A note on the foundation of relativistic mechanics. II: Covariant hamiltonian general relativity
arXiv:gr-qc/0202079
Abstract
I illustrate a simple hamiltonian formulation of general relativity, derived from the work of Esposito, Gionti and Stornaiolo, which is manifestly 4d generally covariant and is defined over a finite dimensional space. The spacetime coordinates drop out of the formalism, reflecting the fact that they are not related to observability. The formulation can be interpreted in terms of Toller's reference system transformations, and provides a physical interpretation for the spinnetwork to spinnetwork transition amplitudes computable in principle in loop quantum gravity and in the spin foam models.
arXiv comment7 pages, no figures, 2nd part of gr-qc/0111037
Cited by in corpus (13)
- Fundamental Structure of Loop Quantum Gravity
- Relational Observables in Gravity: a Review
- Change in Hamiltonian General Relativity from the Lack of a Time-like Killing Vector Field
- Multisymplectic unified formalism for Einstein-Hilbert Gravity
- Covariant hamiltonian formalism for field theory: Hamilton-Jacobi equation on the space G
- A simple background-independent hamiltonian quantum model
- Multisymplectic formalism and the covariant phase
- Covariant Momentum Map Thermodynamics for Parametrized Field Theories
- On A Covariant Hamiltonian Description of Palatini's Gravity on Manifolds with Boundary
- Converting Classical Theories to Quantum Theories by Solutions of the Hamilton-Jacobi Equation
- The notion of observable in the covariant Hamiltonian formalism for the calculus of variations with several variables
- On the problem of time in two and four dimensions
- Covariant Hamiltonian formalism for the calculus of variations with several variables: Lepage--Dedecker versus de Donder--Weyl