M. Johansson and K. Rasmussen
We extend earlier work [K. Rasmussen et al., Phys. Rev. Lett. 84, 3740
(2000)] on the statistical mechanics of the cubic one-dimensional discrete
nonlinear Schroedinger (DNLS) equation to a more general class of models,
including higher dimensionalities and nonlinearities of arbitrary degree. These
extensions are physically motivated e.g. by the desire to describe situations
with an excitation threshold for creation of localized excitations, as well as
by recent suggestions for non-cubic DNLS models to describe Bose-Einstein
condensates in deep optical lattices, taking into account the effective
condensate dimensionality. Considering ensembles of initial conditions with
given values of the two conserved quantities, norm and Hamiltonian, we calculate
analytically the boundary of the 'normal' Gibbsian regime corresponding to
infinite temperature, and perform numerical simulations to illuminate the nature
of the localization dynamics outside this regime for various cases. Furthermore,
we show quantitatively how this DNLS localization transition manifests itself
for small-amplitude oscillations in generic Klein-Gordon lattices of weakly
coupled anharmonic oscillators (in which energy is the only conserved quantity),
and determine conditions for existence of persistent energy localization over
large time scales.