On the cosmological constant in the deformed Einstein-Cartan gauge gravity in De Donder-Weyl Hamiltonian formulation
D. Vasak, J. Kirsch, J. Struckmeier, H. Stoecker

TL;DR
This paper proposes a modified gravity theory based on the De Donder-Weyl Hamiltonian formulation that predicts a vanishing total energy-momentum and offers a natural explanation for the small observed cosmological constant.
Contribution
It introduces Covariant Canonical Gauge Gravity (CCGG), a quadratic extension of Einstein-Cartan theory, which predicts a zero total energy-momentum and explains the smallness of the cosmological constant.
Findings
Predicts a vanishing total energy-momentum of space-time and matter.
Shows the observed cosmological constant is a small correction from deviations and dynamical effects.
Provides a natural resolution to the cosmological constant problem.
Abstract
A modification of the Einstein-Hilbert theory, the Covariant Canonical Gauge Gravity (CCGG), leads to a cosmological constant that represents the energy of the space-time continuum when deformed from its (A)dS ground state to a flat geometry. CCGG is based on the canonical transformation theory in the De Donder-Weyl (DW) Hamiltonian formulation. That framework modifies the Einstein-Hilbert Lagrangian of the free gravitational field by a quadratic Riemann-Cartan concomitant. The theory predicts a total energy-momentum of the system of space-time and matter to vanish, in line with the conjecture of a "Zero-Energy-Universe" going back to Lorentz (1916) and Levi-Civita (1917). Consequently a flat geometry can only exist in presence of matter where the bulk vacuum energy of matter, regardless of its value, is eliminated by the vacuum energy of space-time.% . The observed…
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Taxonomy
TopicsCosmology and Gravitation Theories · Relativity and Gravitational Theory · Black Holes and Theoretical Physics
