next-generation environmental technologies for advanced harvesting of solar energy. The operating principles of DSCs are well documented: a photoanode (working electrode) is covered in mesoporous and nanocrystalline metal oxide (usually TiO 2 ), which is sensitized by a monolayer of dye molecules adsorbed via anchoring groups. [ 2 ] Upon photon absorption, the excited dyes inject an electron into the conduction band of the semiconducting TiO 2 , generating a potential difference with respect to this working electrode and a counter-electrode (a transparent conducting oxide, usually fl uorine-doped tin oxide FTO). Thus, the adsorbed electron is transported to the counter-electrode, i.e., initiating the electrical current in the solar cell. An electrolyte solution between these electrodes acts as a redox couple, taking the electron from the counter-electrode and passing it back to the dye in order to regenerate its ground state, thus completing the electrical circuit. The redox process is catalyzed by platinum, a thin fi lm of which is coated into the counter-electrode. Due to its slow recombination with electrons from TiO 2 , the redox couple typically employed is I − / I 3 − . However, it is worth noting that a Co (II/III) tris(bipyridyl) redox couple is gaining traction as an alternative, given that it has a higher redox potential ( E redox ≈ +0.535 V) compared to I − / I 3 − ( E redox ≈ +0.35 V) and it mitigates better against energy losses in the dye regeneration process. [ 1,3,4 ] As the most effi cient, and hence most commonly used dyes contain the expensive and relatively rare transition metal ruthenium, [ 5,6 ] metal-free organic dyes have become attractive candidates due to their low cost, high molar extinction coeffi cients, and inherent design fl exibility. [ 5,6 ] Most organic dyes are based on donor-(π-bridge)-acceptor ( D -π-A ) architectures, in which a π-conjugated system connects an electron-donating group ( D ) with an electron-accepting group ( A ). Upon photoexcitation, the resulting "push-pull" effect is characterized by anisotropic intramolecular charge transfer (ICT) from the donor to the acceptor, which facilitates electron injection into the semiconductor. Modifi cations to the three main components of the D -π-A architecture allow a fi ne-tuning of the magnitude of this "push-pull" effect, in terms of the molar extinction coeffi cient (ε), the maximum peak absorption wavelength (λ max peak ), tris(bipyridyl) suggests promise for these computationally designed dyes as co-sensitizers for DSC applications.