Abstract

An analytical expression for the maximal Lyapunov exponent λ1λ_1 in generalized Fermi-Pasta-Ulam oscillator chains is obtained. The derivation is based on the calculation of modulational instability growth rates for some unstable periodic orbits. The result is compared with numerical simulations and the agreement is good over a wide range of energy densities εε. At very high energy density the power law scaling of λ1λ_1 with εε can be also obtained by simple dimensional arguments, assuming that the system is ruled by a single time scale. Finally, we argue that for repulsive and hard core potentials in one dimension λ1∼ελ_1 \sim \sqrtε at large εε.

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