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		<title>JonoThora: Psionics expansion (01a + 01b): content authored / LaTeX-restored per local submodule; lint-clean.</title>
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		<summary type="html">&lt;p&gt;Psionics expansion (01a + 01b): content authored / LaTeX-restored per local submodule; lint-clean.&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Stochastic Resonance =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Intermediate&lt;br /&gt;
| reading_time = 7 minutes&lt;br /&gt;
| prerequisites = Signal-processing basics (SNR); some dynamical-systems intuition.&lt;br /&gt;
| if_too_advanced_see = [[FitzHugh-Nagumo_Equations]]&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     = Signal-to-noise ratio in dB; noise variance in arbitrary units.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Stochastic resonance&amp;#039;&amp;#039;&amp;#039; (SR) is the counter-intuitive phenomenon that &amp;#039;&amp;#039;&amp;#039;adding noise to a nonlinear system can enhance — rather than degrade — its ability to detect a weak periodic signal&amp;#039;&amp;#039;&amp;#039;. The detected signal-to-noise ratio (SNR) of the output exhibits a maximum at a non-zero optimal noise level.&lt;br /&gt;
&lt;br /&gt;
SR is a robust, well-validated phenomenon in physics, signal processing, and biology. In the framework, SR is the mechanism by which &amp;#039;&amp;#039;&amp;#039;noisy biological systems&amp;#039;&amp;#039;&amp;#039; (neurons, sensory receptors) can detect very weak periodic forcing — including, in principle, the weak ψ-field perturbations the framework predicts.&lt;br /&gt;
&lt;br /&gt;
== Discovery ==&lt;br /&gt;
&lt;br /&gt;
SR was originally proposed by Benzi, Sutera, and Vulpiani (1981, &amp;#039;&amp;#039;Journal of Physics A&amp;#039;&amp;#039; 14: L453) as a possible explanation for the periodicity of Earth&amp;#039;s ice ages. The Earth&amp;#039;s climate system, viewed as a bistable system between glacial and interglacial states, was found to respond resonantly to weak Milankovitch orbital forcing — only with the help of internal climatic noise.&lt;br /&gt;
&lt;br /&gt;
The Earth-climate application remains contested, but the underlying mathematical phenomenon is rigorous and has been demonstrated in many physical systems.&lt;br /&gt;
&lt;br /&gt;
== Mathematical core ==&lt;br /&gt;
&lt;br /&gt;
Consider a bistable system — a particle in a double-well potential — driven by a weak periodic force and a white-noise background:&lt;br /&gt;
&lt;br /&gt;
  dx/dt = − dV/dx + A · cos(ω t) + ξ(t)&lt;br /&gt;
&lt;br /&gt;
with double-well potential V(x) = − x&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;/2 + x&amp;lt;sup&amp;gt;4&amp;lt;/sup&amp;gt;/4 (or similar), weak periodic forcing A · cos(ω t), and Gaussian noise ξ(t) with variance σ&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Noise-free&amp;#039;&amp;#039;&amp;#039; (σ = 0) and weak forcing (A &amp;lt; threshold for crossing the barrier): particle stays in one well; no signal detection.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Strong noise&amp;#039;&amp;#039;&amp;#039; (σ very large): particle randomly jumps between wells regardless of forcing; signal swamped.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Optimal noise&amp;#039;&amp;#039;&amp;#039; (σ tuned to match forcing): noise-assisted barrier-crossings synchronise with the periodic forcing. Output SNR is maximised at this optimum.&lt;br /&gt;
&lt;br /&gt;
The Kramers escape rate r&amp;lt;sub&amp;gt;K&amp;lt;/sub&amp;gt; = (ω&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;/2π) · exp(−ΔV/σ&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;) controls the spontaneous crossing rate; SR occurs when 2 · r&amp;lt;sub&amp;gt;K&amp;lt;/sub&amp;gt; ≈ ω/(2π).&lt;br /&gt;
