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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;= Polaritons =&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 quantum optics (cavity QED, Rabi splitting).&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; g = Rabi (coupling) frequency.&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Polaritons&amp;#039;&amp;#039;&amp;#039; are hybrid [[Quasiparticle|quasiparticles]] formed by the strong coupling of a photon to a matter excitation. The matter excitation can be a phonon, exciton, magnon, plasmon, or any other long-lived collective mode. When the coupling g exceeds the linewidth of both constituents, the system is in the &amp;#039;&amp;#039;&amp;#039;strong-coupling regime&amp;#039;&amp;#039;&amp;#039; and the eigenstates are no longer photon-like or matter-like — they are hybrid &amp;#039;&amp;#039;&amp;#039;polaritons&amp;#039;&amp;#039;&amp;#039; with properties of both.&lt;br /&gt;
&lt;br /&gt;
Polaritons are the basis of much modern cavity-QED, hybrid quantum information, and microcavity-based devices. In the [[Psionics|psionic framework]], polariton substrates inherit the ψ-coupling of their matter component while gaining the engineering control of their photon component.&lt;br /&gt;
&lt;br /&gt;
== Types of polaritons ==&lt;br /&gt;
&lt;br /&gt;
| Name | Photon partner | Matter partner |&lt;br /&gt;
|---|---|---|&lt;br /&gt;
| Phonon polariton | IR/optical photon | Polar optical phonon |&lt;br /&gt;
| Exciton polariton | Visible photon (in microcavity) | Wannier or Frenkel exciton |&lt;br /&gt;
| Magnon polariton | Microwave photon (in cavity) | Magnon |&lt;br /&gt;
| Plasmon polariton | Optical / IR photon | Surface plasmon |&lt;br /&gt;
| Cavity polariton | Microwave / optical | Atomic / molecular two-level system |&lt;br /&gt;
&lt;br /&gt;
== Anti-crossing dispersion ==&lt;br /&gt;
&lt;br /&gt;
When a photon mode at frequency ω&amp;lt;sub&amp;gt;ph&amp;lt;/sub&amp;gt;(&amp;#039;&amp;#039;&amp;#039;k&amp;#039;&amp;#039;&amp;#039;) is coupled to a matter mode at frequency ω&amp;lt;sub&amp;gt;matter&amp;lt;/sub&amp;gt;(&amp;#039;&amp;#039;&amp;#039;k&amp;#039;&amp;#039;&amp;#039;) with coupling strength g, the polariton dispersion is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\omega_\pm(\mathbf{k}) = \tfrac{1}{2}\!\left[\,\omega_{\text{ph}}(k) + \omega_{\text{matter}}(k) \pm \sqrt{[\omega_{\text{ph}}(k) - \omega_{\text{matter}}(k)]^2 + 4 g^2}\,\right]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At resonance (ω&amp;lt;sub&amp;gt;ph&amp;lt;/sub&amp;gt; = ω&amp;lt;sub&amp;gt;matter&amp;lt;/sub&amp;gt;), the splitting is &amp;#039;&amp;#039;&amp;#039;Δω = 2g&amp;#039;&amp;#039;&amp;#039; — the &amp;#039;&amp;#039;&amp;#039;Rabi splitting&amp;#039;&amp;#039;&amp;#039;. The avoided crossing is the experimental signature of strong coupling.&lt;br /&gt;
&lt;br /&gt;
== Strong-coupling regime ==&lt;br /&gt;
&lt;br /&gt;
Strong coupling requires g &amp;gt; κ&amp;lt;sub&amp;gt;ph&amp;lt;/sub&amp;gt;, γ&amp;lt;sub&amp;gt;matter&amp;lt;/sub&amp;gt;, where κ&amp;lt;sub&amp;gt;ph&amp;lt;/sub&amp;gt; is the photon decay rate (cavity linewidth) and γ&amp;lt;sub&amp;gt;matter&amp;lt;/sub&amp;gt; is the matter decoherence rate. In this regime:&lt;br /&gt;
&lt;br /&gt;
* Polaritons are well-defined eigenstates.&lt;br /&gt;
* Energy exchange between photon and matter occurs &amp;#039;&amp;#039;&amp;#039;coherently&amp;#039;&amp;#039;&amp;#039;, not as an irreversible emission/absorption.&lt;br /&gt;
* The system supports quantum-coherent operations: vacuum Rabi splitting, polariton condensation, quantum-information protocols.&lt;br /&gt;
&lt;br /&gt;
Strong coupling is now routinely achieved in:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Optical microcavities&amp;#039;&amp;#039;&amp;#039; (DBR mirrors, photonic-crystal cavities).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Superconducting microwave cavities&amp;#039;&amp;#039;&amp;#039; coupled to qubits.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Plasmonic nanocavities&amp;#039;&amp;#039;&amp;#039; (single-emitter strong coupling, 2016–2024).&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Cavity-magnonics&amp;#039;&amp;#039;&amp;#039; (Tabuchi 2014 onward).&lt;br /&gt;
&lt;br /&gt;
== Polariton condensation ==&lt;br /&gt;
&lt;br /&gt;
At sufficient density and low enough temperature, &amp;#039;&amp;#039;&amp;#039;exciton-polariton condensates&amp;#039;&amp;#039;&amp;#039; form Bose-Einstein-like coherent states. First demonstrated by Kasprzak et al. (2006, &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 443: 409) in CdTe microcavities; later in GaAs and organic semiconductor cavities at room temperature.&lt;br /&gt;
