Sobolev stability of plane wave solutions to the cubic nonlinear Schrödinger equation on a torus
(2013)
It is shown that plane wave solutions to the cubic nonlinear Schrödinger equation on a torus behave orbitally stable under generic perturbations of the initial data that are small in a high-order Sobolev norm, over long times that extend to arbitrary negative powers of the smallness parameter. The perturbation stays small in the same Sobolev norm over such long times. The proof uses a Hamiltonian reduction and transformation and, alternatively, Birkhoff normal forms or modulated Fourier expansions in time.
We consider multiscale Hamiltonian systems in which harmonic oscillators with several high frequencies are coupled to a slow system. It is shown that the oscillatory energy is nearly preserved over long times eps^{-N} for arbitrary N>1, where eps^{-1} is the size of the smallest high frequency. The result is uniform in the frequencies and does not require non-resonance conditions.
We give an algorithm to compute N steps of a convolution quadrature approximation
to a continuous temporal convolution using only O(N logN) multiplications and O(logN) active
memory. The method does not require evaluations of the convolution kernel, but instead O(logN)
evaluations of its Laplace transform, which is assumed sectorial. The algorithm can be used for the
stable numerical solution with quasi-optimal complexity of linear and nonlinear integral and integrodifferential
equations of convolution type. In a numerical example we apply it to solve a subdiffusion
equation with transparent boundary conditions.
To approximate convolutions which occur in evolution equations with memory terms, a variable-stepsize algorithm is presented for which advancing $N$ steps requires only $O(N\log N)$ operations and $O(\log N)$ active memory, in place of $O(N^2)$ operations and $O(N)$ memory for a direct implementation. A basic feature of the fast algorithm is the reduction, via contour integral representations, to differential equations which are solved numerically with adaptive step sizes. Rather than the kernel itself, its Laplace transform is used in the algorithm. The algorithm is illustrated on three examples: a blow-up example originating from a Schrödinger equation with concentrated nonlinearity, chemical reactions with inhibited diffusion, and viscoelasticity with a fractional order constitutive law.