2009/01/21 by R. N. Ghalati, Ghalati, R. N. · 1 citation
Physics and Astronomy · #Black Holes and Theoretical Physics #Cosmology and Gravitation Theories #FOS: Physical sciences #General Relativity and Quantum Cosmology (gr-qc) #Quantum chaos and dynamical systems #gr-qc
paper · pdf · doi:10.48550/arxiv.0901.3344
35 pages
openalex publication_date 2009/01/21 · arxiv created 2009/04/07 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
A novel Dirac Hamiltonian formulation of the first order Einstein-Hilbert (EH) action, in which algebraic constraints are not solved to eliminate fields from the action at the Lagrangian level, has been shown to lead to an action and a constraint structure apparently distinct from the ADM action and the ADM constraint structure in that secondary first class constraints as well as tertiary first class constraints arise with an unusual Poisson Bracket (PB) algebra [24]. By canonical transformations of the fundamental fields we show how from the tertiary constraints one may derive the Hamiltonian and momentum constraints. Special attention is paid to the Hamiltonian formulation of the first order EH action in terms of the variables h, hi and qij employed in [19,20]. It is shown that the variables h and hi are left undetermined in the formalism. This fact is used for a proper gauge fixation of the secondary constraints and reduction to the Faddeev action [19,20]. Considering invariances of the total action, the generator of the gauge transformations of the EH Lagrangian action is derived. Using this generator, the explicit form of the gauge invariance of the field h is obtained, by which the relation between the gauge functions and the descriptors of the diffeomorphism invariance is determined in order for the gauge transformations to correspond to diffeomorphism invariance. By linearizing the novel Hamiltonian formulation of [24], the Hamiltonian formulation of the first order action for the free spin two field [4,24] is derived.