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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. 2 …a series of advanced technology reports produced in FY 2009 under the Defense Intelligence Agency, ffbl…
  • p. 3 …Schematic of the SIC-based Super-lens Which Is Imaging Sub-wavelength Holes Buried Under the…
  • p. 9 …Applications ofmetamaterials to photon harvesting is especially fitting for advanced aerospace platforms because of the necessity…
  • p. 10 UNCLASSIFIED/ JFQA 8FFl81alft U!II! GIit i • Far Field Super-Lens Based on the Interferometry of…
  • p. 13 …Within the confines of an advanced aerospace platform such device (with its necessary auxiliaries) may not…
  • p. 16 …To advance this goal, and to develop a tool sometimes referred to as the FSL, we…
  • p. 19 …Figure 10 demonstrates this interference pattern which reveals the phase advance of the sub-diffraction waves…
  • p. 20 …Slowing Down and Manipulating Electromagnetic Pulses (EMP) Using Advanced Metamaterials Given the space constraints of an…
  • p. 23 …These frequency domains are likely to be of greater use for advanced aerospace platforms than the…
  • p. 26 …If the wavelength falls inside the transparency window of the atmosphere (between 3 and 4 μm…
  • p. 27 …Some type of thermophotovoltaic converter will almost undoubtedly be installed on the advanced aerospace platforms of…
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 above. 27 pages are in the text index: search them above, or from the library's search.