Examines the influence of surface roughness on electrical resistivity in epitaxial films, indicating significant resistivity penalties.
The effect of atomic-scale surface roughness on electron transport is investigated using 6.5 nm-thick epitaxial Ru(0001) films, a promising metal for next-generation interconnects. Sputter deposition at 350 °C followed by stepwise vacuum annealing to 950 °C yields atomically smooth Ru(0001)/Al2O3(0001) films which are subsequently roughened by depositing ΘRu = 0.5, 1.0, and 2.0 monolayers (MLs) of additional Ru at room temperature. In situ four-point probe measurements show a resistivity ρ = 9.08–9.44 μΩ cm for 6.5 nm-thick films and a 4%–6% increase in sheet resistance upon roughening, attributed to electron scattering at atomic-height surface steps. The measured resistivity penalty Δρr = 0.41 μΩ cm caused by a ΘRu = 0.5 ML coverage suggests formation of 2D islands with an average step-edge separation ls = 2.7 nm, as quantified by a step-edge scattering model. This is in good agreement with ls = 3.6 ± 0.3 nm estimated from atomic force micrographs. Increasing ΘRu further to 1.0 ML causes a slight decrease in roughness and Δρr, indicating coalescence of 2D islands which increases ls to 3.0 nm. However, a ΘRu = 2.0 ML coverage causes 3D mound formation, an increased resistivity penalty Δρr = 0.49 μΩ cm, and a reduced ls = 2.3 nm, consistent with a significant damping of Kiessig fringes measured by x-ray reflectivity. These results demonstrate that atomic-scale topographical variations impose significant resistivity penalties for deeply scaled metallic interconnects.
No takes yet. Share an insight, caveat, or question.
Nishat et al. (2026) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: