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	<title>Excitons - Revision history</title>
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		<title>JonoThora: Phase N (01b): LaTeX restoration — promote Unicode display-math to &lt;math&gt;; lint-clean per tools/wiki_latex_lint.py</title>
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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;= Excitons =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Intermediate&lt;br /&gt;
| reading_time = 6 minutes&lt;br /&gt;
| prerequisites = [[Quasiparticle]]; basic semiconductor physics (electron-hole pairs, band gaps).&lt;br /&gt;
| if_too_advanced_see = [[Quasiparticle]]&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 = Non-relativistic; SI.&lt;br /&gt;
| units     = ℏ = reduced Planck; μ = reduced electron-hole mass; ε&amp;lt;sub&amp;gt;r&amp;lt;/sub&amp;gt; = relative dielectric constant.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Excitons&amp;#039;&amp;#039;&amp;#039; are bound states of an electron and a hole in a semiconductor or insulator. They are [[Quasiparticle|quasiparticles]] of charge-neutral electronic excitation — a hydrogen-like two-body system held together by Coulomb attraction in a screening dielectric environment.&lt;br /&gt;
&lt;br /&gt;
In the [[Psionics|psionic framework]], excitons are the key quasiparticle bridge between solid-state physics and biological [[Biological_Substrate_of_Psi|psi substrates]]: Frenkel excitons in molecular crystals (and in tryptophan networks of microtubules) are the substrate for &amp;#039;&amp;#039;&amp;#039;superradiant N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; scaling&amp;#039;&amp;#039;&amp;#039; that the framework predicts couples coherently to ψ.&lt;br /&gt;
&lt;br /&gt;
== Wannier-Mott excitons ==&lt;br /&gt;
&lt;br /&gt;
In conventional semiconductors with small effective masses and large dielectric constants (Si, GaAs, CdSe):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;E_n = -\,\frac{\mu\,e^4}{2\,\hbar^2\,\varepsilon_r^2\,n^2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
— hydrogen-like spectrum, with the binding energy scaled by μ/m&amp;lt;sub&amp;gt;e&amp;lt;/sub&amp;gt; and 1/ε&amp;lt;sub&amp;gt;r&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;. For typical III-V semiconductors:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Bohr radius&amp;#039;&amp;#039;&amp;#039; a&amp;lt;sub&amp;gt;X&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;*&amp;lt;/sup&amp;gt; = ε&amp;lt;sub&amp;gt;r&amp;lt;/sub&amp;gt; ℏ&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; / (μ e&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;) ~ 5–10 nm.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Binding energy&amp;#039;&amp;#039;&amp;#039; E&amp;lt;sub&amp;gt;X&amp;lt;/sub&amp;gt; ~ 2–25 meV (much less than the band gap).&lt;br /&gt;
* Excitons are &amp;#039;&amp;#039;&amp;#039;delocalised&amp;#039;&amp;#039;&amp;#039; across many unit cells.&lt;br /&gt;
&lt;br /&gt;
Wannier excitons are observed cleanly only at low temperatures (below E&amp;lt;sub&amp;gt;X&amp;lt;/sub&amp;gt;/k&amp;lt;sub&amp;gt;B&amp;lt;/sub&amp;gt; ~ 30 K) in conventional semiconductors. In wide-gap materials (ZnO, GaN, 2D semiconductors) they can persist to room temperature.&lt;br /&gt;
&lt;br /&gt;
== Frenkel excitons ==&lt;br /&gt;
&lt;br /&gt;
In molecular crystals, organic semiconductors, and biological molecules, excitons are &amp;#039;&amp;#039;&amp;#039;localised to a single molecule&amp;#039;&amp;#039;&amp;#039; (or small cluster) due to small dielectric constants and low molecular polarisabilities:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Binding energy&amp;#039;&amp;#039;&amp;#039; E&amp;lt;sub&amp;gt;X&amp;lt;/sub&amp;gt; ~ 100 meV to ~ 1 eV.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Spatial extent&amp;#039;&amp;#039;&amp;#039; ~ molecular size (1 nm or less).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Energy transfer between molecules&amp;#039;&amp;#039;&amp;#039; via dipole-dipole (Förster) or exchange (Dexter) coupling.&lt;br /&gt;
&lt;br /&gt;
Frenkel excitons are the photophysics of organic dyes, photosynthesis, and biological chromophores.&lt;br /&gt;
&lt;br /&gt;
== Förster resonance energy transfer (FRET) ==&lt;br /&gt;
&lt;br /&gt;
The rate of dipole-mediated energy transfer between two molecules at distance R:&lt;br /&gt;
&lt;br /&gt;
  k&amp;lt;sub&amp;gt;FRET&amp;lt;/sub&amp;gt; ∝ 1 / R&amp;lt;sup&amp;gt;6&amp;lt;/sup&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;Förster radius&amp;#039;&amp;#039;&amp;#039; R&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; — the distance at which transfer is 50% efficient — is typically 1–10 nm for biological chromophores. Below R&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;, transfer is fast (ps timescale); above, exponentially slow.&lt;br /&gt;
&lt;br /&gt;
FRET is the dominant energy-transfer mechanism in:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Photosynthetic antenna complexes&amp;#039;&amp;#039;&amp;#039; — light-harvesting chlorophyll arrays.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Förster microscopy&amp;#039;&amp;#039;&amp;#039; — molecular-distance ruler in cell biology.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Microtubule tryptophan networks&amp;#039;&amp;#039;&amp;#039; — see below.&lt;br /&gt;
&lt;br /&gt;
== Superradiance ==&lt;br /&gt;
&lt;br /&gt;
When N chromophores are within R&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; of each other and they share a coherent electronic state, their emission rate is enhanced from N (incoherent) to N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; (superradiant). This is the Dicke superradiance phenomenon, first proposed in 1954.&lt;br /&gt;