&lt;br /&gt;
== Universal phenomenology ==&lt;br /&gt;
&lt;br /&gt;
The SR phenomenon is observed in:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Bistable electronic circuits&amp;#039;&amp;#039;&amp;#039; — direct laboratory demonstration.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Lasers&amp;#039;&amp;#039;&amp;#039; near bistability.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Climate models&amp;#039;&amp;#039;&amp;#039; (original Benzi-Sutera-Vulpiani application).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Sensory neurons&amp;#039;&amp;#039;&amp;#039; — see &amp;quot;biological SR&amp;quot; below.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Magnetic systems&amp;#039;&amp;#039;&amp;#039; near phase transitions.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Stochastic computing&amp;#039;&amp;#039;&amp;#039; — modern noise-driven analog computers.&lt;br /&gt;
&lt;br /&gt;
== Biological stochastic resonance ==&lt;br /&gt;
&lt;br /&gt;
The most striking applications are biological:&lt;br /&gt;
&lt;br /&gt;
=== 1. Crayfish mechanoreceptors ===&lt;br /&gt;
&lt;br /&gt;
Douglass, Wilkens, Pantazelou, Moss (1993, &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 365: 337). Crayfish mechanoreceptors detect weak water vibrations from prey (and predators). The system is intrinsically noisy. SR analysis shows that the receptor&amp;#039;s detection of weak periodic vibrations is &amp;#039;&amp;#039;&amp;#039;optimised at intermediate noise levels&amp;#039;&amp;#039;&amp;#039; — too little noise misses the signal; too much noise swamps it.&lt;br /&gt;
&lt;br /&gt;
This was the first clean biological demonstration of SR and made it clear that &amp;#039;&amp;#039;&amp;#039;biology uses noise constructively&amp;#039;&amp;#039;&amp;#039; rather than fighting it.&lt;br /&gt;
&lt;br /&gt;
=== 2. Cricket cercal system ===&lt;br /&gt;
&lt;br /&gt;
Levin and Miller (1996). The cricket&amp;#039;s wind-receptor system at the cercus shows SR-type behaviour in its detection of weak air movements.&lt;br /&gt;
&lt;br /&gt;
=== 3. Human balance and tactile perception ===&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Tactile detection&amp;#039;&amp;#039;&amp;#039; (Collins, Imhoff, Grigg 1996) — adding noise vibration to fingertips &amp;#039;&amp;#039;&amp;#039;lowers the threshold&amp;#039;&amp;#039;&amp;#039; for detecting weak tactile signals. Used clinically for diabetic-neuropathy patients with sensory loss.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Postural balance&amp;#039;&amp;#039;&amp;#039; (Priplata et al. 2003) — vibrating insoles reduce sway in elderly subjects, using SR principles.&lt;br /&gt;
&lt;br /&gt;
=== 4. Neural-network SR ===&lt;br /&gt;
&lt;br /&gt;
Networks of bistable neurons exhibit SR collectively. The dynamics of population firing in response to weak periodic input is enhanced by intrinsic neural noise.&lt;br /&gt;
&lt;br /&gt;
=== 5. Hearing ===&lt;br /&gt;
&lt;br /&gt;
Cochlear hair-cell mechanotransduction shows SR-type behaviour, with intrinsic mechanical noise enhancing detection of weak tones near threshold.&lt;br /&gt;
&lt;br /&gt;
== Framework relevance ==&lt;br /&gt;
&lt;br /&gt;
