About the Feynman Path Integral and Principle of Least Time

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SUMMARY

The discussion clarifies that in the context of the Feynman Path Integral, all paths contribute to the integral, not just the shortest path. The method of stationary phase is employed to approximate the path integral, revealing that the most significant contributions arise from paths that adhere to classical equations of motion. This insight challenges the common misconception surrounding Fermat's principle and the dominance of the shortest path in path integrals.

PREREQUISITES
  • Understanding of Feynman Path Integral
  • Familiarity with Fermat's Principle
  • Knowledge of the method of stationary phase
  • Basic grasp of classical mechanics and equations of motion
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  • Explore the mathematical formulation of the Feynman Path Integral
  • Study the method of stationary phase in detail
  • Investigate the implications of Fermat's Principle in optics
  • Learn about classical equations of motion in physics
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Physicists, students of quantum mechanics, and anyone interested in the mathematical foundations of path integrals and classical motion principles.

EsbMtrx
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I don't entirely get why we usually say that only the shortest path contributes in the path integral. If you calculate the volume of nth fresnel zones which is the locus where the path length is between n-1 and n wavelengths from the shortest path in 3 dimensions, they are the same I believe. So I figured each path length is contributed by the same number of paths and the shortest one wouldn't dominate. My question pertains to Fermat's principle.

ps: this is my first thread here so I apologize in advance if I did anything wrong
 
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It is not correct that only the shortest path contributes in the path integral. All paths contribute. However, you can use the method of stationary phase to approximate the path integral, and then you find that the largest contribution is from the paths that satisfy the classical equations of motion.
 
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