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By Peter Markos, Costas M. Soukoulis

This textbook deals the 1st unified therapy of wave propagation in digital and electromagnetic structures and introduces readers to the necessities of the move matrix approach, a robust analytical instrument that may be used to version and examine an array of difficulties touching on wave propagation in electrons and photons. it's geared toward graduate and complicated undergraduate scholars in physics, fabrics technology, electric and machine engineering, and arithmetic, and is perfect for researchers in photonic crystals, adverse index fabrics, left-handed fabrics, plasmonics, nonlinear results, and optics. Peter Markos and Costas Soukoulis commence by means of constructing the analogy among wave propagation in digital platforms and electromagnetic media after which express how the move matrix should be simply utilized to any form of wave propagation, comparable to electromagnetic, acoustic, and elastic waves. The move matrix process of the tight-binding version permits readers to appreciate its implementation quick and the entire strategies of solid-state physics are basically brought. Markos and Soukoulis then construct the dialogue of such subject matters as random structures and localized and delocalized modes round the move matrix, bringing impressive readability to the topic. overall inner mirrored image, Brewster angles, evanescent waves, floor waves, and resonant tunneling in left-handed fabrics are brought and taken care of intimately, as are vital new advancements like photonic crystals, unfavorable index fabrics, and floor plasmons. challenge units reduction scholars operating during the topic for the 1st time.

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Additional info for Wave Propagation: From Electrons to Photonic Crystals and Left-Handed Materials

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9 we see that the transmission is high when the wavelength of the electron is much larger than the barrier width. When b increases, the wave function inside the barrier decreases exponentially and, consequently, the transmission coefficient also decreases. This result again states that for a given ratio E /V0 the only important parameter, which determines transmission properties, is the ratio of the electron wavelength to the width of the barrier. 10. Here, however, we fix the parameter b = 2 and vary the energy of the electron.

30) and p2 n 2 En = − 1 for V0 < 0. 31) While n acquires all values 1, 2, . . 31) must be positive. 31) can be satisfied for any rectangular potential, independent of its height V0 and width . What is important is not the parameters of the potential themselves, but the ratio k / of the wavelength of the particle inside the barrier, k , to the barrier width = 2a. Note that, although sin 2k a = 0 also for k = 0, the transmission coefficient T is less than one in this case. 23) and lim k →0 sin 2k a = 2a.

14). 27)]. Solution. 150) we have for a unitary matrix S that det S det S† = 1. 151) On the other hand, ∗ ∗ ∗ ∗ det S† = S11 S22 − S12 S21 = [det S]∗ . 152) By combining the previous equations we obtain |det S| = 1. 60) for the transfer matrix. Solution. 154) 26 ■ Chapter 1 which can be written in the form + − W− L = r WL +tWR , + − W+ R = t WL +r WR . 155) we express W− R = t WL − t r WL . 155), we obtain    + −1 W R   t −rt r  = W− −t −1 r R   r t −1   W+ L   . 60). 131). Solution.

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