Hybrid Sputtering Approach for Reliable TOF-SIMS Depth Profiling of Inorganic-Organic Multilayer Films
Surface Analysis Spotlight: TOF-SIMS
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by Jacob Schmidt
Staff Scientist
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Inorganic–organic stacks are everywhere now: optics coatings, perovskite solar cells, OLEDs, fuel-cell membranes, and the failure modes live at the interfaces.
The problem: TOF-SIMS depth profiling of hybrid stacks is hard.
- Ar-GCIB is great for organics as it generates low molecular damage, preserving the molecular ions, but it sputters many inorganics painfully slowly.
- Monoatomic sputtering can remove inorganics well, but it can destroy molecular information in the organic layers.
This article shows a practical fix: co-sputtering with low-energy monoatomic cesium (Cs+) and an argon gas cluster beam (Ar-GCIB) to get reliable depth profiles through an inorganic overlayer without sacrificing the organic molecular information underneath.
Key takeaways:
- Low-energy Cs⁺ (0.5 keV) boosts sputter yield of the Al overlayer where Ar-GCIB struggles.
- Ar-GCIB preserves organic molecular ions, and when paired correctly, the spectra look essentially like Ar-GCIB-only conditions for the polymer sputtering.
- The example used in this paper was 40 nm Al on PC or PET films. Ar-GCIB alone couldn’t fully clear Al even after long sputtering, but the hybrid method removes Al and cleanly reaches the polymer layer.
- The authors achieved interface resolution (84–16% width of AlO⁻) of ~4.8 nm on AL/PC and ~2.0 nm on AL/PET under the optimized hybrid conditions.
This Cs+ / Ar-GCIB hybrid sputter approach is exactly what you want when device reliability depends on nanometer-scale chemistry at buried interfaces: high-sensitivity + depth resolution + practical sputter rates across hybrid materials without loss of molecular information.

Depth profiling results of 40 nm-thick AI films deposited on bulk PC substrates. (a) Sputtering with Ar-GCIB alone. (b) Cosputtering using Ar-GCIB and Cs+ under the optimized conditions.
To learn more, you can find the original paper at J. Vac. Sci. Technol. B 43, 064006 (2025); doi: 10.1116/6.0005000