Nilpotent Classical Mechanics

Details Nilpotent Classical Mechanics Nilpotent Classical Mechanics

2006-09-11

arxiv.org/abs/hep-th/0609072v3

Int.J.Mod.Phys.A22:2513-2534,2007

Physics

High Energy Physics

High Energy Physics - Theory

23 pages, no figures. Corrected version. 2 references added

Scientific paper

10.1142/S0217751X07036749

The formalism of nilpotent mechanics is introduced in the Lagrangian and Hamiltonian form. Systems are described using nilpotent, commuting coordinates $\eta$. Necessary geometrical notions and elements of generalized differential $\eta$-calculus are introduced. The so called $s-$geometry, in a special case when it is orthogonally related to a traceless symmetric form, shows some resemblances to the symplectic geometry. As an example of an $\eta$-system the nilpotent oscillator is introduced and its supersymmetrization considered. It is shown that the $R$-symmetry known for the Graded Superfield Oscillator (GSO) is present also here for the supersymmetric $\eta$-system. The generalized Poisson bracket for $(\eta,p)$-variables satisfies modified Leibniz rule and has nontrivial Jacobiator.

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