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Defense Intelligence Reference Document Quantum Tomography Of Negative Energy States In The Vacuum

Defense Intelligence Agency · 51 pages · text from the file's own layer

This Defense Intelligence Reference Document from the Defense Intelligence Agency is dated 11 January 2011. It was produced in FY 2010 under the Advanced Aerospace Weapons System Applications (AAWSA) Program. It reviews negative, or sub-vacuum, energy found in squeezed light and the Casimir effect, and explains quantum optical homodyne tomography as a way to measure and map that energy in the lab. It proposes balanced homodyne detector arrays that could help detect anomalous aerospace platforms using engineered spacetime propulsion.

  • p. 5 …A first step in this direction was already taken by Hansen et al. 4 in 2001…
  • p. 38 …impossible. Time-domain BHD resolves this limitation. Hansen et al. 4 describe their experimental time-domain…
  • p. 39 …mode that matches that of the LO. Hansen et al. 4 point out that time-domain…
  • p. 47 …Nearly a decade ago, Hansen et al. 4 reported on their experimental time-domain (or pulsed…
  • p. 50 …1016-1022. 4 Hansen, H., et al. (2001), "Ultrasensitive pulsed, balanced homodyne detector: application to time…
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polarization of the signal field 5. The subsequent PBS2 separates the two orthogonally
polarized signals, which are detected at the photodiodes PDx and PDy. The charge
collected at point V (corresponding to point Pin Figure 15) provides a measure of
(l)Grd (and its higher moments). Note that the setup is arranged in such a way, that if
5 happened to be a monochromatic coherent state, then it would be phase-matched to
the LO at the point x, but shifted in phase by rr at the pointy.
Figure 19 displays Marecki's computer model plot of the predicted Casimir spectral
density as a function of the distance from the plates x and the frequency w. For a
comparison with quantum optics literature, he plotted the normalized difference
between the vacuum and ground state spectral density in the figure (see References [5]
and [6] for more detail). Note in the figure that for w < rrc/a, the Casimir spectral
I I
density vanishes: aG,-d(rn,x,x) =0, while discontinuities in it appear at w = nnc/a.
Figure 20 displays the corresponding computer model plot by Marecki of the predicted
"suppressed 11
vacuum fluctuations in the ground state relative to "undisturbed" vacuum
[ II II]
fluctuations (in absence of the plates) in dB, 10Log 10 ac,-Jw,x,x)/a'"ac(w,x,x) .
40
Imm
Casimir plate
TEl Coherent field (Local Oscillator)
y-Direction
lμm
x-Directlon
Figure 16. Diagram of Casimir Cavity with BHD Photodiodes. (courtesy of P.
Marecki)
1.0
_ 0.8
§_ 0.6
'; 0.4
0.2
0.0
-1000 -500
Side view:
0 y[μm] 500 1000
Figure 17. Experimental Setup of BHD Photodiodes and LO Field. (courtesy of P.
Marecki) This setup is drawn on the plot of they-component of the electric field of the
TEl mode of the Casimir cavity. The mode, serving as the LO, propagates in the z-
direction perpendicular to the plot.
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Report, from the dia collection. The PDF is mirrored here; the original link is above. 51 pages are in the text index: search them above, or from the library's search.