Exact solution of the two-dimensional scattering problem for a class of delta-function potentials supported on subsets of a line

We use the transfer matrix formulation of scattering theory in two-dimensions (2D) to treat the scattering problem for a potential of the form v{x,y) = ? delta(ax + by)g{bx - ay) where ?, a, and b are constants, delta(X) is the Dirac delta function, and g is a real- or complex-valued function. We map this problem to that of v{x,y) = ? delta(x)g(y) and give its exact (nonapproximate) and analytic (closed-form) solution for the following choices of g(y): (i) a linear combination of delta 5 functions, in which case v(x,y) is a finite linear array of 2D delta functions; (ii) a linear combination of e(i alpha)n(y) with alpha(n) real; (iii) a general periodic function that has the form of a complex Fourier series. In particular we solve the scattering problem for a potential consisting of an infinite linear periodic array of 2D delta functions. We also prove a general theorem that gives a sufficient condition for different choices of g(y) to produce the same scattering amplitude within specific ranges of values of the wavelength lambda. For example, we show that for arbitrary real and complex parameters, a and z, the potentials z Sigma n=-infinity(infinity) delta(x)delta(y - an) a(-1z delta(x))[l + 2cos(2 pi/a)] have the same scattering amplitude for a < lambda (3) 2a.