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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. 3 …Hyperlens Based on a Converging Array of Metal Wires ........................ 10 Figure 9. Far-Field Super-lens…
  • p. 4 …Radiative Antenna (Single Metal Strip} Coupled to a Dark Antenna (Two Perpendicular Metal Bars) .......................................................... 19 Figure…
  • p. 7 …Instead of using metallic structures deposited on a substrate (left panel of Figure 3), CMMs consist…
  • p. 8 …high (or the dielectric permittivity of a metal is.,not sufficiently large), electrostatfc resonances disrupt magnetic…
  • p. 11 …simple holes that were milled in the metal using an FIB. They were buried underneath the…
  • p. 14 …The hyper-lens involves an array of thin metallic wires converging towards the tip. As is…
  • p. 21 …to be negative (for example, a metal-dielectric-metal waveguide would suffice), the key here is…
  • p. 22 …Radiative element (metal strip) by itself gets strongly polarized by the incident EM wave, resulting in…
  • p. 23 …radiative antenna (single metal strip) coupled to a dark antenna (two perpendfcular metal bars). Such metamaterial…
  • p. 27 …Metamaterials tend to be lossy because of the large field concentration in the metal. Therefore, work…
UNCLASSIFIED/ /FOil 9PPll!!lllit 1!18& 0'11kY
cyl. r s JJ.r
I 0.260 1.654 0.003
2 0.254 1.677 0.023
3 0.245 1.718 0.052
4 0.230 1.771 0.085
5 0.208 1.825 0.120
6 0.190 1.886 0.154
7 0.173 l.951 0.188
8 0.148 2.027 0.220
9 0.129 2.110 0.250
10 0.116 2.199 0.279
r1yyre .a., a::xdmp1e ur t:t l"l~1c1mc:tl.~rttll .._.umpun-,n&.: 1n .... --•-:,•• .......... _,,, ............ ~ .............. _ ...... ~-• .... - ■ •••.1 ---·~··· ···-
in-plane lattice paramete1·s are av= a,= 10/3 mm. The ring is square, with edge length I =3 mm and tracewidth w
= 0.2 mm. The substrate is 381 μm-thick Duro1d 5870 (E = 2 33, td = 0.0012 at 10 GHz, where td is the loss
tangent). The cu film, from which the SRRs are patterned, is 17 μm thick. The parameters rand s are given in the
table together with the associated value of μ-. (Reference 6)
Electric properties of metamaterials can be similarly controlled. An example of a planar
electrically-active metamaterial is shown in Figure 2.
2
I
l Figure 2. Example of Another Metamaterial Component: Electric
Ring Resonator (ERR). This component provides tunable resonant
electric response to the incident electromagnetic field, and can be
utilized for engineering the frequency-dependent dielectric
permittivity c(w) . Possible application: THz and microwave absorbers.
(Reference 7)
UNCLASSIFIEDJ;GFOlil 8FFl&l,1k Wlli IHHsl.f

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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.