In the [[Psionics|psionic framework]]:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Weak ψ-field forcing&amp;#039;&amp;#039;&amp;#039; on neural systems would be a subliminal periodic drive: too weak to cross firing thresholds by itself.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;SR amplification&amp;#039;&amp;#039;&amp;#039;: neuronal noise (synaptic, channel, thermal) provides the noise background. SR predicts that a fraction of weak ψ-forcing is converted to detectable firing-rate modulation — at intermediate noise levels.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Cognitive correlates&amp;#039;&amp;#039;&amp;#039;: the brain operates in a regime where intrinsic noise is large enough for SR to amplify weak external forcing. This is plausibly why anomalous-cognition signals are detectable at all (the brain integrates many noisy SR amplifiers across the cortex).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Quantitative prediction&amp;#039;&amp;#039;&amp;#039;: the magnitude of ψ-mediated anomalous-cognition signals should depend on the brain&amp;#039;s noise level. Deep meditation (low noise) might be LESS sensitive to weak ψ-forcing than alert waking (moderate noise).&lt;br /&gt;
&lt;br /&gt;
This is a non-trivial prediction that distinguishes the framework from &amp;quot;consciousness amplifies psi&amp;quot; intuitions: SR predicts moderate noise enhances detection.&lt;br /&gt;
&lt;br /&gt;
== Sanity checks ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;No signal, only noise&amp;#039;&amp;#039;&amp;#039; → no SR; pure noise output. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;No noise, weak signal&amp;#039;&amp;#039;&amp;#039; → no SR; signal undetected. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Optimal noise level&amp;#039;&amp;#039;&amp;#039; → maximum output SNR. ✓ Demonstrated in many systems.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Very strong signal&amp;#039;&amp;#039;&amp;#039; → SR not needed; signal detected at all noise levels. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;ψ → 0&amp;#039;&amp;#039;&amp;#039; (in framework) → SR still operates on classical sensory signals; no framework-specific implications. ✓ ([[Sanity_Check_Limits]] §12.)&lt;br /&gt;
&lt;br /&gt;
== Open questions for the framework ==&lt;br /&gt;
&lt;br /&gt;
# Quantitative estimate of the SR-amplification factor for ψ-forcing of cortical networks.&lt;br /&gt;
# Empirical test: do meditative-quietude states show altered SR-curves relative to waking?&lt;br /&gt;
# Is the brain&amp;#039;s noise level evolutionarily tuned for SR? (Strong indirect evidence yes, but not direct test.)&lt;br /&gt;
# Connection to [[Recurrent_Coherence_Theory|RCT]] spectral fingerprints: SR may select which spectral modes amplify weak forcing.&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[FitzHugh-Nagumo_Equations]]&lt;br /&gt;
* [[Wilson-Cowan_Model]]&lt;br /&gt;
* [[Recurrent_Coherence_Theory]]&lt;br /&gt;
* [[Bioelectromagnetism]]&lt;br /&gt;
* [[Biological_Substrate_of_Psi]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Benzi, R., Sutera, A., Vulpiani, A. (1981). &amp;quot;The mechanism of stochastic resonance.&amp;quot; &amp;#039;&amp;#039;Journal of Physics A: Mathematical and General&amp;#039;&amp;#039; 14: L453.&lt;br /&gt;
* Douglass, J. K., Wilkens, L., Pantazelou, E., Moss, F. (1993). &amp;quot;Noise enhancement of information transfer in crayfish mechanoreceptors by stochastic resonance.&amp;quot; &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 365: 337–340.&lt;br /&gt;
* Collins, J. J., Imhoff, T. T., Grigg, P. (1996). &amp;quot;Noise-enhanced tactile sensation.&amp;quot; &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 383: 770.&lt;br /&gt;
* Priplata, A. A., et al. (2003). &amp;quot;Vibrating insoles and balance control in elderly people.&amp;quot; &amp;#039;&amp;#039;The Lancet&amp;#039;&amp;#039; 362: 1123–1124.&lt;br /&gt;
* Gammaitoni, L., Hänggi, P., Jung, P., Marchesoni, F. (1998). &amp;quot;Stochastic resonance.&amp;quot; &amp;#039;&amp;#039;Reviews of Modern Physics&amp;#039;&amp;#039; 70: 223–287.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Dynamics]]&lt;br /&gt;
[[Category:Neuroscience]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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