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This Defense Intelligence Reference Document from the Defense Intelligence Agency, dated 6 April 2010, reviews electromagnetic and optical metamaterials for aerospace use. It was produced in FY 2009 under the Advanced Aerospace Weapon System Applications (AAWSA) Program. The report covers super-lenses and hyper-lenses for imaging objects smaller than the diffraction limit, slowing light to shrink components, energy-harvesting absorbers, and one-way chiral devices. It concludes that metamaterials matter for aerospace because they allow smaller, lighter components.
UNCLASSIFIED,) I OR OFFICl:ili!L U9! 9Hl!\Z slowed down and/or stopped light, the schematic shown in Figure 13 provides some key ideas. Moreover, the prospect of producing a low-loss negative index material in the optical domain still remains somewhat distant. Therefore, it may be worthwhile to examine other approaches to slowing down light that have emerged in the past few years. Stopping and/or slowing down light is an old idea originating from the atomic concept of Electromagnetically Induced Transparency (EIT). The phenomenon has been considered to be purely quantum mechanical until several groups have demonstrated that it has some classical analogies (Reference 31). Remarkably, at least one group has demonstrated in the past year that EIT can be achieved using plasmonic metamaterials (Reference 32). The idea is to create a plasmonic "molecule" consisting of a radiative element coupled with a subradiant (dark) element. The. plasmonic molecule showed electromagnetic response that closely resembles the electromagnetically induced transparency in an atomic system. Because of its subwavelength dimension, this electromagnetically induced transparency-like molecule was shown to be suitable as a building block to construct a "slow light" plasmonic metamaterial. The specific design of the plasmonic molecule is shown in Figure 15. 40.0 36.S 33.3 ' t 30-0 26.7 23.S • 20.2 [ j 16.9 13.? 10.1 1.11 3.88 e Figure 16. "'Plasmonic Molecule" Exhibiting EIT, Left: Radiative element (metal strip) by itself gets strongly polarized by the incident EM wave, resulting in weak transmission/strong reflection. Right: Radiative element coupled to the "dark" element (two strips). Dark element possesses a non-radiative quadrupole resonance which is excited by the radiative element and de-polarizes the radiative element. The result: vanishing reflection, high transmission. Color bar: I~ normalized to the incident laser field at A = 700 nm. (Reference 32) This specific plasmonic molecule consists of the "dark state" (two parallel plasmonic antennas oriented perpendicular to the incident vertical electric field) and the "radiative state" (single plasmonic antenna oriented parallel to the electric field). The quality factor of the "dark antenna" state Is an order of magnitude higher than that of the "radiative" antenna. When the "radiative" antenna is spatially separated from the "dark" antenna (or when the dark antennas are not present at all), all or most of the incident radiation is reflected from an array of "radiative" antennas whenever the resonance frequency of the antenna coincides with that of the laser. In this example, the long antenna is 128 nm long, and the resonance wavelength is at )\ = 700 nm.' The key effect here is that the resonance of the "dark'' antenna should be at the same wavelength. 18 UNCLASSIFIED//li&ll 81ililtil1'1k Ullii 8911a¥
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Report, from the dia collection. The PDF is mirrored here; the original link is above. 27 pages are in the text index: search them above, or from the library's search.