2010
DOI: 10.48550/arxiv.1010.2021
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Diffusion and Self-Organized Criticality in Ricci Flow Evolution of Einstein and Finsler Spaces

Sergiu I. Vacaru

Abstract: Imposing non-integrable constraints on Ricci flows of (pseudo) Riemannian metrics we model mutual transforms to, and from, non-Riemannian spaces. Such evolutions of geometries and physical theories can be modelled for nonholonomic manifolds and vector/ tangent bundles enabled with fundamental geometric objects determining Lagrange-Finsler and/or Einstein spaces. Prescribing corresponding classes of generating functions, we construct different types of stochastic, fractional, nonholonomic etc models of evolutio… Show more

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Cited by 5 publications
(30 citation statements)
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“…Following the Carathéodory measure theoretic idea [49] and Birkhoff's approach to ergodicity [50,51], we can clarify the relation between ergodic and recurrent systems. In the case of geometric flows, we can define ergodicity by replacing Boltzmann's sets with sets of of non zero volume measure which was generalized for nonholonomic manifolds and generalized Finsler spaces in [52,53,54,17]. Here we note that geometric flows as ergodic systems are recurrent but not vice versa.…”
Section: Relativistic Models Of Geometric Flow Thermodynamicsmentioning
confidence: 99%
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“…Following the Carathéodory measure theoretic idea [49] and Birkhoff's approach to ergodicity [50,51], we can clarify the relation between ergodic and recurrent systems. In the case of geometric flows, we can define ergodicity by replacing Boltzmann's sets with sets of of non zero volume measure which was generalized for nonholonomic manifolds and generalized Finsler spaces in [52,53,54,17]. Here we note that geometric flows as ergodic systems are recurrent but not vice versa.…”
Section: Relativistic Models Of Geometric Flow Thermodynamicsmentioning
confidence: 99%
“…Let us associate a non-stretching curve γ(τ, l) on a Einstein manifold V to geometric evolution of a dmetric g(τ ), where τ can be identified with the geometric flow parameter of temperature type and l is the arclength of the curve, see details in [53,58,59]. Such a curve is characterized by an evolution d-vector Y = γ τ and tangent d-vector X = γ l for which g(X, X) =1.…”
Section: Generating Cosmological Solitonic Hierarchiesmentioning
confidence: 99%
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