Applying Huygens's principle to light propagation

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Huygens's principle describes light propagation by modeling all points along a wave front as point sources for new waves, effectively explaining phenomena like diffraction. It suggests that light travels in straight lines because all potential photon paths cancel out except those in a narrow beam. The discussion raises a question about why photons appear to travel only in one direction along their path, positing that they could theoretically move both forwards and backwards. However, it is proposed that two closely spaced wave fronts, with a 180º phase shift, lead to constructive interference in one direction and destructive interference in the opposite, resulting in zero probability for backward travel. This explanation aligns with current understanding and is considered an accepted model in the field.
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I was taught that Huygens's principle is an accurate description of the way light propagates. Something like: "All points along a wave front can be modeled as point-sources for new waves having the same phase and frequency." This appears to be a good model to explain phenomena such as diffraction.

From my limited understanding, Huygens's principle also explains why light* travels in approximately straight lines: all possible photon paths cancel destructively except for those in a narrow central ~cylindrical beam. (Not sure about the exact "shape" of the beam. I assume a cylinder or cone as an approximation.)

The above explanation is well and good, and I understand some parts of it to a limited degree, but there is one point that I don't understand at all. If Hugens's principle explains why light travels in a straight line, does it also explain why light travels in (apparently) only the positive or negative direction along that line--but not both? My interpretation of Huygens's principle, when applied to a photon, is that the photon has equal probability to travel forwards (along its straight-line path/cylinder) as backwards. Furthermore, the photon need not travel only in the positive direction, or only in the negative, but could alternate between the two directions anywhere up to an infinite number of times between its emission and eventual absorption--if absorption ever occurred--and could hence be inferred to have traveled at any speed < c.

What is wrong with this reasoning?

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* Further question: does a photon have to be coming from an extended source in order to have directionality? By "extended source" I mean something like a slit or hole; and by "having directionality" I mean that the photon propagates in a manner other than symmetrically in all directions, as an expanding sphere. For example, a photon from a laser would be "highly directional".
 
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Thank you, jtbell, that is just what I needed!

So, if I understand the gist of Miller's paper (http://www-ee.stanford.edu/~dabm/146.pdf) whenever light propagates, there is not just one wave front, but two closely spaced wave fronts. The second wave front chases the first, trailing behind it by an infinitesimal distance, and is also phase-shifted by 180º w.r.t. the first wave front. This phase shift causes total constructive phase interference in one direction ("forwards") and total destructive interference in the opposite direction ("backwards"). The result is a zero probability of the photon traveling "backwards". This is a fairly neat explanation. Is it the accepted model?
 
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