Re: Microwave structure
Metamaterials, as you know, show EpsR<0 or 0<=EpsR<1. This properties is inherited from the structure geometry rather than electrical properties. For example, consider an hypothetic material with negative refractive index. From transmission Snell's law, at the interface between an incident media and a metamaterial, the wave refraction is inverted and lies on the same side of the normal entering the material. Moreover, phase fronts and power flux move along opposite directions. Some applications: cloacking devices, superlenses, agile antennas.
I worked on materials with a positive but less than 1 refraction index, so called metamaterial grids. These structures have the characteristic of an almost 0 refraction angle. In a few words, given any antenna, 2 or 3 metallic grids are placed at a proper distance over the antenna itself. The gratings behave as a kind of array of convergent microlenses. Distance from antenna and grid periodicity must be correctly chosen not to significantly affect the antenna input impedance and to obtain the desired gain. The wave incident on grids from antenna is refracted with a near-zero angle (refraction index close to zero), so the two grids act like a metamaterial. As consequence, beam-width reduces, with a great improvement of antenna gain in broadside direction.
I.