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		<summary type="html">&lt;p&gt;Phase N (01b): LaTeX restoration — promote Unicode display-math to &amp;lt;math&amp;gt;; lint-clean per tools/wiki_latex_lint.py&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Jansen-Rit Neural Mass =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Intermediate&lt;br /&gt;
| reading_time = 7 minutes&lt;br /&gt;
| prerequisites = ODEs; [[Wilson-Cowan_Model|Wilson-Cowan]]; some EEG/MEG familiarity.&lt;br /&gt;
| if_too_advanced_see = [[Wilson-Cowan_Model]]&lt;br /&gt;
| if_you_want_the_math_see = This page&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{Notation&lt;br /&gt;
| signature = Mostly-plus (irrelevant here).&lt;br /&gt;
| units     = Voltages in mV; time in ms; gain factors A, B in mV; rates a, b in 1/s.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Jansen-Rit neural-mass model&amp;#039;&amp;#039;&amp;#039; (Jansen and Rit, 1995) is a lumped model of a cortical column. It treats three interacting populations — &amp;#039;&amp;#039;&amp;#039;pyramidal cells&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;excitatory interneurons&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;inhibitory interneurons&amp;#039;&amp;#039;&amp;#039; — as point masses, each described by a second-order ODE.&lt;br /&gt;
&lt;br /&gt;
Jansen-Rit is the most widely-used neural-mass model in EEG/MEG source modelling. Multi-column networks built from Jansen-Rit units underlie tools like &amp;#039;&amp;#039;&amp;#039;The Virtual Brain&amp;#039;&amp;#039;&amp;#039; (TVB) and many dynamic-causal-modelling (DCM) workflows.&lt;br /&gt;
&lt;br /&gt;
== Statement ==&lt;br /&gt;
&lt;br /&gt;
Three coupled second-order ODEs for the membrane potentials y&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;, y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; of pyramidal, excitatory-interneuron, and inhibitory-interneuron populations:&lt;br /&gt;
&lt;br /&gt;
  d&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;y&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;/dt&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; = A · a · S[ y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; − y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; ] − 2a · dy&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;/dt − a&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; · y&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
  d&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/dt&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; = A · a · [ p(t) + C&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; · S[C&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; y&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;] ] − 2a · dy&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;/dt − a&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; · y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
  d&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/dt&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; = B · b · C&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; · S[C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; y&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;] − 2b · dy&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;/dt − b&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; · y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Components ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
! Symbol !! Meaning !! Typical value&lt;br /&gt;
|-&lt;br /&gt;
| y&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; || Pyramidal-cell membrane potential || mV&lt;br /&gt;
|-&lt;br /&gt;
| y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; || Excitatory-interneuron potential || mV&lt;br /&gt;
|-&lt;br /&gt;
| y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; || Inhibitory-interneuron potential || mV&lt;br /&gt;
|-&lt;br /&gt;
| A || Excitatory PSP amplitude || 3.25 mV&lt;br /&gt;
|-&lt;br /&gt;
| B || Inhibitory PSP amplitude || 22.0 mV&lt;br /&gt;
|-&lt;br /&gt;
| a || Inverse excitatory time constant || 100 /s (10 ms)&lt;br /&gt;
|-&lt;br /&gt;
| b || Inverse inhibitory time constant || 50 /s (20 ms)&lt;br /&gt;
|-&lt;br /&gt;
| C&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;–C&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; || Intra-column connection strengths || C ≈ 135 (with C&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;=C, C&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;=0.8C, C&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;=C&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;=0.25C)&lt;br /&gt;
|-&lt;br /&gt;
| S(v) || Sigmoidal firing function: S(v) = 2 e&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; / (1 + exp(r(v&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; − v))) || e&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; ≈ 2.5 /s, r ≈ 0.56 /mV, v&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; ≈ 6 mV&lt;br /&gt;
|-&lt;br /&gt;
| p(t) || External input (e.g. thalamic) || 120–320 /s (white-noise band)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;EEG signal&amp;#039;&amp;#039;&amp;#039; is identified with y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; − y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; — the net excitatory minus inhibitory drive onto the pyramidal cell — because pyramidal-cell post-synaptic potentials in apical dendrites are the dominant source of the scalp EEG.&lt;br /&gt;
&lt;br /&gt;
== Derivation sketch ==&lt;br /&gt;
&lt;br /&gt;
