2013
DOI: 10.1103/physrevd.87.067501
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Least-action principle and path-integral for classical mechanics

Abstract: In this paper we show how the equations of motion of a superfield, which makes its appearance in a path-integral approach to classical mechanics, can be derived without the need of the least-action principle

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Cited by 6 publications
(12 citation statements)
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“…A quick check of the symmetries, especially the ghost number makes it clear that we are talking about an N T = 2 multiplet as discussed in the text. The occurrence of this topological symmetry algebra has been noted in the literature [68,69]. These references were interested in providing a path integral formulation of classical mechanics as a counterpart to the operator formalism developed by Koopman and von Neumann [70,71].…”
Section: Stochastic Dynamicsmentioning
confidence: 95%
“…A quick check of the symmetries, especially the ghost number makes it clear that we are talking about an N T = 2 multiplet as discussed in the text. The occurrence of this topological symmetry algebra has been noted in the literature [68,69]. These references were interested in providing a path integral formulation of classical mechanics as a counterpart to the operator formalism developed by Koopman and von Neumann [70,71].…”
Section: Stochastic Dynamicsmentioning
confidence: 95%
“…We said before that we can realize theλ a as a derivative operator (like in Eq. (13) and obviously the ϕ a as a multiplicative one:φ a |ϕ = ϕ a |ϕ .…”
Section: The Evolution Of ψ(Q P) Is Given By the Liouville Equationmentioning
confidence: 99%
“…Simulation model of a cubic lattice consists of the parameter points x = d (n 0 , n 1 , n 2 , n 3 ) where d is the lattice spacing and n 1 , n 2 , n 3 are reciprocical lattice vectors where n 0 is redundant parameter. Numerical simulation of channeled ion trajectories coherent in spacetime with a lattice, is performed applying the path integral formalism [18,19] across a system ((1 1 0) Si crystal plane) whose degrees of freedom are related to effective potential field variable / x at each lattice site x. In order to immerse into the simulation model the effective potential induced by the planar channeling oscillations, we applied the prescription for the path integral in the momentum space where particle's Hamiltonian is H = p(t) 2 / 2m + 1/2mx 2 q 2 , (p, q e R 3 ) and p(t) 2 = P j p j (t) 2 ; incorporating the particle dynamics into the former Hamiltonian while summing over all possible paths and integrating over all possible momenta within specified time interval gives where U pl (p(t)) is the total potential in momentum space, which is experienced by the particle as a sum of the potentials of all the planes:…”
Section: Simulation Modelmentioning
confidence: 99%