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Defense Intelligence Reference Document High-Frequency Gravitational Wave Communications

Defense Intelligence Agency · 57 pages · text from the file's own layer

This Defense Intelligence Reference Document was prepared by the Defense Intelligence Agency under its Advanced Aerospace Weapon System Applications (AAWSA) program, is dated 6 April 2010 and is part of a series of advanced technology reports produced in FY 2009. It reviews proposed laboratory generators and detectors of high-frequency gravitational waves for communications. It favors an infrared-excited molecules transmitter and the Li-Baker detector, estimating about 1.9 million bits per second over 7,000 km through the Earth. It also discusses timing standards and interplanetary navigation uses.

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2.2.4 Li-Baker HFGW Detector
The detector, shown in Figure 14, has five major components:
1. A Gaussian (focused, with minimal side lobes) microwave beam (GB) is aimed along
the +z-axis at the same frequency as the intended HFGW signal to be detected (Yariv,
1975), typically in the GHz band, and also aligned in the same direction as the HFGW to
be detected. The microwave transmitter's horn antenna is not shown, but would be
located on the -z-axis.
2. A static magnetic field B, generated by two powerful magnets, typically using
powerful superconductor magnets such as those found in a conventional MRI medical
body scanner, is directed along the y-axis.
3. Two paraboloid-shaped reflectors, which are formed from "fractal membranes" (Wen
et al., 2002; Zhou et al., 2003; Hou et al., 2005), are located in the y-z plane at the
origin of the coordinate system to aim and focus the detection photons at diffraction-
limited spot antennas connected to two microwave receivers. These reflectors, shown in
planer form in Figure 15, are segmented (similar to a Fresnel lens) and located back-to-
back in the y-z plane. They are thin enough (less than a centimeter thick in the x-
direction) to not block the z-directed Gaussian beam. These microwave reflectors reflect
the x-directed detection photons (PPF) and reject the z-directed Gaussian-beam
photons, which move parallel to the surface of the reflectors in the y-z plane.
4. High-sensitivity shielded microwave receivers are located at each end of the x-axis
each about one meter distant from the origin.
5. Interior noise from thermal photon generation is eliminated by cooling the Li-Baker
detection apparatus to below~ 48 mK (0.048 Kelvin). Thus there are effectively no
thermal photons at 10 GHz. Noise from the interior background photon flux (BPF) from
the EM Gaussian beam is reduced to a negligible level by moving the receivers out to
the side about a meter away from the EM beam and by a series of superconductor or
microwave absorbent baffles to "shade" the receivers. Stray EM resulting from
scattering of particulate matter near the apparatus and possible dielectric dissipation
can be effectively suppressed by evacuating the apparatus to about 7.5x 10-7 Torr (a
rather high vacuum). External noise is eliminated by the use of a steel and titanium
cryogenic containment vessel surrounding the low-temperature Li-Baker detection
apparatus.
In summary, several different HFGW receivers can be utilized for communication; but
the proposed Li-Baker detector (plans & specification development in Appendix B)
shows the most promise (detailed underlying concept is derived in the paper included
as Appendix C).
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Report, from the dia collection. The PDF is mirrored here; the original link is above. 57 pages are in the text index: search them above, or from the library's search.