Documents / Report
This Defense Intelligence Reference Document (DIA-08-1003-016), dated 30 March 2010 and produced by the Defense Intelligence Agency under its Advanced Aerospace Weapon System Applications (AAWSA) Program, reviews quantum entanglement and nonlocality. It asks whether they could carry observer-to-observer signals faster than light or backward in time, with real-time control of a Mars rover as an example. It finds no compelling answer yet and says the question must be settled by experiment.
UNCLASSIFIED/ /1"1!11'- l!ll"l"U!llltt l!l!ii! s,11!¥ when the coincidence requirement is relaxed. This may be explained by the action of coherence-entanglement complementarity, as discussed in the next section. V. Coherence-Entanglement Complementarity As discussed above, the finite extent of the source is expected to limit the possibility of observing a two-slit interference pattern, which would be the "signal" if nonlocal communication were possible. Figure 6 shows schematically (not to scale) this "thick source" effect. The source volume on the left is the region of the nonlinear crystal that is illuminated by the UV pump-laser beam directed along the u axis. The source volume is a cylinder a few mm thick and a mm or so in radius with a center point C. The source cylinder is assumed to be tilted at an angle e with respect to the horizontal z axis on which the slit system and detector plane are symmetrically centered. We note that e = 0° in the Ghost Interference experiment and e = 28.2° in the Dopfer experiment. A horizontal distance Lxs away from the source is a two-slit system, a pair of apertures a with center-to-center separation d. Light passing through the slit system travels a horizontal distance Lsd and is detected at detector plane at position X1. L 1 • B Source Volume ••p Slit System Detector Plane Figure 6. Thick-Source Effect (not to scale): Waves arriving at the two slits from points A and Bat the extrema of the source volume may have significant path length and phase differences, while waves from the central point Care in phase at the slits. If the point of photon production is off the z axis, there will be a path length difference between waves relative to C as they arrive at the two slits. In Figure 6, waves from points A and B could have path length differences greater that half a wavelength and phase differences greater than 180°. Roughly speaking, this shifts the interference pattern relative to waves created at central point C so that maxima become minima and vice versa. The net effect of averaging over all points in the source volume would therefore be to wash out the two-slit interference pattern. That two-slit interference pattern must be observed unambiguously, because it is the "signal" that would be used in any nonlocal communication. This operability is quantified by an observable called "visibility," which is related to the peak-to-valley ratio of the interference pattern. The constancy of the relative phase at the two slits for photons arriving from various parts of the source is called "coherence" and ensures a high visibility. It should be clear that a point-like source has perfect coherence, while a source with a large solid angle as 10 UNCLASSIFIED/ ,'P9Pl 8ffl81Als Wlili SUIL¥
Not linked to a story yet.
Report, from the dia collection. The PDF is mirrored here; the original link is above. 32 pages are in the text index: search them above, or from the library's search.