2003
DOI: 10.1063/1.1576904
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The algebraic entropy of classical mechanics

Abstract: We describe the 'Lie algebra of classical mechanics', modelled on the Lie algebra generated by kinetic and potential energy of a simple mechanical system with respect to the canonical Poisson bracket. It is a polynomially graded Lie algebra, a class we introduce. We describe these Lie algebras, give an algorithm to calculate the dimensions c n of the homogeneous subspaces of the Lie algebra of classical mechanics, and determine the value of its entropy lim n→∞ c

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Cited by 7 publications
(6 citation statements)
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“…This allows methods, usually known as 'Runge-Kutta-Nyström' methods, with smaller errors and often with fewer force evaluations as well. A full analysis of the Lie algebra generated by f 1 and f 2 for simple mechanical systems is provided in [96].…”
Section: Simple Mechanical Systemsmentioning
confidence: 99%
“…This allows methods, usually known as 'Runge-Kutta-Nyström' methods, with smaller errors and often with fewer force evaluations as well. A full analysis of the Lie algebra generated by f 1 and f 2 for simple mechanical systems is provided in [96].…”
Section: Simple Mechanical Systemsmentioning
confidence: 99%
“…It is, however, distinct from this established definition in that there is no underlying set of recurrence inequalities to provide additional structure (see, for example, [37,Lemma 4.1.7]). The proposed entropy concept also coincides in certain special cases (modulo a logarithm) with the notion of entropy defined for graded algebras [40,41]. But that connection does not appear to be so important for the present work.…”
Section: Introductionmentioning
confidence: 72%
“…The main point here is that in the case (69) (we will refer to that as the RKN case), [[[F [b] , F [a] ], F [b] ], F [b] ] = 0 identically. This is equivalent to F [babb] = 0 in (53), which introduces some linear dependencies among higher order terms in the expansion of log(Ψ(h)) (see [59] for a detailed study). This means that the characterization given in Theorem 1 for a splitting integrator (36) to be of order r (for r ≥ 4) is no longer applicable if one restricts to the case (69).…”
Section: Runge-kutta-nyström Methodsmentioning
confidence: 99%