An averaging theorem for FPU in the thermodynamic limit
Consider an FPU chain composed of N ≫ 1 N≫ 1 particles, and endow the phase space
with the Gibbs measure corresponding to a small temperature β^-1 β-1. Given a fixed KK, we
construct KK packets of normal modes whose energies are adiabatic invariants (ie, are
approximately constant for times of order β^ 1-a β 1-a, a> 0 a> 0) for initial data in a set of
large measure. Furthermore, the time autocorrelation function of the energy of each packet
does not decay significantly for times of order β β. The restrictions on the shape of the …
with the Gibbs measure corresponding to a small temperature β^-1 β-1. Given a fixed KK, we
construct KK packets of normal modes whose energies are adiabatic invariants (ie, are
approximately constant for times of order β^ 1-a β 1-a, a> 0 a> 0) for initial data in a set of
large measure. Furthermore, the time autocorrelation function of the energy of each packet
does not decay significantly for times of order β β. The restrictions on the shape of the …
Abstract
Consider an FPU chain composed of particles, and endow the phase space with the Gibbs measure corresponding to a small temperature . Given a fixed , we construct packets of normal modes whose energies are adiabatic invariants (i.e., are approximately constant for times of order , ) for initial data in a set of large measure. Furthermore, the time autocorrelation function of the energy of each packet does not decay significantly for times of order . The restrictions on the shape of the packets are very mild. All estimates are uniform in the number of particles and thus hold in the thermodynamic limit , .
Springer
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