Definition

An oscillatory integral with large parameter λ\lambda has the form

I(λ)=Rneiλϕ(x)a(x)dx,I(\lambda)=\int_{\mathbb R^n}e^{i\lambda\phi(x)}a(x)\,dx,

where the real-valued function ϕ\phi is the phase and aa is the amplitude. The term may also denote an operator obtained by allowing the phase and amplitude to depend on input and output variables.

Cancellation

Away from of ϕ\phi, gives decay faster than the absolute-value estimate. Near nondegenerate critical points, stationary phase gives an asymptotic expansion whose leading order is λn/2\lambda^{-n/2}.

Fourier-like relations

Fourier transformation is the model oscillatory integral. In quantum chaos, incoming and outgoing boundary data are related by oscillatory integral operators, so simultaneous localization becomes a question.

References
  1. Lars Hörmander, The Analysis of Linear Partial Differential Operators I, Springer, 2003. DOI record.