x0 $\in R^2$ for the $n$ Fourier frequencies.kern(x0, h, freq)n $\times$ 2 matrix with the n Fourier frequencies, where n is the number of points in the analyzed lattice.x0 $\in R^2$ for the $n$ Fourier frequencies. In particular the $k$-th vector element is
$$e^{-\frac{(\boldsymbol{\omega}_k - x_0)^T(\boldsymbol{\omega}_k - x_0)}{h^2}}.$$scICA, locmulti, grad, hess.