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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Amari Neural Field =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Intermediate&lt;br /&gt;
| reading_time = 7 minutes&lt;br /&gt;
| prerequisites = PDEs; convolution integrals; [[Wilson-Cowan_Model|Wilson-Cowan]].&lt;br /&gt;
| if_too_advanced_see = [[Wilson-Cowan_Model]]&lt;br /&gt;
| if_you_want_the_math_see = This page; [[Neural_Field_Equations]]&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{Notation&lt;br /&gt;
| psi_convention = ψ = scalar field amplitude (separate from u, the neural-field variable here).&lt;br /&gt;
| signature      = Mostly-plus.&lt;br /&gt;
| units          = SI; cortical position x in metres; firing rates in Hz; synaptic drive u in mV.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Amari neural-field equation&amp;#039;&amp;#039;&amp;#039; (Shun-ichi Amari, 1977) is the spatial-continuum generalisation of [[Wilson-Cowan_Model|Wilson-Cowan]]. Instead of two lumped populations, it treats neural activity as a &amp;#039;&amp;#039;&amp;#039;continuous scalar field&amp;#039;&amp;#039;&amp;#039; u(x, t) defined over cortical position x.&lt;br /&gt;
&lt;br /&gt;
This is the mathematically natural setting for studying spatial patterns of cortical activity: travelling waves, localised &amp;quot;bumps&amp;quot; (working memory), pinwheels (orientation columns), and pattern formation.&lt;br /&gt;
&lt;br /&gt;
== Statement ==&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\tau\,\frac{\partial u(\mathbf{x},t)}{\partial t} = -u(\mathbf{x},t) + \!\int_\Omega\! w(\mathbf{x} - \mathbf{x}&amp;#039;)\,f\bigl(u(\mathbf{x}&amp;#039;,t)\bigr)\,d^n x&amp;#039; + h(\mathbf{x},t)&amp;lt;/math&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 !! Units&lt;br /&gt;
|-&lt;br /&gt;
| u(x, t) || Synaptic-input field || mV (or arbitrary)&lt;br /&gt;
|-&lt;br /&gt;
| Ω || Cortical domain || m&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; (or m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;)&lt;br /&gt;
|-&lt;br /&gt;
| x, x&amp;#039; || Cortical positions || m&lt;br /&gt;
|-&lt;br /&gt;
| w(x − x&amp;#039;) || Synaptic-connectivity kernel || m&amp;lt;sup&amp;gt;−2&amp;lt;/sup&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| f(u) || Firing-rate function (sigmoid) || Hz&lt;br /&gt;
|-&lt;br /&gt;
| h(x, t) || External input || mV&lt;br /&gt;
|-&lt;br /&gt;
| τ || Membrane time constant || ~ 10 ms&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Derivation sketch ==&lt;br /&gt;
&lt;br /&gt;
Start from Wilson-Cowan with the position index x. In the large-population limit:&lt;br /&gt;
&lt;br /&gt;
# Replace the discrete-population weights w&amp;lt;sub&amp;gt;EE&amp;lt;/sub&amp;gt;, w&amp;lt;sub&amp;gt;EI&amp;lt;/sub&amp;gt;, ... by a spatial kernel w(x − x&amp;#039;). For a single population (effective net coupling), this kernel commonly has the &amp;#039;&amp;#039;&amp;#039;Mexican-hat&amp;#039;&amp;#039;&amp;#039; shape: positive at short range, negative at intermediate range.&lt;br /&gt;
# Replace the population activity by a continuous field u(x, t).&lt;br /&gt;
# Replace the sum over connections by a spatial integral.&lt;br /&gt;
&lt;br /&gt;
The result is the Amari equation.&lt;br /&gt;
&lt;br /&gt;
== Mexican-hat connectivity ==&lt;br /&gt;
&lt;br /&gt;
A canonical choice is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;w(\mathbf{x} - \mathbf{x}&amp;#039;) = A_+\,\exp\!\left(-\frac{|\mathbf{x}-\mathbf{x}&amp;#039;|^2}{\sigma_+^2}\right) - A_-\,\exp\!\left(-\frac{|\mathbf{x}-\mathbf{x}&amp;#039;|^2}{\sigma_-^2}\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with &amp;lt;math&amp;gt;A_+ &amp;gt; A_- &amp;gt; 0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\sigma_- &amp;gt; \sigma_+&amp;lt;/math&amp;gt; — short-range excitation, longer-range inhibition. This is the empirical pattern of intracortical connectivity for many cortical regions.&lt;br /&gt;
&lt;br /&gt;
== Localised solutions: &amp;quot;bumps&amp;quot; ==&lt;br /&gt;
&lt;br /&gt;
A central result: with Mexican-hat connectivity, the Amari field admits stable localised solutions — &amp;#039;&amp;#039;&amp;#039;bumps&amp;#039;&amp;#039;&amp;#039; — that persist in the absence of input. These bumps:&lt;br /&gt;
&lt;br /&gt;
* Carry localised activity at position x&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; indefinitely.&lt;br /&gt;
* Are the mathematical basis for &amp;#039;&amp;#039;&amp;#039;working memory&amp;#039;&amp;#039;&amp;#039; (the bump stores &amp;quot;the cup is to the left&amp;quot;).&lt;br /&gt;
* Are the basis for &amp;#039;&amp;#039;&amp;#039;attentional spotlights&amp;#039;&amp;#039;&amp;#039;.&lt;br /&gt;
* Can drift, split, merge under perturbation.&lt;br /&gt;
&lt;br /&gt;
== Travelling waves ==&lt;br /&gt;
&lt;br /&gt;
The Amari field also supports &amp;#039;&amp;#039;&amp;#039;travelling-wave&amp;#039;&amp;#039;&amp;#039; solutions:&lt;br /&gt;
