In mathematics, Nambu dynamics is a generalization of Hamiltonian mechanics involving multiple Hamiltonians. Recall that Hamiltonian mechanics is based upon the flows generated by a smooth Hamiltonian over a symplectic manifold. The flows are symplectomorphisms and hence obey Liouville's theorem. This was soon generalized to flows generated by a Hamiltonian over a Poisson manifold. In 1973, Yoichiro Nambu suggested a generalization involving NambuPoisson manifolds with more than one Hamiltonian.
Specifically, consider a differential manifold M, for some integer N ≥ 2; one has a smooth Nlinear map from N copies of C∞ (M) to itself, such that it is completely antisymmetric: the Nambu bracket, {h_{1}, ..., h_{N−1}, .}, which acts as a derivation {h_{1}, ..., h_{N−1},fg} = {h_{1}, ..., h_{N−1}, f} g + f {h_{1}, ..., h_{N−1}, g}; whence the Filippov Identities (FI), (evocative of the Jacobi identities, but unlike them, not antisymmetrized in all arguments, for N ≥ 2 ):
so that {f_{1}, ..., f_{N−1}, •} acts as a generalized derivation over the Nfold product {. ,..., .}.
There are N − 1 Hamiltonians, H_{1}, ..., H_{N−1}, generating an incompressible flow,

 d⁄_{dt} f= {f, H_{1}, ..., H_{N−1}}.
The generalized phasespace velocity is divergenceless, enabling Liouville's theorem. The case N = 2 reduces to a Poisson manifold, and conventional Hamiltonian mechanics.
For larger even N, the N−1 Hamiltonians identify with the maximal number of independent invariants of motion (cf. Conserved quantity) characterizing a superintegrable system which evolves in Ndimensional phase space. Such systems are also describable by conventional Hamiltonian dynamics; but their description in the framework of Nambu mechanics is substantially more elegant and intuitive, as all invariants enjoy the same geometrical status as the Hamiltonian: the trajectory in phase space is the intersection of the N−1 hypersurfaces specified by these invariants. Thus, the flow is perpendicular to all N−1 gradients of these Hamiltonians, whence parallel to the generalized cross product specified by the respective Nambu bracket.
Quantizing Nambu dynamics leads to intriguing structures which coincide with conventional quantization ones when superintegrable systems are involved—as they must.
Famous quotes containing the word mechanics:
“It is only the impossible that is possible for God. He has given over the possible to the mechanics of matter and the autonomy of his creatures.”
—Simone Weil (1909–1943)