arXiv2017
We provide an exact solution of the scattering problem for the potentials of the form $v(x,y)=χ_a(x)[v_0(x)+ v_1(x)e^{iαy}]$, where $χ_a(x):=1$ for $x\in[0,a]$, $χ_a(x):=0$ for $x\notin[0,a]$, $v_j(x)$ are real or complex-valued functions, $χ_a(x)v_0(x)$ is an exactly solvable scattering potential in one dimension, and $α$ is a positive real parameter.If $α$ exceeds the wavenumber $k$ of the incident wave, the scattered wave does not depend on the choice of $v_1(x)$. In particular, $v(x,y)$ is invisible if $v_0(x)=0$ and $k<α$. For $k>α$ and $v_1(x)\neq 0$, the scattered wave consists of a finite number of coherent plane-wave pairs $ψ_n^\pm$ with wavevector: $\mathbf{k}_n=(\pm\sqrt{k^2-(nα)^2},nα)$, where $n=0,1,2,\cdots<k/α$. This generalizes to the scattering of wavepackets and suggests means for generating quantum states with a quantized component of momentum and pairs of states with an entangled momentum. We examine a realization of these potentials in terms of certain optical slabs. If $k=Nα$ for some positive integer $N$, $ψ_N^\pm$ coalesce and their amplitude diverge. If $k$ exceeds $Nα$ slightly, $ψ_N^\pm$ have a much larger amplitude than $ψ_n^\pm$ with $n<N$. This marks a resonance effect that arises for the scattered waves whose wavevector makes a small angle with the faces of the slab.