Resonant diffraction of electromagnetic waves from solids (a review)

• Published in: Physics of the solid state Vol. 55; no. 5; pp. 905 - 923
• Main Authors: Ivchenko, E. L., Poddubny, A. N.
• Format: Journal Article
• Language: English
• Published: Dordrecht SP MAIK Nauka/Interperiodica 01-05-2013; Springer
• Subjects: Analysis; Electromagnetism; Gamma rays; Invisibility; Nuclear radiation; Physics; Physics and Astronomy; Quantum wells; Reviews; Solid State Physics; Bragg Structure; Optical Lattice; Bragg Condition; Photonic Crystal; Stop Band
• DOI: 10.1134/S1063783413050120
• EISSN: 1090-6460
• ISSN: 1063-7834

The subject of the review is the diffraction of an electromagnetic wave on a periodic condensed matter where the Bragg condition is satisfied at the frequency of resonance excited in this medium. The Bragg systems known as resonant photonic crystals in general have been considered, and the propagation, reflection, transmission, and diffraction of electromagnetic radiation in different objects—(I) periodic quantum-well structures near the exciton resonance, (II) optical lattices of atoms cooled in a laser field, and (III) bulk crystals and multilayers with gamma-ray resonance intranuclear transitions—have been described in a unified context. The main attention has been paid to the steady-state linear diffraction, including resonant reflection and transmission, which is the best studied and allows a comparison of the three aforementioned systems with the aim of revealing specific characteristics and common features. A characteristic common property of the considered systems is the suppression of non-radiative channels and an inhomogeneous broadening of the resonance frequency. The second fundamental property of resonant photonic crystals is that the interaction of light with resonant excitation can occur in two regimes depending on the thickness of the sample. In the superradiant regime realized for a small number of resonant layers
N
(fine structures), the height of the peak and half-width of the reflection spectrum monotonically increase with increasing value of
N
. With a further increase in
N
, there occurs a transition to a photonic-crystal regime where the half-width of the reflection spectrum is saturated, which manifests itself in the form of an optical stop band. The theoretical description is illustrated by experimental spectra measured for all three resonant Bragg systems.