Abstract

Using double 2+2 and 3+1 nonholonomic fibrations on Lorentz manifolds, we extend the concept of W-entropy for gravitational fields in general relativity (GR). Such F- and W-functionals were introduced in the Ricci flow theory of three dimensional (3-d) Riemannian metrics by Perelman (the entropy formula for the Ricci flow and its geometric applications. arXiv:math.DG/0211159). Non-relativistic 3-d Ricci flows are characterized by associated statistical thermodynamical values determined by W-entropy. Generalizations for geometric flows of 4-d pseudo-Riemannian metrics are considered for models with local thermodynamical equilibrium and separation of dissipative and non-dissipative processes in relativistic hydrodynamics. The approach is elaborated in the framework of classical field theories (relativistic continuum and hydrodynamic models) without an underlying kinetic description, which will be elaborated in other work. The 3+1 splitting allows us to provide a general relativistic definition of gravitational entropy in the Lyapunov–Perelman sense. It increases monotonically as structure forms in the Universe. We can formulate a thermodynamic description of exact solutions in GR depending, in general, on all spacetime coordinates. A corresponding 2+2 splitting with nonholonomic deformation of linear connection and frame structures is necessary for generating in very general form various classes of exact solutions of the Einstein and general relativistic geometric flow equations. Finally, we speculate on physical macrostates and microstate interpretations of the W-entropy in GR, geometric flow theories and possible connections to string theory (a second unsolved problem also contained in Perelman’s work) in Polyakov’s approach.

Highlights

  • 1 Introduction damental results in geometric analysis and topology

  • Using double 2 + 2 and 3 + 1 nonholonomic fibrations on Lorentz manifolds, we extend the concept of W-entropy for gravitational fields in general relativity (GR)

  • There is a standard theory of the thermodynamics of the black hole (BH) solutions originally elaborated by Bekenstein– Hawking constructions for stationary solutions in gravity theories

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Summary

Induced N-adapted 3-d hypersurface metrics

We define the first fundamental form (the induced 3-metric) on :. We introduce the concept of a unit normal d-vector, n, to a which is constructed following such a procedure. Such d-vectors can be used for various models of geometric flow evolution and thermodynamic models. For any d-vector v which is tangent to , the conditions dt, v = 0 and −→e t allow one to define the unique direction normal to a not null. The unit normal vector to supersurfaces, nα ∝ ∂αt, when ∂α := ∂/∂uα, can be constructed for a future-directed timelike vector field. It is useful to define the unit normal nα to the hypersurfaces when nα = −N ∂αt and nαeαı = 0.

Induced 3-d hypersurface ‘preferred’ linear connections
Important formulas on space-like N-adapted hypersurfaces
Geometric evolution of Einstein gravitational fields
Distortion relations on induced linear connections
Nonholonomc Perelman’s functionals on 3-d hypersurfaces
Nonholonomic Ricci flow evolution equations for 3-d hypersurface metrics
Geometric evolution to 4-d Lorentz configurations as exact solutions in GR
Generation of off-diagonal solutions
The Levi-Civita conditions
Solutions with nonholonomically induced torsion
LC-varieties for effective Einstein manifolds
Off-diagonal deformations of physically important solutions in GR
Ellipsoid Kerr–de Sitter configurations
Nonholonomically deformed wormhole configurations
Solitonic waves for inhomogeneous cosmological solutions
Off-diagonal deformations of FLRW metrics and gravitational solitonic waves
Nonholonomic thermodynamics of gravitational fields
General relativistic models of W-entropy and geometric flow evolution
W-thermodynamic values for exact solutions in GR
Modified 3-d Ricci flows with induced nonholonomic torsion
Modified 3-d Ricci flows of LC-configurations
N-adapted 3-d Ricci flows on exact solutions in GR
Relativistic thermodynamic values for N-adapted 3-d modified Ricci flows
Parameterizations for the CET model
Final remarks and conclusions
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