Dispersion relation of polaritons in GaP. Red curves are the uncoupled phonon and photon dispersion relations, black curves are the result of coupling (from top to bottom: upper polariton, LO phonon, lower polariton).

In physics, polaritons are quasiparticles resulting from strong coupling of electromagnetic waves with an electric or magnetic dipole-carrying excitation. They are an expression of the common quantum phenomenon known as level repulsion, also known as the avoided crossing principle. Polaritons describe the crossing of the dispersion of light with any interacting resonance.


  • History 1
  • Types 2
  • Principles 3
  • See also 4
  • References 5
  • Further reading 6
  • External links 7


Oscillations in ionized gases were observed by Tonks and Langmuir in 1929. Collective interactions were published by David Pines and David Bohm in 1952 and plasmons were described in silver by Fröhlich and Pelzer in 1955. Ritchie predicted surface plasmons in 1957, then Ritchie and Eldridge published experiments and predictions of emitted photons from irradiated metal foils in 1962. Andreas Otto first published on surface plasmon-polaritons in Zeitschrift fur Physik in 1968.


A polariton is the result of the mixing of a photon with an excitation of a material. The following are types of polaritons:


Whenever the polariton picture is valid, the model of photons propagating freely in crystals is insufficient. A major feature of polaritons is a strong dependency of the propagation speed of light through the crystal on the frequency. For exciton-polaritons, rich experimental results on various aspects have been gained in copper (I) oxide.

The polariton is a bosonic quasiparticle, and should not be confused with the polaron (a fermionic one), which is an electron plus an attached phonon cloud. Polaritons were first considered theoretically by Kirill Borisovich Tolpygo,[2][3] a Ukrainian physicist, and were initially termed light-excitons in Ukrainian and Russian scientific literature.

See also


  1. ^ N. Eradat "etal", Evidence for braggoriton excitations in opal photonic crystals infiltrated with highly polarizable dyes, Appl. Phys. Lett. 80, 3491 (2002).
  2. ^ Tolpygo, Kirill Borisovich
  3. ^ K.B. Tolpygo, "Physical properties of a rock salt lattice made up of deformable ions," Zh.Eks.Teor.Fiz. v.20, No 6, pp.497–509 (1950), in Russian. English translation: Ukrainian Journal of Physics, v.53, special issue (2008); http://ujp.bitp.kiev.ua/files/journals/53/si/53SI21p.pdf
  • Fano, U. (1956). "Atomic Theory of Electromagnetic Interactions in Dense Materials". Physical Review 103 (5): 1202–1218.  
  • Hopfield, J. J. (1958). "Theory of the Contribution of Excitons to the Complex Dielectric Constant of Crystals". Physical Review 112 (5): 1555–1567.  
  • Otto, A. Excitation of nonradiative surface plasma waves in silver by the method of frustrated total reflection. Z. Phys. 216, 398–410 (1968)

Further reading

  • Baker-Jarvis, J. (2012). "The Interaction of Radio-Frequency Fields With Dielectric Materials at Macroscopic to Mesoscopic Scales" (PDF).  

External links

  • YouTube animation explaining what is polariton in a semiconductor micro-resonator.