By formally invoking the Wiener-Hopf method, we explicitly solve a one-dimensional, singular integral equation for the excitation of a slowly decaying electromagnetic wave, called surface plasmon-polariton (SPP), of small wavelength on a semiinfinite, flat conducting sheet irradiated by a plane wave in two spatial dimensions. This setting is germane to wave diffraction by edges of large sheets of single-layer graphene. Our analytical approach includes (i) formulation of a functional equation in the Fourier domain; (ii) evaluation of a split function, which is expressed by a contour integral and is a key ingredient of the Wiener-Hopf factorization; and (iii) extraction of the SPP as a simple-pole residue of a Fourier integral. Our analytical solution is in good agreement with a finite-element numerical computation.1 Here, we use the term "metamaterial" to mean any atomically thick, conducting material whose optical conductivity allows the generation of SPPs with sufficiently small wavelength; see (2) later. 2 The terms "conducting" and "resistive" sheet or half plane are used interchangeably. The "top Riemann sheet," which is invoked below for a particular branch of a multiple-valued function in the complex plane, should not be confused with the physical sheet causing wave diffraction. 3 The placement of the 1D Helmholtz operator, (d 2 /dx 2 ) + k 2 , outside the integral of (1) affords a kernel, K, that is (logarithmically) integrable through x = x ; cf. Pocklington's integral equation for wire antennas [9,10]. The problem can be stated in alternate forms, e.g., via direct application of the Fourier transform to a boundary value problem [11], which circumvents (1).