CuO/ZnO heterojunction on ITO glass, fabricated via electrodeposition, sputtering, and solar simulation
Fabricated a thin-film solar cell using Copper Oxide (CuO), electrodeposited as Cu₂O and annealed to CuO, as the p-type absorber and Zinc Oxide (ZnO) as the n-type emitter layer on a Indium Tin Oxide (ITO) glass substrate. The goal was to fabricate a CuO/ZnO heterojunction device, characterized at each fabrication step using AFM and SEM, with final IV measurements taken on a Keithley 2400 under both dark and illuminated conditions.
CuO's narrow bandgap makes it an effective light absorber; ZnO provides high electron mobility and optical transparency. While our ITO layer serves as a bottom contact.
AFM after Cu₂O deposition showed pronounced surface texturing. Some peaks appeared incomplete, likely due to inspecting the sample mid-deposition.
SEM was taken after each fabrication step to follow how the surface changed through the stack.
The electrodeposited Cu₂O formed a dense, continuous film of faceted, pyramid-shaped crystallites about 1–2 µm across, with no bare substrate visible across the 41.5 µm field of view. Sharply faceted grains like these are typical of Cu₂O deposited from an alkaline (pH 10) lactate bath, and the full coverage indicates uniform current density across the substrate.
Annealing converted the Cu₂O to CuO, and needle-like nanowires appeared across the surface. They were scattered over the film (left), grew densely out of a crack (center), and lined the film edge (right). Nanowire growth like this is common when copper oxides are thermally oxidized in air at around 400 °C, and is generally attributed to stress in the growing oxide. The clustering at cracks and edges fits that explanation, since those are points of high stress.
The sputtered ZnO formed a fine-grained coating over the CuO. In the right panel the faceted grains beneath are still visible, which shows that the thin ZnO follows the texture of the layer under it rather than smoothing it out. The left and middle panels also show a crack and loose surface debris. Defects like these can become shunt paths through the junction, which matches the low shunt resistance seen in the I-V measurements.
The thin aluminum layer, oxidized during the final anneal, did not form a continuous film. The underlying grains are still visible through it, and bright rounded nodules, from about 0.2 µm to over 1 µm across, sit on the surface either alone or in clusters. This suggests the aluminum gathered into droplet-like nodules rather than wetting the surface. The resulting incomplete coverage is a likely cause of the poor top contact.
In a failed deposition, the Cu₂O grew as separate islands instead of a continuous film. At low magnification (right), the islands are grouped in streaks with bare substrate between them. At 2 kx (center), they are rounded and beginning to merge. At 10 kx (left), each island turns out to be made of many small faceted crystals. A loose electrical contact during deposition is the likely cause: it made the current density uneven, so growth concentrated at a few spots instead of covering the substrate evenly.
Dark IV confirmed diode behavior. Under illumination, the curves suggested significant recombination losses consistent with the surface defects and non-uniform coverage visible in SEM. Shunt resistance was low, indicating leakage paths likely from the incomplete aluminum coverage and porous CuO layer.
Thermal oxidation at 1000°C with Arrhenius modeling using Deal-Grove theory. Characterized by AFM and SEM.
View project
Pipeline to convert nanoscale AFM surface scans into STL files and 3D-print physical models of surface structures.
View project