Sandrine; Reyt, Sebastien; Deransart, Colin; Segebarth, Christoph; Depaulis, Antoine (2008-12-23). "Identifying Neural Drivers with Functional MRI: An Electrophysiological Validation". PLOS Biology. 6 (12): e315. doi:10.1371/journal.pbio.0060315. ISSN 1545-7885. PMC 2605917. PMID 19108604.{{cite journal}}: CS1 maint: unflagged free DOI (link)
  35. ^ David, Olivier; Woźniak, Agata; Minotti, Lorella; Kahane, Philippe (2008-02). "Preictal short-term plasticity induced by intracerebral 1 Hz stimulation". NeuroImage. 39 (4): 1633–1646. doi:10.1016/j.neuroimage.2007.11.005. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help); no-break space character in |title= at position 58 (help)
  36. ^ Reyt, Sébastien; Picq, Chloé; Sinniger, Valérie; Clarençon, Didier; Bonaz, Bruno; David, Olivier (2010-10). "Dynamic Causal Modelling and physiological confounds: A functional MRI study of vagus nerve stimulation". NeuroImage. 52 (4): 1456–1464. doi:10.1016/j.neuroimage.2010.05.021. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  37. ^ Daunizeau, J.; Lemieux, L.; Vaudano, A. E.; Friston, K. J.; Stephan, K. E. (2013). "An electrophysiological validation of stochastic DCM for fMRI". Frontiers in Computational Neuroscience. 6. doi:10.3389/fncom.2012.00103. ISSN 1662-5188.{{cite journal}}: CS1 maint: unflagged free DOI (link)
  38. ^ Moran, Rosalyn J.; Symmonds, Mkael; Stephan, Klaas E.; Friston, Karl J.; Dolan, Raymond J. (2011-08). "An In Vivo Assay of Synaptic Function Mediating Human Cognition". Current Biology. 21 (15): 1320–1325. doi:10.1016/j.cub.2011.06.053. ISSN 0960-9822. {{cite journal}}: Check date values in: |date= (help); no-break space character in |first3= at position 6 (help); no-break space character in |first4= at position 5 (help); no-break space character in |first5= at position 8 (help); no-break space character in |first= at position 8 (help); no-break space character in |title= at position 6 (help)
  39. ^ Moran, Rosalyn J.; Jung, Fabienne; Kumagai, Tetsuya; Endepols, Heike; Graf, Rudolf; Dolan, Raymond J.; Friston, Karl J.; Stephan, Klaas E.; Tittgemeyer, Marc (2011-08-02). "Dynamic Causal Models and Physiological Inference: A Validation Study Using Isoflurane Anaesthesia in Rodents". PLoS ONE. 6 (8): e22790. doi:10.1371/journal.pone.0022790. ISSN 1932-6203.{{cite journal}}: CS1 maint: unflagged free DOI (link)
  40. ^ Chumbley, Justin R.; Friston, Karl J.; Fearn, Tom; Kiebel, Stefan J. (2007-11). "A Metropolis–Hastings algorithm for dynamic causal models". NeuroImage. 38 (3): 478–487. doi:10.1016/j.neuroimage.2007.07.028. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  41. ^ Kahan, Joshua; Foltynie, Tom (2013-12). "Understanding DCM: Ten simple rules for the clinician". NeuroImage. 83: 542–549. doi:10.1016/j.neuroimage.2013.07.008. ISSN 1053-8119. {{cite journal}}: Check date values in: |date= (help)
  42. ^ Moran, Rosalyn; Pinotsis, Dimitris A.; Friston, Karl (2013). "Neural masses and fields in dynamic causal modeling". Frontiers in Computational Neuroscience. 7. doi:10.3389/fncom.2013.00057. ISSN 1662-5188.{{cite journal}}: CS1 maint: unflagged free DOI (link)