We propose a strong-coupling analysis of a polarizable planar interface, in the spirit of a recently introduced Wigner-Crystal formulation. The system is made up of two moieties: a semi-infinite medium (z < 0) with permittivity ε ′ while the other half space in z > 0 is occupied by a solution with permittivity ε, and mobile counter-ions (no added electrolyte). The interface at z = 0 bears a uniform surface charge. The counter-ion density profile is worked out explicitly for both repulsive and attractive dielectric image cases.Copyright line will be provided by the publisher Introduction. Strong coulombic couplings can conveniently be realized in colloidal systems by increasing the valence of micro-ions [1, 2, 3]. The counter-intuitive effects such as like-charge attraction or overcharging that ensue [1,2,3], have been mostly studied under the simplifying assumption that the dielectric permittivity of colloidal particles coincides with that of the surrounding solvent -assumed to be a structure-less medium, characterized by its sole static dielectric response. However, realistic systems, of biological interest in particular, often exhibit highly inhomogeneous dielectric structure, with polarizable colloids having a static dielectric constant (ε ′ ≤ 10), much smaller than that of the solvent (ε ≃ 80 for water). It is therefore desirable to include colloidal polarizability into existing strong-coupling treatments (see below for a precise definition of the relevant coupling parameter). This is the purpose of the present contribution.To our knowledge, the dielectric inhomogeneities were studied in the leading strong-coupling order only for the geometry of two parallel plates [4] where counter-ions are confined in a slab, and similarly in Ref. [5], for a spherical macro-ion in a concentric spherical Wigner-Seitz cell. It was realized that while the image charge effects are generally small in the weak-coupling regime, they become relevant in the strong-coupling limit. Our goal here is to obtain exact results for a single polarizable planar colloid (hatched region in Fig. 1), in the strong-coupling limit (see Fig. 1 for a definition of the coupling parameter Ξ). To this end, the Wigner-Crystal formulation of Strong-Coupling (SC) theory, recently introduced [6], is modified to account for dielectric image charges. We emphasize that this approach has been shown to be in excellent agreement with Monte Carlo simulations, in contrast to previous fugacity SC expansions [3]. The idea is to consider the first relevant large Ξ excitations around the ground state structure, that is a Wigner Crystal realized when, strictly speaking, Ξ → ∞ [6].