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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.
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Because the exploited resonance has a quadrupole nature, it is slightly red-shifted. For
that reason, the length of the "dark" antenna is 100 nm. When the two antennas are
brought together, the radiative antenna polarizes the dark antenna, which, in tum,
depolarizes the radiative antenna. As a result, the dipole moment of the coupled system
is drastically reduced, the reflection drops and transmission increases to almost 100
percent (limited only by losses). Most of the energy is now stored inside the non-
radiative (dark} antenna.
If multiple layers of dark/bright antennas are employed as shown in Figure 16, then
one can achieve one of the most import~mt manifestations of EIT; "slow" light. Slow
light can have many interesting technological applications because (a) slow light is easy
to manipulate by changing the structure's parameters (as described in the section on
tunable metamaterials), and (b) slow light has a high field intensity (enhanced by the
ratio of the free-space propagation speed to the slow propagation speed), therefore, all
nonlinear processes are enhanced for slow light. Such nonlinear processes may include
harmonics generation, optical diode action {see the section on non-reciprocal optical
elements), and many others.
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figure 17. Tru.e Multl-Layer Metamaterial With a Unit Cell Shown in Figure 15: radiative antenna (single
metal strip) coupled to a dark antenna (two perpendfcular metal bars). Such metamaterial exhibits "slow" light
propagation along the incidence direction (slowed dowh by a factor 30 or more). (Reference 32)
It is important to realize that the geometry suggested in Reference 32 is not unique.
For example, the dark and radiative antennas need not reside in the same plane. Nor is
the effect of EIT (and the related phenomenon of slow light) limited to the optical
domain. Both infrared and microwave-range designs have started emerging. These
frequency domains are likely to be of greater use for advanced aerospace platforms
than the visible range targeted by most studies.
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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.