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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.

  • p. 5 …communications are carried on an extremely narrow beam directly through the Earth, there is a very…
  • p. 9 …Alternatively, a pulsed particle beam, which could include antimatter, could trigger nuclear reactions and build up…
  • p. 15 …Thus a HFGW total flux of l .29x 108 wm· 2 in a very narrow beam…
  • p. 16 …With this configuration, the width of the needle-like, narrow HFGW beam at the receive end…
  • p. 17 …The Birmingham University HFGW detector measures changes in the polarization state of a microwave beam (indicating…
  • p. 19 …The result of the intersection of the parallel and superimposed EM and GW beams, according to…
  • p. 20 …However, with the Li-Effect, there is an additional focused microwave beam ("Gaussian beam") at the…
  • p. 21 …The signal (the PPF) and the noise, or background photon flux (BPF) from the Gaussian beam…
  • p. 23 …Assuming a "best efforts" value of 1000 W for the power of the Gaussian beam in…
  • p. 24 UNCLASSIFIED/ ,'l"e" Cl"l"!e!•t tl9E CHE I beam is much greater than the…
  • p. 25 …A Gaussian (focused, with minimal side lobes) microwave beam (GB) is aimed along the +z-axis…
  • p. 30 …With this configuration, the width of the needle-like, narrow HFGW beam at the receive end…
  • p. 38 …with stronger magnetic fields, more intense Gaussian beams, and better baffles as well as new detector…
  • p. 46 …and Zhao P. (1992), "Interaction Between Narrow Wave Beam-Type High Frequency Gravitational Radiation and Electromagnetic…
  • p. 47 …M Land Fang Z. (2007), "Coupling of an open cavity to a microwave beam: a possible…
  • p. 52 …D01.3 Microwave Transmitter {Gaussian beam) Design of the microwave transmitter for the Gaussian beam, directed…
  • p. 53 …of the interior baffles around the Gaussian beam, and a "tunnel" between fractal-membrane reflectors and…
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Appendix A: Nomenclature
A
B
B
C
C
dt
E
FGw
h
hdet
~
N
N
Nphase
Nfreq
Ncode
n
p
Q
R
Rcvrl
Rcvr2
R,
R,.
s
s,
S,
r
T
ta
tint
Xmit1
Xmit2
M
Lip
Lit
/Ix
A
VGW
"WI
w,
44
amplitude of gravitational wave, metric strain in spacetime, m/m
bandwidth, s-1
magnetic field strength, Tesla
speed of light in vacuum (2.998 x 108 ms- 1)
maximum rate of information transfer, bits per second (bps), s- 1
time of future measurement, s
effective energy contained within the detector cavity summed over the detection
averaging time, J
gravitational-wave flux, Wm- 2
strain, m/m
(strain) detection limit, m/m
Planck's reduced constant 1.055 x 10 34 Js
noise, Wm 2
number of linearly arranged GW radiation elements, integer
number of phase space cases to check for acquisition, integer
number of frequency cases to check for acquisition, integer
number of code sync possibilities to check, integer
number of pairs of oppositely jerking at one-time mass elements, integer
power of the generated gravitational waves, W
temporal quality factor or selectivity of the signal-to-noise ratio, dimensionless
range, m
receiver 1
receiver 2
receiver antenna power efficiency, dimensionless
radiated power efficiency, dimensionless
signal strength, wm- 2
input signal strength, Wm- 2
output signal power, W
distance between two jerking-mass, gravitational-wave radiation elements, m
propagation or transmission-factor losses, dimensionless
acquisition test time per test case, s
integration or signal averaging time, s
transmitter 1
transmitter 2
change in force of a jerking-mass, gravitational-wave radiation element, N
momentum uncertainty, kg-ms 1
time interval, s
initial position uncertainty, m
conversion efficiency (ratio of power of the EM input signal to power of the GW
signal generated), dimensionless
conversion efficiency (ratio of power of the GW input signal to power of the EM
signal generated), dimensionless
wavelength, m
gravitational-wave frequency, s 1
frequency of sensed gravitational waves, s-1
transmitting frequency, s- 1
receiver-sensitivity frequency, s- 1
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