AAWSAP DIRD, The Space Communication Implications of Quantum Entanglement and Nonlocality, March 2010
DOW-UAP-D133 · page 16 of 32
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B Source Slit Detector UNCLASSIFIED//FOR OFFICIAL tt.!I!! 8HL'f 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 0 with respect to the horizontal z axis on which the slit system and detector plane are symmetrically centered. We note that 0 = 0° in the Ghost Interference experiment and 0 = 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 x,. System Plane Volume Figure 6. Thick-Source Effect (not to scale): Waves arriving at the two slits from points A and B at the extrema of the source volume may have significant path length and phase differences, while waves from the central point C are 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 UNCLASSIFIED/,,roA &FFISIAL 1:181! 8HL'I" 10