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Defense Intelligence Reference Document Metamaterials For Aerospace Applications

Defense Intelligence Agency · 27 pages · text from the file's own layer

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.

  • p. 5 …magnetic, or other} cannot be found in naturally-occurring materials. The emphasis of this study will…
  • p. 8 …Such miniaturization is possible due to the resonant nature of the individual unit cells. Specifically, the…
  • p. 10 …The speed of light places a natural limit on the size of optical/microwave components. Metamaterials…
  • p. 11 …structure of the living cell in its natural environment. In all likelihood, that environment would be…
  • p. 13 …the constant frequency contour, has a hyperbolic nature) in a tapered format. Several conceptual implementations such…
  • p. 15 …Another advantage of this • imaging technique is that it is interferometric in nature. Therefore, even if…
  • p. 20 …Because of the very large speed of light, there is a natural limit to how small…
  • p. 23 UNCLASSIFIED/f P8rl 8PPIIIAL ld!H! OHL\' Because the exploited resonance has a quadrupole nature, it…
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The electric response of such (or similar) metamaterial is given by
ai
&(Ill)= f - l l' .
or-m; +10Jy (2)
where ma is the resonant frequency and r is the loss coefficient.
Negative index metamaterials are by no means the only potentially useful metamedia.
Several new concepts such as Indefinite Permittivity Metamaterials (IPM) (References
3, 4) and Epsilon-Near-Zero (ENZ) metamaterials (Reference 5) have recently emerged
and found some exciting applications that will be reviewed below. IPMs can be used as
ultra-compact spatial filters (both high-pass and low-pass) whereas ENR metamaterials
can be·used for making sub-wavelength waveguides capable of coupling close to 100
percent of the incident radiation (Reference 8), as well as directing it around tight
bends with negligible bending losses. Yet another class of planar metamaterials,
complementary metamaterials (CMMs), has recently emerged (Reference 7). Instead of
using metallic structures deposited on a substrate (left panel of Figure 3), CMMs consist
of slits in the continuous metal screen (right panel of Figure 3). The shape of the slits
coincides with that of the materials themselves. Such complementary metamaterials
have been recently used for making epsilon-near zero waveguides (Reference 8).
CE4
CE5
CE3 CE6
Figure 3. Geometry of Orlglnal Planar Metamaterlal Unit Cells (OE1-0E6) and Their Complements
(CE1-CE6). The polarization of normally Incident electromagnetlc radiation ls configured as shown ln OEl
and CEl for the original and complementary metamaterials, respectively, (Reference 9)
3
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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 27 pages are in the text index: search them above, or from the library's search.