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We review the convergence of chaotic integrals computed by Monte Carlo simulation, the trace method, dynamical zeta function, and Fredholm determinant on a simple one-dimensional example: the parabola repeller. There is a dramatic difference in convergence between these approaches. The convergence of the Monte Carlo method follows an inverse power law, whereas the trace method and dynamical zeta function converge exponentially, and the Fredholm determinant converges faster than any exponential.
dynamical zeta function, FOS: Physical sciences, Nonlinear Sciences - Chaotic Dynamics, Strange attractors, chaotic dynamics of systems with hyperbolic behavior, Monte Carlo method, Dynamical systems involving maps of the interval, trace method, chaotic integrals, Fredholm determinant, Numerical integration, Relations of infinite-dimensional Hamiltonian and Lagrangian dynamical systems with algebraic geometry, complex analysis, and special functions, Chaotic Dynamics (nlin.CD)
dynamical zeta function, FOS: Physical sciences, Nonlinear Sciences - Chaotic Dynamics, Strange attractors, chaotic dynamics of systems with hyperbolic behavior, Monte Carlo method, Dynamical systems involving maps of the interval, trace method, chaotic integrals, Fredholm determinant, Numerical integration, Relations of infinite-dimensional Hamiltonian and Lagrangian dynamical systems with algebraic geometry, complex analysis, and special functions, Chaotic Dynamics (nlin.CD)
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