We introduce a Hamiltonian framework tailored to degrees of freedom (DOF) of field theories that reside in suitable 3-dimensional open regions, and then apply it to the gravitational DOF of general relativity. Specifically, these DOF now refer to open regions ^R of null infinity I⁺, and R of black hole (and cosmological) horizons Δ representing equilibrium situations. At I⁺ the new Hamiltonian framework yields the well-known BMS fluxes and charges. By contrast, all fluxes vanish identically at Δ just as one would physically expect. In the companion paper [Phys. Rev. D 110, 044048 (2024).] we showed that, somewhat surprisingly, the geometry and symmetries of I⁺ and Δ descend from a common framework. This paper reinforces that theme: Very different physics emerges in the two cases from a common Hamiltonian framework because of the difference in the nature of degrees of freedom on I⁺ and Δ, discussed in the companion paper. Finally, we compare and contrast this Hamiltonian approach with those available in the literature.
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Ashtekar et al. (2024) studied this question.
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