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Defense Intelligence Reference Document Pulsed High-Power Microwave Source Technology

Defense Intelligence Agency · 37 pages · text from the file's own layer

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.

  • p. 6 …on the order of several hundreds of kilovolts per meter with onset or rise times of…
  • p. 7 …If the pulse duration is short compared with thermal diffusion times, then the temperature increases in…
  • p. 8 …The short burst mode operation is necessary because of the high peak powers and subsequent heating…
  • p. 17 …Second, it has a fast turn-on time. Third, the insulating nature of the velvet fibers…
  • p. 18 …As a result, the HPM emission times have been extended. Typically, the cesium salt is dissolved…
  • p. 19 …The period of the lowest frequency is twice the pulse width, and the rise time is…
  • p. 20 …Thus, the faster the rise time and the wider the pulse, the broader the spectral content…
  • p. 21 …8FF11il.t.k WE&i a••k>/ rise time is the time required to heat the…
  • p. 22 …The array can then be phased in time to allow steering of the beam. GaAs switches…
  • p. 24 …The explosives are then used to compress the initial magnetic flux by driving the conducting cylinder…
  • p. 26 …SPLIT-CAVITY OSCILLATORS Split-cavity oscillators (SCOs) utilize transit-time bunching of the beam to generate…
  • p. 28 …in the 3.5-ns-wide pulse is 1.25 GW, and the rise time is…
  • p. 29 …Thus, for H3 the FOM is 250 kV. While developing the H series of HPM sources…
  • p. 30 …Phoenix had the fastest rise time of any HPM source to date. Figure 8 shows the…
  • p. 32 …By timing the switching sequence of each BASS module, the beam was steerable up to 30…
  • p. 35 …Thus, if the frequency chirps during the RF pulse, then the beam direction will sweep. The…
  • p. 36 …This is why the rise time of the driving pulse is so important to antenna response…
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appears to be hydrogen ions, which, because of their low mass, contribute to the
problem of gap closure. The gap closure velocity using carbon cathodes quoted by most
reports researched is 2-2.5 cm/μsec, and diode gaps from the same reports were 1-4
centimeters. Carbon cathodes also have much longer lifetime than velvet. However, one
of the greatest advantages of carbon is the ever-expanding ability to form both macro-
and nanostructures using it as a base or substrate. Structures formed using carbon
include pyramids, fibers, microfibers, nanotubes, and tufts. Many possible carbon
structures still have yet to be formed and tested. Thus far, structures with the most
surface area appear to perform best.
CERAMICS
Ceramics, much like carbon, can be formed into at least microstructures and have some
features that have attracted interest in them for a couple of decades. These include
virtually unlimited lifetimes and extremely low outgassing. A problem with ceramics,
however, is that very high threshold fields are required for diode operation. Coatings to
improve the performance of ceramic cathode structures may exist, and research is
continuing in this area.
CESIUM IODIDE COATED
One of the most recent and impressive materials to be used in cathodes for HPM tubes
is cesium iodide. Cesium is a pure metal that has a work function of only 1.9 eV and a
melting temperature of 28 °Celsius; thus, it is liquid at only slightly above room
temperature. Cesium ions are quite heavy, and that is why this coating was used
initially. It was believed that the gap closure rate would be slowed since the heavy
cesium ions would progress much more slowly across the anode-cathode gap than
would other ion species, given the same electric field. This has proved to be the case,
and closure velocities that are about one-fourth those for velvet or bare carbon (0.4
cm/psec) have been attained. As a result, the HPM emission times have been extended.
Typically, the cesium salt is dissolved in water as a saturated solution and then the
carbon cathodes are dipped several times. Subsequently, the cathodes must be baked
under vacuum for several hours to remove the water from the surface and leave the
hardened cesium salt. Once completed, the cathodes have a very long lifetime unless
contaminated by back splatter of material from the anode. At present, HPM programs
investigating the performance of cathodes having some form of cesium coating over
carbon nanostructures show the most potential for progress in the state of the art. The
goal of these programs is hundreds of kiloamps for tens of microseconds, resulting in
gigawatt narrow-band HPM sources running at repetition rates of possibly 100 hertz and
thus capable of 100-megajoule energy output per burst. Also of great interest at
present are cathodes termed "hybrids," which utilize multiple emission mechanisms in
beam generation. The cathodes developed by these programs are to be used with the
magnetically insulated line oscillator (Sandia National Laboratories [SNL]), the
relativistic klystron oscillator (Kyle Hendricks, Air Force Research Laboratory [AFRL]),
the reltron (Bruce Miller, SNL), and the super reltron, among others.
10
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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 37 pages are in the text index: search them above, or from the library's search.