IntroductionPolymer thin films are a highly specialized class of polymers on surfaces that range in thickness from several nanometers to micrometers. The chemical composition and conformation of the polymer chains at the surface can dictate interfacial properties such as adhesion, friction, wetting, and absorption of molecules from the environment. Ultimately, techniques that afford polymer coatings that are easily tunable provide the most versatility to develop a wide array of surfaces. Specialized surfaces such as arrays and sensors provide an insight into the development of small-scale sensors and devices for fields such as biomaterials science and nanotechnology [1][2][3][4][5][6][7].Polymeric thin films are attached to the surface in one of the two ways: through physical deposition of a thin film (physisorption) or by covalent attachment of the polymer chains to the surface (chemisorption). Weak intermolecular forces between the polymer thin film and the substrate govern surface modification by physisorption. Physisorption can lead to failure of the thin film under nonideal conditions by delamination, dewetting, desorption, and displacement [8]. In contrast, covalent attachment of a polymer thin film to the surface provides enhanced stability to polymer surface modification over physical absorption methods. Polymer brushes consist of macromolecular chains, in which covalent bonds tether the chains to the surface with a large grafting density to alter the unperturbed solution dimensions of the chains [9]. Films generated from polymer brushes exhibit unique surface phenomena that are advantageous in controlling physical properties such as wetting, phase segregation, absorption of molecules and macromolecules, lubrication, and diffusion control [7].These unique properties of polymer brushes are dictated by the extended conformation of the dense, ordered grafting on the surface. The polymer chains extend to balance the free energy associated with chain stretching and chain-solvent interactions. The entropic energy associated with a random walk configuration of the polymer chains favors short, low grafting density brushes. In contrast, a brush will extend to be energetically favorable in a highly solvated,