Brane-world Quantum Gravity
arXiv:0704.1289 · doi:10.1088/1126-6708/2007/04/047
Abstract
The Arnowitt-Deser-Misner canonical formulation of general relativity is extended to the covariant brane-world theory in arbitrary dimensions. The exclusive probing of the extra dimensions makes a substantial difference, allowing for the construction of a non-constrained canonical theory. The quantum states of the brane-world geometry are defined by the Tomonaga-Schwinger equation, whose integrability conditions are determined by the classical perturbations of submanifolds contained in the Nash's differentiable embedding theorem. In principle, quantum brane-world theory can be tested by current experiments in astrophysics and by near future laboratory experiments at Tev energy. The implications to the black-hole information loss problem, to the accelerating cosmology, and to a quantum mathematical theory of four-sub manifolds are briefly commented.
14 pages, no figures, JHEP format, to appear in JHEP April 2007
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Cited by in corpus (6)
- Classical tests in brane gravity
- Geometrical aspects on the dark matter problem
- On the thermal stability of a static spherically symmetric black holes in Nash embedding framework
- Lower tensor-to-scalar ratio as possible signature of modified gravity
- Variation of mass in primordial nucleosynthesis as a test of Induced Matter Brane Gravity
- Probing dynamical embeddings in a five-dimensional spacetime in light of DESI BAO