Possible Paths and Interference Patterns in the Double Slit Experiment

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SUMMARY

The discussion centers on the interpretation of "all possible paths" in Richard Feynman's double slit experiment, specifically regarding the calculation of interference patterns. It concludes that when determining the probability of detection at a location, one must sum the amplitudes of paths through both slits A and B, then square the absolute value of the result. The interference pattern can be derived from this method, although solving the Schrödinger equation for the two-slit problem is suggested as a more straightforward approach. Recommended resources include Feynman's book "QED: The Strange Theory of Light and Matter" and related lecture videos.

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San K
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Does "all possible paths", per fenyman, mean (say in a single particle double slit):

Slit a & b
or does it mean
slit a & b plus slit a plus slit b

how is the interference pattern calculated?

also when we try to get which way :
Could we say that now some of the paths now are no longer possible/valid and hence no interference pattern?
 
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It means that the probability of detection at a given location is calculated by adding the amplitude associated with the path through A (from the emitter to the given location) to the amplitude associated with the path through B, and then taking the square of the absolute value of the result.

I recommend the book "QED: The strange theory of light and matter" by Richard Feynman, and the videos of the lectures that this book is based on.

The interference pattern could in principle be calculated this way, but I suspect that it's easier to just solve the Schrödinger equation for the two-slit problem. I have never calculated it myself though.
 

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