The Fourier transform is a unitary operator from $L^2$ to $L^2$. But all infinite-dimensional Hilbert spaces are isometrically isomorphic to $L^2$. So that means we can define the Fourier transform on arbitrary infinite-dimensional Hilbert spaces.
So my question is, what does the Fourier transform look like on an arbitrary infinite-dimensional Hilbert space? Can it still be defined in terms of an integral?