&lt;br /&gt;
Polariton condensates are &amp;#039;&amp;#039;&amp;#039;non-equilibrium Bose-Einstein condensates&amp;#039;&amp;#039;&amp;#039; — they are continuously pumped and decay. Despite this, they exhibit superfluid-like coherence, vortices, and other classic BEC signatures.&lt;br /&gt;
&lt;br /&gt;
== Plasmon-exciton (plexcitonic) coupling ==&lt;br /&gt;
&lt;br /&gt;
A particularly active research area combines plasmonic and excitonic modes:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Plexcitons&amp;#039;&amp;#039;&amp;#039; — hybrid states formed by plasmonic nanoparticles strongly coupled to molecular excitons.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Single-emitter strong coupling&amp;#039;&amp;#039;&amp;#039; — demonstrated at room temperature with single molecules in plasmonic nanocavities (Chikkaraddy et al. 2016, &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 535: 127).&lt;br /&gt;
&lt;br /&gt;
Plexcitons offer the strongest known light-matter coupling per unit volume — a regime where the coupling constant g is comparable to the matter excitation energy itself.&lt;br /&gt;
&lt;br /&gt;
== Polariton chemistry ==&lt;br /&gt;
&lt;br /&gt;
A frontier topic (2015–2024): when molecules are placed in a strongly-coupled microcavity, &amp;#039;&amp;#039;&amp;#039;chemical reaction rates and pathways can be modified&amp;#039;&amp;#039;&amp;#039; by the polariton dressing. This is non-trivial: the cavity affects internal molecular electronics through the strong-coupling regime.&lt;br /&gt;
&lt;br /&gt;
This is independent confirmation that &amp;#039;&amp;#039;&amp;#039;photonic engineering can modulate matter at the level of chemical kinetics&amp;#039;&amp;#039;&amp;#039; — a precedent for the framework&amp;#039;s claim that EM fields modulate ψ-coupling to molecular and biological systems.&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;Polariton modes inherit the ψ-coupling of their matter component&amp;#039;&amp;#039;&amp;#039;. A magnon polariton couples to ψ via its magnon character; an exciton polariton via its exciton character.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Engineering advantage&amp;#039;&amp;#039;&amp;#039;: polaritons are easier to drive coherently than bare matter excitations, because they have a strong photonic component that can be driven by external lasers or microwave sources.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Polariton condensates&amp;#039;&amp;#039;&amp;#039; provide a controlled, macroscopic, coherent N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;-scaling ψ-source — the solid-state analogue of microtubule superradiance.&lt;br /&gt;
&lt;br /&gt;
== Sanity checks ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Weak coupling (g → 0)&amp;#039;&amp;#039;&amp;#039; → uncoupled photon and matter modes. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Pure photon limit (matter mode absent)&amp;#039;&amp;#039;&amp;#039; → recovers cavity QED. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Vacuum Rabi splitting&amp;#039;&amp;#039;&amp;#039; → measured in many systems. ✓&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;ψ → 0&amp;#039;&amp;#039;&amp;#039; (in framework) → polariton 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;
* [[Magnons]]&lt;br /&gt;
* [[Plasmons]]&lt;br /&gt;
* [[Excitons]]&lt;br /&gt;
* [[Psionic_Device_Overview]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Hopfield, J. J. (1958). &amp;quot;Theory of the contribution of excitons to the complex dielectric constant of crystals.&amp;quot; &amp;#039;&amp;#039;Physical Review&amp;#039;&amp;#039; 112: 1555.&lt;br /&gt;
* Kasprzak, J., et al. (2006). &amp;quot;Bose-Einstein condensation of exciton polaritons.&amp;quot; &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 443: 409–414.&lt;br /&gt;
* Tabuchi, Y., et al. (2014). &amp;quot;Hybridizing ferromagnetic magnons and microwave photons in the quantum limit.&amp;quot; &amp;#039;&amp;#039;Physical Review Letters&amp;#039;&amp;#039; 113: 083603.&lt;br /&gt;
* Chikkaraddy, R., et al. (2016). &amp;quot;Single-molecule strong coupling at room temperature in plasmonic nanocavities.&amp;quot; &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 535: 127–130.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Quasiparticles]]&lt;br /&gt;
[[Category:Cavity QED]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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