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 :
longitudinal optical phonons (LO phonons)
polaritons (transverse em field + TO phonons)
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.
↑
Max Born, Kun Huang, Dynamical Theory of Crystal Lattices, Oxford University Press, 1954 (ISBN9780198503699), « Chapter 8 : Infrared Dispersion and the Retardation Effect on Lattice Vibrations »
↑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.
e=1.602e-19;hbar=1.05457168e-34;c=2.9978e8;ang=1e-10;omega0=45.4e-3*e/hbar;%conversion meV->rd/sOm=61e-3*e/hbar;chi=7.5;k=linspace(0,0.0004/ang)';y1=omega0*ones(size(k));%uncoupled phonon dispersiony2=c*k/sqrt(1+chi);%uncoupled photon dispersiony3=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 polaritonsy5=sqrt((-a2-D)./(2*a1));%lower polaritonsplot(k*ang,[y1y2]*1000*hbar/e,'r--','Linewidth',1.8);holdonplot(k*ang,[y3y4y5]*1000*hbar/e,'k','Linewidth',1.8);holdoffaxis([00.00043560]);set(gca,'FontSize',18,'TickLength',[.02.02],'LineWidth',1.5);xlabel('k (A^{-1})');%A to be replacedylabel('h\omega (meV)');%h to be replaced
Licensing
I, the copyright holder of this work, hereby publish it under the following licenses:
Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and no Back-Cover Texts. A copy of the license is included in the section entitled GNU Free Documentation License.http://www.gnu.org/copyleft/fdl.htmlGFDLGNU Free Documentation Licensetruetrue
to share – to copy, distribute and transmit the work
to remix – to adapt the work
Under the following conditions:
attribution – You must give appropriate credit, provide a link to the license, and indicate if changes were made. You may do so in any reasonable manner, but not in any way that suggests the licensor endorses you or your use.
share alike – If you remix, transform, or build upon the material, you must distribute your contributions under the same or compatible license as the original.
{{Information |Description={{en|1=Dispersion relation of phonon polaritons with parameters corresponding to GaP.}} {{fr|1=Relation de dispersion des polaritons avec des paramètres correspondant au GaP.}} |Source=travail personnel (own work) |Author=[[Use