&lt;br /&gt;
The N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; enhancement is direct experimental evidence that the system is in a &amp;#039;&amp;#039;&amp;#039;collective coherent state&amp;#039;&amp;#039;&amp;#039; — distinguished from incoherent ensembles by the radiation pattern, lifetime, and intensity.&lt;br /&gt;
&lt;br /&gt;
== Microtubule excitons ==&lt;br /&gt;
&lt;br /&gt;
Tryptophan residues in tubulin form an exciton network:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Spacing&amp;#039;&amp;#039;&amp;#039; ~ 1.5–2.0 nm — well within Förster range.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Coupling&amp;#039;&amp;#039;&amp;#039; through tubulin&amp;#039;s α-helical structure.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Coherent excitonic states&amp;#039;&amp;#039;&amp;#039; demonstrated by Celardo et al. (2019) — see [[Celardo_Microtubule_Superradiance]].&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Superradiant emission&amp;#039;&amp;#039;&amp;#039; predicted to scale as N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; in a single microtubule (~ 10&amp;lt;sup&amp;gt;4&amp;lt;/sup&amp;gt; tryptophans).&lt;br /&gt;
&lt;br /&gt;
This is the central biological-substrate result: microtubule tryptophan excitons constitute a &amp;#039;&amp;#039;&amp;#039;room-temperature, biologically-occurring superradiant system&amp;#039;&amp;#039;&amp;#039; — exactly the kind of coherent matter excitation that the framework predicts couples enhancedly to ψ.&lt;br /&gt;
&lt;br /&gt;
== Engineered exciton systems ==&lt;br /&gt;
&lt;br /&gt;
Solid-state exciton systems offer related substrates:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;GaAs/AlGaAs quantum wells&amp;#039;&amp;#039;&amp;#039; — 2D excitons, used as building blocks for exciton-polariton condensates.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;TMDC monolayers&amp;#039;&amp;#039;&amp;#039; (MoS&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, WSe&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) — room-temperature excitons with binding energies ~ 0.5 eV.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Perovskite films&amp;#039;&amp;#039;&amp;#039; — excitons with strong photoluminescence and strong coupling to plasmonic substrates.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Organic semiconductors&amp;#039;&amp;#039;&amp;#039; — pentacene, anthracene; Frenkel excitons with well-characterised properties.&lt;br /&gt;
&lt;br /&gt;
All these substrates are candidates for engineered ψ-coupling devices via the exciton → photon → ψ chain.&lt;br /&gt;
&lt;br /&gt;
== Coupling to ψ ==&lt;br /&gt;
&lt;br /&gt;
In the framework:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Coherent exciton states&amp;#039;&amp;#039;&amp;#039; (whether Frenkel in microtubules or Wannier in quantum wells) are ψ-source channels via the αψ F&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt; F&amp;lt;sup&amp;gt;μν&amp;lt;/sup&amp;gt; vertex.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; superradiance&amp;#039;&amp;#039;&amp;#039; gives a factor-N enhancement of ψ-coupling per exciton, compared to incoherent emission.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Bio-substrate convergence&amp;#039;&amp;#039;&amp;#039;: microtubule exciton networks are the natural-occurring example of this physics — the framework&amp;#039;s claim that biological psi-coupling is enhanced compared to non-coherent matter is grounded in well-established Frenkel-exciton/superradiance theory.&lt;br /&gt;
&lt;br /&gt;
== Sanity checks ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Large R limit&amp;#039;&amp;#039;&amp;#039; → FRET rate goes to zero; excitons in different molecules are independent. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Single-exciton limit&amp;#039;&amp;#039;&amp;#039; → reduces to standard molecular electronic transitions. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Superradiance&amp;#039;&amp;#039;&amp;#039; → N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; scaling demonstrated in atomic and molecular ensembles. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;ψ → 0&amp;#039;&amp;#039;&amp;#039; (in framework) → exciton physics intact; no ψ-coupling. ✓ ([[Sanity_Check_Limits]] §5.)&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Quasiparticle]]&lt;br /&gt;
* [[Phonons]]&lt;br /&gt;
* [[Polaritons]]&lt;br /&gt;
* [[Microtubule]]&lt;br /&gt;
* [[Celardo_Microtubule_Superradiance]]&lt;br /&gt;
* [[Biological_Substrate_of_Psi]]&lt;br /&gt;
* [[Coherent_Quantum_Effects_in_Biology]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Dicke, R. H. (1954). &amp;quot;Coherence in spontaneous radiation processes.&amp;quot; &amp;#039;&amp;#039;Physical Review&amp;#039;&amp;#039; 93: 99.&lt;br /&gt;
* Förster, T. (1948). &amp;quot;Zwischenmolekulare Energiewanderung und Fluoreszenz.&amp;quot; &amp;#039;&amp;#039;Annalen der Physik&amp;#039;&amp;#039; 437: 55–75.&lt;br /&gt;
* Knox, R. S. (1963). &amp;#039;&amp;#039;Theory of Excitons.&amp;#039;&amp;#039; Academic Press.&lt;br /&gt;
* Celardo, G. L., Angeli, M., Craddock, T. J. A., Kurian, P. (2019). &amp;quot;On the existence of superradiant excitonic states in microtubules.&amp;quot; &amp;#039;&amp;#039;New Journal of Physics&amp;#039;&amp;#039; 21: 023005.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Quasiparticles]]&lt;br /&gt;
[[Category:Photophysics]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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