# A second-order ODE of the form (d/dt + a)&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; · y = A · a · u(t) is the impulse response of an &amp;#039;&amp;#039;&amp;#039;excitatory post-synaptic potential&amp;#039;&amp;#039;&amp;#039; (EPSP): a single delta-function input u = δ(t) produces y(t) = A · a · t · exp(−a · t), the canonical α-function PSP shape.&lt;br /&gt;
# Each population&amp;#039;s net membrane potential is the convolution of its PSP impulse response with the firing rate of its inputs.&lt;br /&gt;
# The pre-synaptic firing rate is the sigmoidal function S of the pre-synaptic population&amp;#039;s membrane potential.&lt;br /&gt;
# Three populations (pyramidal, excitatory interneuron, inhibitory interneuron) connected by C&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;–C&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; close the loop.&lt;br /&gt;
&lt;br /&gt;
The compact second-order-ODE form is just the differential equivalent of &amp;quot;PSP impulse response convolved with input rate&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
== Dynamics ==&lt;br /&gt;
&lt;br /&gt;
For appropriate parameters, Jansen-Rit produces:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;α rhythm&amp;#039;&amp;#039;&amp;#039; (~ 10 Hz) — the default state at biologically-realistic parameters.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Slow oscillations&amp;#039;&amp;#039;&amp;#039; at higher inhibitory gain B.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Spike-wave discharges&amp;#039;&amp;#039;&amp;#039; (epilepsy-like) at extreme parameter values.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Bifurcation transitions&amp;#039;&amp;#039;&amp;#039; between regimes as p(t) is varied — used to model state transitions (waking ↔ sleep, normal ↔ epileptic).&lt;br /&gt;
&lt;br /&gt;
Jansen-Rit was originally designed to match the visual-evoked-potential waveform; its parameters were tuned to fit empirical visual ERPs. Its later widespread use for spontaneous-EEG modelling was a fortunate generalisation.&lt;br /&gt;
&lt;br /&gt;
== Sanity-check limits ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;C = 0&amp;#039;&amp;#039;&amp;#039;: decoupled populations; each relaxes to zero. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Linear regime&amp;#039;&amp;#039;&amp;#039; (small y, sigmoid linearised): three decoupled damped oscillators with frequencies ~ a, ~ b. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;B = 0&amp;#039;&amp;#039;&amp;#039; (no inhibition): runaway excitation; no oscillation. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;A = 0&amp;#039;&amp;#039;&amp;#039; (no excitation): no activity. ✓&lt;br /&gt;
&lt;br /&gt;
== Multi-column extension ==&lt;br /&gt;
&lt;br /&gt;
Networks of Jansen-Rit units connected by long-range projections (the &amp;#039;&amp;#039;&amp;#039;connectome&amp;#039;&amp;#039;&amp;#039;) form the basis of large-scale brain models:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d^2 y_{0,i}}{dt^2} = A\,a\,S[\,y_{1,i} - y_{2,i}\,] - 2a\,\frac{dy_{0,i}}{dt} - a^2\,y_{0,i} + \sum_j K_{ij}\,S[\,y_{0,j}(t - \tau_{ij})\,]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with delay τ&amp;lt;sub&amp;gt;ij&amp;lt;/sub&amp;gt; and coupling K&amp;lt;sub&amp;gt;ij&amp;lt;/sub&amp;gt; from diffusion-MRI tractography.&lt;br /&gt;
&lt;br /&gt;
This is the architecture of &amp;#039;&amp;#039;&amp;#039;The Virtual Brain&amp;#039;&amp;#039;&amp;#039; (Sanz Leon et al. 2013) and similar large-scale tools.&lt;br /&gt;
&lt;br /&gt;
== Connection to ψ ==&lt;br /&gt;
&lt;br /&gt;
In the framework, Jansen-Rit units source ψ via their firing-rate output: J&amp;lt;sub&amp;gt;ψ&amp;lt;/sub&amp;gt;(x,t) ∝ S[y&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;(x,t) − y&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;(x,t)]. ψ propagates non-locally and feeds back via an additive β · ψ term in the input to each column. Coherent collective oscillations across many Jansen-Rit columns produce the strongest ψ source — connecting the framework to standard whole-brain neuroimaging.&lt;br /&gt;
&lt;br /&gt;
== Experimental status ==&lt;br /&gt;
&lt;br /&gt;
Jansen-Rit is &amp;#039;&amp;#039;&amp;#039;mainstream computational neuroscience&amp;#039;&amp;#039;&amp;#039;:&lt;br /&gt;
&lt;br /&gt;
* Fit to visual-evoked potentials (the original 1995 work).&lt;br /&gt;
* Used in DCM for spontaneous EEG / MEG (Friston-group software).&lt;br /&gt;
* Underpins TVB and similar whole-brain simulators.&lt;br /&gt;
* Validates against frequency-band statistics, ERP waveforms, and parametric pharmacological-modulation studies.&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Wilson-Cowan_Model]]&lt;br /&gt;
* [[Amari_Neural_Field]]&lt;br /&gt;
* [[Hodgkin-Huxley_Equations]]&lt;br /&gt;
* [[Neural_Field_Equations]]&lt;br /&gt;
* [[Wilson-Cowan_Coupled_to_Psi]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Jansen, B. H., Rit, V. G. (1995). &amp;quot;Electroencephalogram and visual evoked potential generation in a mathematical model of coupled cortical columns.&amp;quot; &amp;#039;&amp;#039;Biological Cybernetics&amp;#039;&amp;#039; 73: 357–366.&lt;br /&gt;
* David, O., Friston, K. J. (2003). &amp;quot;A neural mass model for MEG/EEG: Coupling and neuronal dynamics.&amp;quot; &amp;#039;&amp;#039;NeuroImage&amp;#039;&amp;#039; 20: 1743–1755.&lt;br /&gt;
* Sanz Leon, P., et al. (2013). &amp;quot;The Virtual Brain: A simulator of primate brain network dynamics.&amp;quot; &amp;#039;&amp;#039;Frontiers in Neuroinformatics&amp;#039;&amp;#039; 7: 10.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Equations]]&lt;br /&gt;
[[Category:Neuroscience]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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