Abstract
Nanolaminates─atomically layered stacks of dissimilar oxides─are widely used to engineer dielectric behavior at the nanometer scale. Among these, atomic layer deposition (ALD)-grown Al2O3/TiO2 stacks have been reported to exhibit “giant” dielectric constant (κ ∼ 103) at subnanometer periods. Here we show that the apparent high-κ is not an intrinsic dielectric enhancement but a measurement artifact arising from electrically percolative Al2O3/TiO2 stacks treated as ideal dielectrics. Using Al2O3/TiO2 nanolaminate metal–insulator–metal (MIM) capacitors and a combination of electrical (C–f, I–V, EIS), spectroscopic (XPS, HAXPES), and structural (TEM) measurements, we found that TMA/H2O growth yields Al-deficient Al2O3 on TiO2 that appears morphologically continuous yet lacks full atomic closure, forming electronically percolative pathways that recover insulating behavior only after a fully coalesced overlayer develops. In contrast, TMA/O3 deposition produces fully continuous Al2O3 that remains insulating even at subnanometer thickness. These results establish practical design rules, showing that oxidant chemistry and film thickness together govern film continuity and insulating behavior, thereby clarifying when ultrathin ALD Al2O3 functions as a true insulator versus a quasi-conductive layer. The insights extend directly to applications in microelectronics (gate stacks, MIM/DRAM capacitors), quantum devices (2DEGs, tunnel barriers), and electrochemical/photovoltaic systems (battery electrodes, electrocatalysts, and perovskite interface engineering), where reliable subnanometer coatings are essential.
| Original language | English |
|---|---|
| Pages (from-to) | 68169-68178 |
| Number of pages | 10 |
| Journal | ACS Applied Materials and Interfaces |
| Volume | 17 |
| Issue number | 50 |
| DOIs | |
| State | Published - Dec 17 2025 |
Keywords
- AlO/TiOnanolaminate
- atomic layer deposition (ALD)
- HAXPES
- high-kdielectrics
- Maxwell−Wagner relaxation
- metal−insulator−metal (MIM) capacitors
- oxygen vacancies
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