This paper is concerned with a novel exponential wave integrator Fourier pseudo-spectral method for simulating the long-term dynamics of the nonlinear Schrödinger equation with a wave operator under weak nonlinearity, characterized by \(0 < ε 1\). The proposed method exhibits several notable features: it is symmetric or reversible in time, highly accurate in both temporal and spatial directions, and able to simultaneously approximate both \(u\) and its temporal derivative \(∂_t u\) at each time step. A key technique in deriving our numerical method is to adopt the corrected trapezoidal rule, which enables the proposed scheme to achieve high-order temporal accuracy. An optimal and uniform error estimate is established for a time period up to \(T = O(ε-β)\) with \(β ∈ [0,2]\); the error bound is \((ε2-βτ^4 + hᵐ⁻¹)\) in the discrete \(H^1\) norm to the approximation of \(u\) and in the discrete \(L^2\) norm to the approximation of \(∂_t u\) with time step \(τ\) and mesh size \(h\). Numerical experiments are carried out to confirm our theoretical analysis.
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Cheng et al. (2026) studied this question.
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