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Defense Intelligence Reference Document Traversible Wormholes Stargates And Negative Energy

Defense Intelligence Agency · 42 pages · text from the file's own layer

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.

  • p. 4 …A Stargate in Times Square ..................................................................... 9 Figure 9. Conceptual Squeezed Light Negative Energy Generator ........................ 14 Figure…
  • p. 5 …the study of traversable wormholes and the study of time machines. Wormholes are hyperspace tunnels through…
  • p. 6 …the Cosmic Neighborhood can encompass other universes, other space dimensions, and other times beyond the four…
  • p. 7 …The solution to this problem is to dispense entirely with long interstellar voyage times or the…
  • p. 8 …But time travel via wormhole is beyond the scope of this paper. Suffice it to say…
  • p. 9 …The desired requirements are the following (Reference 1, 3): • Travel time through the wormhole tunnel or…
  • p. 10 …The proper time of travel as measured by space travelers going through the wormhole is given…
  • p. 11 …specific moment of time (t = canst). The top of Figure 2 shows the embedding diagram for…
  • p. 12 …time axis). Then identify these two incomplete spacetimes along the timelike boundaries CQ x ~n. The…
  • p. 13 …Create the Wormhole Throat an (time is suppressed in this diagram) Figure 4. The Same Diagram…
  • p. 14 …3 K ' 1 is a diagonal matrix (2) having the two principal radii of curvature, p1…
  • p. 17 …The General Relativistic Definition of Exotic Matter and the Energy Conditions This section will consider the…
  • p. 19 …3), violations of the second law of thermodynamics (Reference 34, 35), and time machines (Reference 2…
  • p. 20 …the expense of increasing the noise in the conjugate observable; at the same time the variations…
  • p. 21 …w is the angular frequency of light, I is time, and: denotes the z-axis direction…
  • p. 27 …product space), where ~H is the real line defining the time dimension for this particular product…
  • p. 28 …If the acceleration varies with time, the conductor will generally emit or absorb photons (i.e…
  • p. 30 …The QI conjecture relates (via model dependent time integrals of the energy density along geodesics) the…
  • p. 31 …the initial negative pulse; and c) the longer the time interval between the two pulses, the…
  • p. 35 …for extended periods of time over extended spatial distributions for the purpose of engineering a traversable…
  • p. 37 …S., and Yurtsever, U., "Wormholes, time machines, and the weak energy conditions," Physical Review Letters, Vol…
  • p. 38 …R., The Large-Scale Structure of Space-Time, Cambridge Univ. Press, Cambridge, 1973, pp. 88-91…
  • p. 39 …H., "Quantum coherence effects and the second law of thermodynamics," Proceedings of the Royal Society of…
  • p. 40 …K., "Demonstration of the Casimir Force in the 0.6 to 6 μm Range," Physical Review…
UNCLASSIFIED//F81il 8FFHil.l1k WE'lii Si'llk>C
=-(l.35xl0c7kg) l,hmat
I meter (9)
=-(0.7]MT) ],hrn,LI
I meter
where M"1, is the (equivalent) mass required to build the wormhole, lcthroat is a suitable
measure of the linear dimension (width or diameter) of the throat, and MJ is the mass
of the planet Jupiter. One can also obtain the required energy, Ei11, by multiplying both
sides of Equation (9) by c2 . Equation (9) shows that a mass of -0.71 M1 will be required
to build a wormhole 1-m in size. As the wormhole size increases, the mass requirement
grows negative-large. Table 2 presents a tabulation of the required negative
(equivalent) mass as a function of sample wormhole throat sizes. After being alarmed
by the magnitude of the results, one should note that Mw11 is not the total mass of the
wormhole as seen by remote observers. The non-linearity of the general relativistic field
equation dictates that the total mass is zero (actually, the total net mass being positive,
negative or zero in the Newtonian approximation depending on the details of the
negative energy configuration constituting the wormhole system). Finally, Visser et al.
(Reference 59) demonstrated the existence of spacetime geometries containing
traversable wormholes that are supported by arbitrarily small quantities of negative
energy, and this was proved to be a general result. The next section will expand on this
further.
Table 2. Negative Equivalent Mass Required for
Traversable Wormhole
Athroat (m) Mwh
1000 -709.9 Mi
100 -71 M1
10 -7.1 M1
1 -0. 71 M1
0.1 -22.6 Mr-
0.01 -2.3 M,
MJ = 1.90 x 1027 kg, Mo = 5.98 x 1024 kg
B. PHYSICAL CONSTRAINTS ON NEGATIVE ENERGY
The Quantum Inequalities (QI) conjecture is an extension of the Heisenberg Uncertainty
Principle to curved spacetimes. Much research has been conducted around this one
topic alone. The literature is too numerous to cite here but the reader should consult
(Reference 10) and (Reference 46) for detailed information. The QI conjecture relates
(via model dependent time integrals of the energy density along geodesics) the energy
density of a free quantum field and the time during which this energy density is
observed. This conjecture was devised as an attempt to quantify the amount of
22
UNCLASSIFIED/;<FSi'A Si'FFIGIAk Wli'lii Si'Hkl:f

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