Question:
How to reduce the Feynman Integral to classical action?
Solution:
Recall that the Feynman Integral reduce to classical action when we take the exponential term to minimum, as required for the Laplace method. So the answer is
$ \delta S[x(t)] = 0 $
How to reduce the Feynman Integral to classical action?
Solution:
Recall that the Feynman Integral reduce to classical action when we take the exponential term to minimum, as required for the Laplace method. So the answer is
$ \delta S[x(t)] = 0 $
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