In General Relativity, the Hamiltonian formulation of the dynamics and the Poisson bracket of observables depend on the choice of a codimension 1 submanifold as initial time-slice. But such a submanifold is not invariant under diffeomorphisms. As a consequence, Noether's first theorem, which associates to a symmetry a conserved momentum, does not define a homomorphism of Lie algebras. Starting in the 1960s, this issue has led to the development of multisymplectic geometry, eventually replacing the Poisson algebra of momenta with an $L_\infty$-algebra of currents. I will show that:
Links:
[1] https://www.mpim-bonn.mpg.de/taxonomy/term/39
[2] https://www.mpim-bonn.mpg.de/node/3444
[3] https://www.mpim-bonn.mpg.de/node/13069