2021
DOI: 10.1088/1751-8121/ac2321
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The Schwinger action principle for classical systems*

Abstract: We use the Schwinger action principle to obtain the equations of motion in the Koopman–von Neumann operational version of classical mechanics. We restrict our analysis to non-dissipative systems. We show that for velocity-independent forces the Schwinger action principle can be interpreted as a variational principle.

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Cited by 6 publications
(7 citation statements)
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“…In this section, we show two methods to obtain the Heisenberg equation of motion for the position and velocity operators from the variation of an action operator. The results given here are an expansion of the ones given in [35].…”
Section: Action Principlesmentioning
confidence: 92%
See 1 more Smart Citation
“…In this section, we show two methods to obtain the Heisenberg equation of motion for the position and velocity operators from the variation of an action operator. The results given here are an expansion of the ones given in [35].…”
Section: Action Principlesmentioning
confidence: 92%
“…In section 6 we derive the Lagrange equation of motion from the variation of the so-called Schwinger action, extending previous work on the Schwinger action principle [35] to systems with holonomic constraints. We comment on the possible relation of the Schwinger action principle with the Gauss principle of least constraints.…”
Section: Introductionmentioning
confidence: 93%
“…In the case of pure states, this difficulty was resolved with the demonstration that the Wigner function should be interpreted as a phase space probability amplitude. This is in direct analogy with the Koopman-von Neumann (KvN) representation of classical dynamics [19,[21][22][23][24][25][26][27][28][29][30][31][32][33] which explicitly admits a wavefunction on phase space, and which the Wigner function of a pure state corresponds to in the classical limit. The extension of this interpretation to mixed states has to date been lacking however, given that such states must be described by densities and therefore lack a direct correspondence to wavefunctions.…”
Section: Introductionmentioning
confidence: 93%
“…However, its utility is limited in comparison to the classical counterpart because the phase space variables are merely formal parameters, half of which are implicitly defined and are hard to compute. In contrast, the Feynman's path integral approach [7], which is closely related to the Schwinger quantum action principle [8][9][10], can be specialized in terms of conventional phase space variables and is useful in a plethora of applications, from chemistry to quantum gravitation [11][12][13][14][15][16]. However, this approach involves the trajectory-selecting variational analysis only at the level of the semiclassical stationary phase approximation.…”
Section: Introductionmentioning
confidence: 99%