On the angle between the first and the second Lyapunov vectors in spatio-temporal chaos
arXiv:1311.7548 · doi:10.1088/1751-8113/46/25/254014
Abstract
In a dynamical system the first Lyapunov vector (LV) is associated with the largest Lyapunov exponent and indicates ---at some point on the attractor--- the direction of maximal growth in tangent space. The LV corresponding to the second largest Lyapunov exponent generally points at a different direction, but tangencies between both vectors can in principle occur. Here we find that the probability density function (PDF) of the angle ψspanned by the first and the second LVs should be expected approximately symmetric around π/4 and peaked at 0 and π/2. Moreover, for small angles we uncover a scaling law for the PDF Q of ψ_l=\lnψwith the system size L: Q(ψ_l)=L^{-1/2} f(ψ_l L^{-1/2}). We give a theoretical argument that justifies this scaling form and also explains why it should be universal (irrespective of the system details) for spatio-temporal chaos in one spatial dimension.
12 pages
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