April 1977 | Pochi Yeh, Ammon Yariv, and Chi-Shain Hong
This paper presents a general theory for electromagnetic wave propagation in periodic stratified media. The authors analyze the propagation of electromagnetic radiation in media with finite, semi-infinite, and infinite extent. They use a diagonalization of the unit cell translation operator to derive exact solutions for Bloch waves, dispersion relations, and band structures. The theory is shown to have strong formal similarities to the quantum theory of electrons in crystals, making use of concepts such as Bloch modes, forbidden gaps, evanescent waves, and surface waves.
The paper discusses various applications of periodic media, including integrated optics and laser technology. It considers a variety of experimental situations, such as Bragg waveguides, birefringence, group velocity at arbitrary directions, phase matching in nonlinear optical applications, multichannel waveguides, and optical surface waves. The authors also consider the important problem of propagation and reflection in media with periodic gain and loss alternation, which is relevant to x-ray laser oscillation in artificially layered media.
The paper introduces a matrix method and translation operator to analyze the propagation of electromagnetic waves in periodic stratified media. The authors derive the translation matrix, which relates the complex amplitudes of the incident and reflected plane waves in one layer of a unit cell to those of the equivalent layer in the next unit cell. The matrix is unimodular, meaning its determinant is 1.
The paper then discusses Bloch waves and band structures in periodic media. It shows that the periodic medium can be considered as a one-dimensional lattice invariant under lattice translation. The Bloch wave is of the form $ E_K(x,z) = E_K(x)e^{iKx}e^{i\beta z} $, where $ E_K(x) $ is periodic with period $ \Lambda $. The Bloch wave number $ K $ is related to the dispersion relation between $ \omega $, $ \beta $, and $ K $.
The paper also discusses Bragg reflectors, which are periodic structures that can be used to reflect light. The authors derive an analytic expression for the reflectivity of a multilayer reflector, which is shown to be a function of the number of periods and the angle of incidence.
The paper then discusses guided waves in periodic media, including symmetric and asymmetric types of waveguides. The authors derive the mode dispersion relations and field distributions for these waveguides, showing that the number of modes in each band is equal to the number of channels.
The paper also discusses electromagnetic surface waves in periodic media. These waves are bounded by the interface between two semi-infinite systems and are localized near the surface. The authors show that the existence of surface states is due to the fact that the propagation conditions in the periodic medium correspond to a "forbidden" band.
The paper concludes by summarizing the key findings and showing that many aspects of the optics of periodic layered media are closely analogous to the physics of electrons in crystals. The authorsThis paper presents a general theory for electromagnetic wave propagation in periodic stratified media. The authors analyze the propagation of electromagnetic radiation in media with finite, semi-infinite, and infinite extent. They use a diagonalization of the unit cell translation operator to derive exact solutions for Bloch waves, dispersion relations, and band structures. The theory is shown to have strong formal similarities to the quantum theory of electrons in crystals, making use of concepts such as Bloch modes, forbidden gaps, evanescent waves, and surface waves.
The paper discusses various applications of periodic media, including integrated optics and laser technology. It considers a variety of experimental situations, such as Bragg waveguides, birefringence, group velocity at arbitrary directions, phase matching in nonlinear optical applications, multichannel waveguides, and optical surface waves. The authors also consider the important problem of propagation and reflection in media with periodic gain and loss alternation, which is relevant to x-ray laser oscillation in artificially layered media.
The paper introduces a matrix method and translation operator to analyze the propagation of electromagnetic waves in periodic stratified media. The authors derive the translation matrix, which relates the complex amplitudes of the incident and reflected plane waves in one layer of a unit cell to those of the equivalent layer in the next unit cell. The matrix is unimodular, meaning its determinant is 1.
The paper then discusses Bloch waves and band structures in periodic media. It shows that the periodic medium can be considered as a one-dimensional lattice invariant under lattice translation. The Bloch wave is of the form $ E_K(x,z) = E_K(x)e^{iKx}e^{i\beta z} $, where $ E_K(x) $ is periodic with period $ \Lambda $. The Bloch wave number $ K $ is related to the dispersion relation between $ \omega $, $ \beta $, and $ K $.
The paper also discusses Bragg reflectors, which are periodic structures that can be used to reflect light. The authors derive an analytic expression for the reflectivity of a multilayer reflector, which is shown to be a function of the number of periods and the angle of incidence.
The paper then discusses guided waves in periodic media, including symmetric and asymmetric types of waveguides. The authors derive the mode dispersion relations and field distributions for these waveguides, showing that the number of modes in each band is equal to the number of channels.
The paper also discusses electromagnetic surface waves in periodic media. These waves are bounded by the interface between two semi-infinite systems and are localized near the surface. The authors show that the existence of surface states is due to the fact that the propagation conditions in the periodic medium correspond to a "forbidden" band.
The paper concludes by summarizing the key findings and showing that many aspects of the optics of periodic layered media are closely analogous to the physics of electrons in crystals. The authors