Summary

This image presents the dispersion relation of phonon polaritons according to a simple theory^[1], giving the two following dispersion relations for the coupled optical phonon/electromagnetic field system :

1. longitudinal optical phonons (LO phonons)
   ${\displaystyle \omega ^{2}=\omega _{0}^{2}+{\frac {\Omega ^{2}}{1+\chi _{\infty }}}={\text{const}};}$
2. polaritons (transverse em field + TO phonons)
   ${\displaystyle \mathbf {k} ^{2}={\frac {\omega ^{2}}{c^{2}}}\left[1+\chi _{\infty }+{\frac {\Omega ^{2}}{\omega _{0}^{2}-\omega ^{2}}}\right].}$

The dashed red curves correspond to the uncoupled modes (photons and phonons: Ω = 0), and the black curves represent solutions of the above equations with parameters chosen to fit the dispersion relation of polaritons in GaP^[2], giving

Uncoupled optical phonon frequency

ω₀ = 45.4 meV

Coupling parameter

Ω = 61 meV

Electric susceptibility

χ_∞ = 7.5

Note that k is very small compared to π/a.

1. ↑ Max Born, Kun Huang, Dynamical Theory of Crystal Lattices, Oxford University Press, 1954 (ISBN 9780198503699), « Chapter 8 : Infrared Dispersion and the Retardation Effect on Lattice Vibrations »
2. ↑ C. H. Henry and J. J. Hopfield, Raman Scattering by Polaritons, Phys. Rev. Lett. 15, 964 - 966 (1965).

(further minor editing and conversion to svg done with inkscape)

Summary

DescriptionPhonon polaritons.svg	English: Dispersion relation of phonon polaritons with parameters corresponding to GaP. Français : Relation de dispersion des polaritons avec des paramètres correspondant au GaP.
Date	15 November 2008
Source	Own work
Author	Mathieu Perrin
SVG development InfoField	The SVG code is valid.   This diagram was created with MATLAB.
Source code InfoField	MATLAB code e=1.602e-19; hbar = 1.05457168e-34; c=2.9978e8; ang=1e-10; omega0=45.4e-3*e/hbar; %conversion meV->rd/s Om=61e-3*e/hbar; chi=7.5; k=linspace(0,0.0004/ang)'; y1=omega0*ones(size(k)); %uncoupled phonon dispersion y2=c*k/sqrt(1+chi); %uncoupled photon dispersion y3=sqrt(y1.^2+Om^2/(1+chi));%longitudinal phonons %solve for omega in %k^2*c^2=omega^2*(1+chi+Om^2/(omega0^2-omega^2)) a1 = (1+chi)*ones(size(k)); a2 = -((1+chi)*omega0^2+k.^2*c^2+Om^2); a3 = k.^2*c^2*omega0^2; D = sqrt(a2.^2-4*a1.*a3); y4=sqrt((-a2+D)./(2*a1));%upper polaritons y5=sqrt((-a2-D)./(2*a1));%lower polaritons plot(k*ang, [y1 y2]*1000*hbar/e,'r--','Linewidth',1.8); hold on plot(k*ang, [y3 y4 y5]*1000*hbar/e,'k','Linewidth',1.8); hold off axis([0 0.0004 35 60]); set(gca,'FontSize',18,'TickLength',[.02 .02],'LineWidth',1.5); xlabel('k (A^{-1})'); %A to be replaced ylabel('h\omega (meV)'); %h to be replaced

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