It is shown that the nonlinear wave equation $\partial^2_t \phi -\partial^2_x \phi -\mu_0 \partial_x(\partial_x \phi)^3=0$, which is the continuum limit of the Fermi-Pasta-Ulam $\beta$ model, has a positive Lyapunov exponent $\lambda_1$ , whose analytic energy dependence is given. The result (a first example for field equations) is achieved by evaluating the lattice-spacing dependence of $\lambda_1$ for the FPU model within the framework of a Riemannian description of Hamiltonian chaos. We also discuss a difficulty of the statistical mechanical treatment of this classical field system, which is absent in the dynamical description.

Analytic Lyapunov exponents in a classical nonlinear field equation

Franzosi Roberto;Franzosi Roberto;
2000

Abstract

It is shown that the nonlinear wave equation $\partial^2_t \phi -\partial^2_x \phi -\mu_0 \partial_x(\partial_x \phi)^3=0$, which is the continuum limit of the Fermi-Pasta-Ulam $\beta$ model, has a positive Lyapunov exponent $\lambda_1$ , whose analytic energy dependence is given. The result (a first example for field equations) is achieved by evaluating the lattice-spacing dependence of $\lambda_1$ for the FPU model within the framework of a Riemannian description of Hamiltonian chaos. We also discuss a difficulty of the statistical mechanical treatment of this classical field system, which is absent in the dynamical description.
2000
Bose-Einstein condensation
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/271223
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