John Company

AAWSAP DIRD, The Space Communication Implications of Quantum Entanglement and Nonlocality, March 2010

DOW-UAP-D133 · page 14 of 32

Page 14 of 32 of DOW-UAP-D133

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a)
Pump
Figure 4. "Unfolding" the Ghost Interference Experiment
The authors point out that there is a simple way of thinking about momentum­
entanglement measurements involving entangled photons. It can be shown from Snell's
Law and conservation of momentum in the crystal that if one photon has a small
momentum that causes it to be slightly deflected to the right of the pump beam by an
angle 0, then the twin entangled photon will be deflected to the left by the same angle
0, a situation reminiscent of reflection from a mirror. This allows the experiment to be
"unfolded" by replacing the effective reflection by a straight-through path, as shown in
Figure 4. The point of the unfolding is that the entangled photons behave exactly as
would be the case if the direction of the deflected photon was reversed, so that it
originated at the detection point D1, passed through one or two slits at C and D, and
produced a one or two slit interference pattern at X2 detected by D2.
Why is the coincidence needed? First, it should be clear from Figure 2 that detector D2
detects not only the entangled twins of the photons that pass through the slit openings,
but also the entangled twins of the much larger number of photons that are stopped by
the opaque parts of the slits. Therefore, without coincidences, no interference pattern
could possibly be observed at X2, Moreover, one can see from Figure 4b that detector D1
behind the slits receives light in a very localized region, and if it were moved vertically
in the diagram, the interference pattern at D2 would be shifted, with maxima becoming
minima and vice versa. Without coincidences requiring a particular location for the
detection at D1, the D2 distribution would have to average over all possible D1 positions,
washing out the two-slit interference pattern. Therefore, because of the geometry used,
the Ghost Interference experiment required a coincidence to observe a two-slit
interference pattern like the one shown in Figure 3a.
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