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The principle of least action in physics is a historical precursor of the modern understanding that trajectories of particles and configurations of fields realized in classical mechanics are characterized as being the variational extrema or critical loci of a functional on the space of all possible configurations, called the action functional. For typical examples of this principle – some of which were known to the ancient Greeks and which were then formalized in some generality in the 18th century – these extrema are indeed minima, as with, for instance, the propagation of a ray of light through optical media in optics. More generally one speaks of the principle of extremal action or the principle of stationary action. But in fact mostly today one just speaks of the Euler-Lagrange equations of motion, which are the equations that characterize these extremal trajectories.
With the advent of quantum mechanics, the principle of extremal action found an explanation in more fundamental terms as the classical limit of quantum dynamics. A simple, though somewhat heuristic, way to see this is via path integral quantization: whereas propagation in quantum mechanics is given by the path integral by which every trajectory $\phi$ between two prescribed configurations contributes with a probability amplitude given by the exponentiated value $\exp(i S(\phi))$ of the action functional $S$ on this trajectory, at least under some conditions the main contribution to this integral is from trajectories close to the critical points of the action functional.
Last revised on March 18, 2014 at 01:00:42. See the history of this page for a list of all contributions to it.