“…where x ∈ C d is the sample being imaged, m ∈ C d is a mask which represents the probe's incident illumination on (a portion of) the sample, • denotes the Hadamard (pointwise) product, S k is a shift operator, and D : C d → C d is a function that describes the diffraction of the probe radiation from the sample to the plane of the detector after possibly passing though, e.g, a lens. Prior work in the computational mathematics community related to ptychographic imaging has primarily focused on far-field 1 ptychography (FFP) in which D is the action of a discrete Fourier transform matrix (see, e.g., [10,11,12,13,14,15]) in (1). Here, in contrast, we consider the less well studied setting of near-field ptychography (NFP) which describes situations where the masked sample is too close to the detector to be well described by the FFP model.…”