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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.
UNCLASSIFIED//F8A 8FFI~Ie ■ 1!55 0111 Y where the first and second terms in the second line are the kinetic and potential energies of the oscillator, respectively. The additional 1/2 appearing in the first line of Eq. (1) is called the vacuum zero-point energy for the reason to be explained in the next section. The first line of Eq. (1) is more commonly expressed in units of energy (Joules) in quantum mechanics, which is obtained simply by multiplying the right-hand side by the photon energy flrn so that fI(l\c = hco (rt+½) . It is beyond the scope of this report to elaborate further on the entire subject of the quantum optics. The reader should consult Reference [38] for more information. Basic Notions on the Origin of the Quantum Vacuum Zero-Point Fluctuations Here we discuss the basic notions of the quantum vacuum zero-point fluctuations (ZPF), which is an important feature in quantum optics. The origin of the ZPF is attributed to the Heisenberg Uncertainty Principle. According to this principle, q and [J are any two conjugate observables that we are interested in measuring, and they obey the commutation relation already shown in the previous section. Their corresponding uncertainty relation is 1'1.C/1"1.1);:::: h/2, where &j is the variance (a.k.a. uncertainty) of observable q and l'1.jJ is that of the conjugate observable 1) . This relation states that if one measures observable q with very high precision (i.e., its uncertainty 1'1.lf is very small), then a simultaneous measurement of observable p will be less precise (i.e., its uncertainty 1'1.fa is very large), and vice versa. In other words, it is not possible to simultaneously measure two conjugate observable quantities with infinite precision. This minimum uncertainty is not due to any correctable flaws in measurement, but rather reflects the intrinsic fuzziness in the quantum nature of energy and matter. Substantial theoretical and experimental work has shown that in many quantum systems the limits to measurement precision is imposed by the quantum vacuum ZPF embodied within the uncertainty principle. Nowadays we rather see the Heisenberg Uncertainty Principle as a necessary consequence, and therefore, a derived result of the wave nature of quantum phenomena. The uncertainties are just a consequence of the Fourier nature of conjugate pairs of quantities (observables). For example, the two Fourier-wave-conjugates time and frequency become the pair of quantum-particle conjugates time and energy and the two Fourier-wave-conjugates displacement and wave number become the pair of quantum-particle conjugates position and momentum. The Heisenberg Uncertainty Principle dictates that a quantized electromagnetic oscillator (a.k.a. a photon state) can never come entirely to rest, since that would be a state of exactly zero energy, which is forbidden by the commutation relation given in the previous section. Instead, every mode of the field has Jim/2 as its average minimum energy in the vacuum, and this is called the zero-point energy (ZPE).H This ZPE term is added to the classical blackbody spectral radiation energy density p(w)dco fi.e., the energy per unit volume of radiation in the frequency interval (m, (U + dw)] [25]: ,. flw is the energy of a single mode (or photon). 7 UNCLASSIFIED/ 1«F81it 8FFIIIAI!: 1!181! &••1::Y
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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.