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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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2 Chapter 1 Introduction<br />

incident wave<br />

t = 0.62s<br />

t = 1.00s<br />

reflected wave<br />

t = 1.25s<br />

reflected wave<br />

transmitted wave<br />

incident wave<br />

t = 0.62s<br />

t = 1.00s<br />

reflected wave<br />

t = 1.25s<br />

reflected wave<br />

transmitted wave<br />

Figure 1.1 Illustration of the bandgap phenomenon for wave propagation in a onedimensional<br />

layered structure. The plots show the incident/transmitted wave pulses as<br />

well as the reflected wave pulse at three different time instances. Left plots: a single inclusion<br />

with different material properties. Right plots: Four equidistantly placed inclusions,<br />

where the distance between the inclusions combined with the material properties leads<br />

to in-phase reflections of the incident wave. With infinitely many inclusions present, a<br />

complete reflection of the wave will occur – known as the bandgap phenomenon.<br />

given along the vertical axis and the reduced wave vector given along the horizontal<br />

axis. Afrequency rangeappearsforwhich nomodesexist. Inthisgap(thebandgap)<br />

waves cannot propagate regardless of the direction. The small inserted figure shows<br />

theirreducible Brillouin zone (Brillouin,1953)spannedbythetriangleΓ−X−M−Γ.<br />

The zone relates to the smallest repetitive unit in the periodic material – the unit<br />

cell (it is here a quadratic cell) – as well as its symmetry properties. The irreducible<br />

Brillouin zone indicates the wave vectors which are necessary to investigate in order<br />

to completely describe wave propagation through the material. It turns out to be<br />

sufficient to examine the wave vectors corresponding to the triangular path 1 .<br />

About half a century later, in 1987, the discovery of the bandgap phenomenon<br />

for optical waves – photonic bandgaps – by John (1987) and Yablonovitch (1987)<br />

marks a major breakthrough in the field of electromagnetics. This finding had<br />

1 In principle the entire triangular area must be examined, but it is commonly accepted that it<br />

is sufficient to examine the wavevectorson the exterior triangular path. To the author’s knowledge<br />

no proof of this has been presented yet.

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