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This Defense Intelligence Reference Document (DIA-08-1004-004), dated 6 April 2010, was produced by the Defense Intelligence Agency under its Advanced Aerospace Weapon System Applications (AAWSA) Program. It is one of a series of advanced technology reports from FY 2009. It reviews the general relativity physics of traversable wormholes and flat-faced "stargate" solutions for faster-than-light travel. It also covers the exotic negative energy these would need, proposed lab methods for generating it such as the Casimir effect and squeezed vacuum, and the constraints involved.
UNCLASSIFIED//FVA: VFFICICP 1!55 0111 Y negative energy or energy condition violations required to build a traversable wormhole spacetime. Investigators have invoked the QI to rule out many of the macroscopic wormhole spacetimes. When generating negative energy the QI postulate that: a) the longer the pulse of negative energy lasts, the weaker it must be; b) a pulse of positive energy must follow and the magnitude of the positive pulse must exceed that of the initial negative pulse; and c) the longer the time interval between the two pulses, the larger the positive pulse must be. This actually sounds quite reasonable on energy conservation grounds until one discovers that the Casimir effect and its non-Maxwellian quantum field analogs violate all three conditions. There are also a number of squeezed vacuum sources and Dirac field states that manifestly violate all three conditions. Cosmological inflation, cosmological particle production, classical scalar fields, the conformal anomaly, and gravitational vacuum polarization are among the many other examples that also violate the QI. Visser (Reference 60) also points out that observational data indicate that large amounts of "exotic matter" are required to exist in the universe in order to account for the observed cosmological evolution parameters. The QI have also not been verified by laboratory experiments. The assumptions used to derive the QI and the efficacy of their derivation for various cases has been called into question by numerous investigators. Krasnikov (Reference 61) constructed an explicit counterexample for generalized FTL spacetimes showing that the relevant QI breaks down even in the simplest FTL cases. And he also addressed Fewster's (Reference 62) technical arguments on this issue. It is important to point out that the Qls have been mainly proven for free massless scalar fields in flat two-dimensional Minkowski spacetime, so there remains the unanswered questions of extending the QI into a four- dimensional curved spacetime model (with or without boundaries) and how much negative energy density can arise for interacting fields. It turns out that Visser and coworkers (Reference 59, 63, 64) developed a superior way to properly quantify the amount of negative energy or energy condition violations required to build a traversable wormhole spacetime. They propose a quantifier in terms of a spatial volume integral, which amounts to calculating the following definite integrals (Reference 59, 63, 64): fr,,dV~O; f(r,,+p,)dV~O (10) with an appropriate choice of the integration measure dV (= 4m2 dr or g 112drd0drp, where g = det(g,w) is the matrix determinant of gw). The amount of energy condition violation is defined as the extent to which Equation (10) can become negative. The value of Equation (10) provides information about the total amount of energy condition violating matter that must exist for any given FTL spacetime under study (e.g., warp drives and traversable wormholes). It was further shown that Equation (10) can be adjusted to become vanishingly small by appropriate choice of parameters; therefore, examples can be constructed whereby the energy condition violation can be made arbitrarily small. But the violation cannot be made to vanish entirely. Equation (10) also gives the result that traversable wormholes require arbitrarily small amounts of negative energy to build (whereby Equation (9) serves only as a gross upper limit) such that within a wormhole spacetime (Reference 59): 23 pc~o, f p,dV ➔ O C UNCLASSIFIED/ ;rell 8PPI@Itllt tt.!I!! 8HLY ( 11)
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