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How is it proved that the extremal of the action obtained with Hamilton's principle in classical mechanics or classical field theory is in fact a minimum of the action and not just a stationary point? Furthermore how does one show that this minimum is unique? Is it correct to state that the uniqueness of the minimal path follows from the ability to apply the Picard-Lindeloef theorem to the Euler-Lagrange equation?

Qmechanic
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ErwinS
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