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This Defense Intelligence Reference Document from the Defense Intelligence Agency, dated 28 January 2010, surveys pulsed high-power microwave (HPM) source technology. It was produced under the Advanced Aerospace Weapon System Applications (AAWSA) program. It covers insulation, cathode materials, high-voltage switching, pulse generators, microwave sources such as magnetrons, gyrotrons and the Phoenix and Jolt sources, and antennas. The document concludes that progress depends on advances in cathodes, switching and insulation. It says compact ultrawideband antennas will remain difficult to build.
UNCLASSIFIED/;SflHl 8FFHil.t.k Wfili IH.k\f where: a and bare dimensions of the sides and t. is the wavelength. For conical horns, the gain is given by: G = 5D 2/k 2 where: Dis the diameter and/, is the wavelength. Mode conversion is critically important with horn antennas in order to generate field patterns of use. The fundamental modes, TE10 in rectangular waveguide and TE11 in circular waveguide, are preferred since they radiate a field pattern with peak field strength on axis. These are the most common modes used in electronic vulnerability testing. Parabolic dish antennas are the most common type found in conventional microwave applications, but their use in narrowband HPM has been limited because of breakdown problems in center feed geometries. Variations of the parabolic dish have, however, been very successful. The Active Denial System (ADS) uses a flat parabolic surface (FLAPS) antenna. FLAPS uses an array of crossed dipole scatterers placed about 1/8 wavelength above a ground plane to create a geometrically flat surface that behaves like a parabolic dish. Each dipole controls its corresponding polarization. Incident energy causes a standing wave to be established between the dipole and the ground plane. The interaction of the Figure 12. FLAPS Antenna With a Cross-Shorted Dipole Array dipole reactance and the standing wave causes the incident RF energy to be reradiated with a phase shift determined by the dipole length, thickness, and distance from the ground plane, as well as by the angle of incident RF, the dielectric constant of the media between the dipole and ground plane, and the proximity to adjacent dipoles. Figure 12 shows the essential elements of the FLAPS antenna with a cross-shorted dipole array. These antennas are easier to store and have less wind resistance than conventional parabolic dishes. The Vlasov antenna is also well suited to narrowband HPM radiation and has some distinct advantages. It can be fed with a TM01 mode and produce a directed beam with a nearly Gaussian profile; mates easily to the cylindrically symmetric HPM sources, such as the MILO and vircators; is easily constructed; and has a large feed aperture to support high electric fields. Typically sources that generate their power in the TM on modes require a mode converter for radiating anything other than a donut beam, but the Vlasov antenna does not; the antenna is actually adapted from a mode converter. 26 UNCLASSIFIED/ /f81il 8fFI&I.«1k W&liii Qllb¥
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Report, from the dia collection. The PDF is mirrored here; the original link is above. 37 pages are in the text index: search them above, or from the library's search.