Abstract
We define a canonical system as a canonical manifoldM plus a canonical vectorfield onM. For such systems a unique kinematical interpretation is deduced from a set of Kinematical Axioms satisfied by the algebra of differentiable functions onM. This algebra is required to contain a subalgebra which is maximal commutative under the Poisson bracket.M is shown to be diffeomorphic to the cotangent bundle over its quotient manifold, which is defined by the given subalgebra. Canonical systems satisfying these axioms are then classified. If the “phase space interpretation” is adopted they are shown to describe the motion of masspoints in some configuration space under the influence of and interacting by arbitrary vector and scalar potentials.
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Communicated by J. Ehlers
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Drühl, K. On the space-time interpretation of classical canonical systems I: The general theory. Commun.Math. Phys. 49, 277–288 (1976). https://doi.org/10.1007/BF01608732
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DOI: https://doi.org/10.1007/BF01608732