Maximally Chaotic Dynamical Systems and Fundamental Interactions

Abstract

We give a general review on the application of Ergodic theory to the investigation of dynamics of the Yang-Mills gauge fields and of the gravitational systems, as well as its application in the Monte Carlo method and fluid dynamics. In ergodic theory the maximally chaotic dynamical systems (MCDS) can be defined as dynamical systems that have nonzero Kolmogorov entropy. The hyperbolic dynamical systems that fulfil the Anosov C-condition belong to the MCDS insofar as they have exponential instability of their phase trajectories and positive Kolmogorov entropy. It follows that the C-condition defines a rich class of MCDS that span over an open set in the space of all dynamical systems. The large class of Anosov-Kolmogorov MCDS is realised on Riemannian manifolds of negative sectional curvatures and on high-dimensional tori. The interest in MCDS is rooted in the attempts to understand the relaxation phenomena, the foundations of the statistical mechanics, the appearance of turbulence in fluid dynamics, the non-linear dynamics of Yang-Mills field and gravitating N-body systems as well as black hole thermodynamics. Our aim is to investigate classical-and quantum-mechanical properties of MCDS and their role in the theory of fundamental interactions.

Classical and quantum butterfly effect in nonlinear vector mechanics

“…Finally, note that the model (1.3) is very similar to some spatially reduced string and gauge models [93,[99][100][101][102][103][104][105][106][107][108][109]. In particular, the N = 3 variant of (1.3) is nothing but a spatially reduced SU (2) Yang-Mills [99], which is known to possess a nonzero classical Lyapunov exponent κ ∼ 4 √ E, see [93,[100][101][102].…”