&lt;br /&gt;
  u(x, t) = U(x − v · t)&lt;br /&gt;
&lt;br /&gt;
These propagate at a velocity v determined by the kernel and gain. They are the mathematical model for:&lt;br /&gt;
&lt;br /&gt;
* Cortical waves observed in electrophysiology (e.g. during slow-wave sleep).&lt;br /&gt;
* Spreading depression and migraine aura.&lt;br /&gt;
* Wave-propagation models of epileptic seizures.&lt;br /&gt;
&lt;br /&gt;
== Dynamics ==&lt;br /&gt;
&lt;br /&gt;
Stability of bumps depends on the kernel and the gain of f(u). Amari&amp;#039;s original 1977 paper showed:&lt;br /&gt;
&lt;br /&gt;
* For Heaviside firing functions f(u) = Θ(u − θ), bumps exist for a window of input strengths.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Wider&amp;#039;&amp;#039;&amp;#039; bumps are unstable; &amp;#039;&amp;#039;&amp;#039;narrower&amp;#039;&amp;#039;&amp;#039; bumps stable (counter-intuitive but rigorous).&lt;br /&gt;
* For sigmoidal f, the analysis becomes more involved but the bump phenomenology persists.&lt;br /&gt;
&lt;br /&gt;
== Sanity-check limits ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;No spatial coupling&amp;#039;&amp;#039;&amp;#039; (w → δ-function at zero): reduces to point Wilson-Cowan (u&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; ≡ u&amp;lt;sub&amp;gt;local&amp;lt;/sub&amp;gt;). ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Uniform input h(x,t) = h&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&amp;#039;&amp;#039;&amp;#039;: solution u(x,t) ≡ u&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; uniform (no spatial structure). ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Δ → 0&amp;#039;&amp;#039;&amp;#039; or w → 0: pure exponential decay; no patterns. ✓&lt;br /&gt;
&lt;br /&gt;
== Connection to ψ ==&lt;br /&gt;
&lt;br /&gt;
In the [[Wilson-Cowan_Coupled_to_Psi|ψ-coupled extension]], the Amari equation gains a ψ-driven term:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\tau\,\partial_t u = -u + \!\int\! w(\mathbf{x}-\mathbf{x}&amp;#039;)\,f\bigl(u(\mathbf{x}&amp;#039;,t)\bigr)\,d^n x&amp;#039; + h(\mathbf{x},t) + \beta\,\psi(\mathbf{x},t)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and sources ψ via:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;J_\psi(\mathbf{x},t) = \kappa_J\,f\bigl(u(\mathbf{x},t)\bigr)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
ψ propagates from x to x&amp;#039; as a separate, relativistic field (□ψ − m&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;ψ − λψ&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt; = ...) — so ψ provides a &amp;#039;&amp;#039;&amp;#039;non-local&amp;#039;&amp;#039;&amp;#039; coupling channel that cortical-network connectivity alone does not capture.&lt;br /&gt;
&lt;br /&gt;
== Experimental status ==&lt;br /&gt;
&lt;br /&gt;
Amari fields are standard in computational neuroscience:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Working memory in prefrontal cortex&amp;#039;&amp;#039;&amp;#039; — bump solutions match electrophysiology of delay-period activity (Wang 1999, 2001).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Cortical-wave observations&amp;#039;&amp;#039;&amp;#039; — match Amari-style propagation (Rubino et al. 2006; Townsend et al. 2015).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Pinwheels and orientation maps&amp;#039;&amp;#039;&amp;#039; — emerge from Amari fields with self-organising plasticity (Wolf-Geisel 1998 and successors).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;MEG / EEG spatial spectra&amp;#039;&amp;#039;&amp;#039; — fit to Amari + delay extensions (the Robinson-Rennie family of models).&lt;br /&gt;
&lt;br /&gt;
The Amari equation is mainstream, well-validated computational neuroscience.&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Wilson-Cowan_Model]]&lt;br /&gt;
* [[Neural_Field_Equations]]&lt;br /&gt;
* [[Wilson-Cowan_Coupled_to_Psi]]&lt;br /&gt;
* [[Jansen-Rit_Neural_Mass]]&lt;br /&gt;
* [[Effective_Field_Theory_of_Consciousness]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Amari, S. (1977). &amp;quot;Dynamics of pattern formation in lateral-inhibition type neural fields.&amp;quot; &amp;#039;&amp;#039;Biological Cybernetics&amp;#039;&amp;#039; 27: 77–87.&lt;br /&gt;
* Coombes, S., Beim Graben, P., Potthast, R., Wright, J. (eds.) (2014). &amp;#039;&amp;#039;Neural Fields: Theory and Applications.&amp;#039;&amp;#039; Springer.&lt;br /&gt;
* Wang, X.-J. (1999). &amp;quot;Synaptic basis of cortical persistent activity: The importance of NMDA receptors to working memory.&amp;quot; &amp;#039;&amp;#039;Journal of Neuroscience&amp;#039;&amp;#039; 19: 9587–9603.&lt;br /&gt;
* Bressloff, P. C. (2012). &amp;quot;Spatiotemporal dynamics of continuum neural fields.&amp;quot; &amp;#039;&amp;#039;Journal of Physics A: Mathematical and Theoretical&amp;#039;&amp;#039; 45: 033001.&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>
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