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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.
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detection losses. The input signal J is attenuated and, simultaneously, contaminated
by the vacuum fluctuations entering the second (unused) input port of the fictitious
beam splitter. The absorber acts like a fictitious beam splitter, and when light is
attenuated it can be imagined as being split into a transmitted part and an absorbed
part. On the other hand, we know from the fluctuation-dissipation theorem that losses
are always accompanied by fluctuations [57]. At least the vacuum fluctuations of the
absorbing medium must be taken into account. In the simple absorber model, these
fluctuations come into play via the second (unused) input port of the fictitious beam
splitter as shown in Figure 9. The annihilation operator ii of the partially absorbed
(input signal) mode is transformed by the fictitious beam splitter according to
&' =r{2.'.l+O-ri/_:,c\, where the factor T\ (0 < T\::::; I) reduces the intensity of any initial
coherent state la) to lri 112
a) after undergoing partial absorption, U' is the output signal
mode that goes to the detector (which counts the number of photons it absorbs,
h' = (1" (1' ), and ii2 is the mode operator of the vacuum fluctuations entering the second
(unused) input port of the fictitious beam splitter. The second term (1-rit"d~ in U' is
essential to guarantee that the attenuated light field remains a proper bosonic mode,
otherwise energy conservation and the aforementioned bosonic commutation relations
would be violated.
Finally, we note without further elaboration that the mode operators, quadrature wave
functions, and Wigner functions are all rotated through some angle under the action of
a beam splitter. And the Wigner function of a signal is smoothed during absorption
under the action of a fictitious beam splitter. This provides additional models to
develop the properties of other types of optical instruments and understand their
behavior on incoming light modes (or input signals).
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vacuum
a,
signal
a
detector
absorption
Figure 9. Illustration of a Fictitious Beam Splitter.
(courtesy of Ulf Leonhardt)
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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.