AVS 64th International Symposium & Exhibition | |
Surface Science Division | Thursday Sessions |
Session SS+AS+EM-ThA |
Session: | Semiconductor Surfaces |
Presenter: | Nicole Herbots, Cactus Materials |
Authors: | N. Herbots, Cactus Materials R. Islam, Cactus Materials |
Correspondent: | Click to Email |
Bonding two semiconductors surfaces such as Si and GaAs can increase performance in solar cell efficiency and high power electronics. In this work, the surface chemistry and topography of Si and GaAs are investigated to optimize the bonding of the pair. A new process called Nano-bonding™ [1,2 ] can nucleate cross-bonding molecules via electron exchange between two surfaces into a macroscopically continuous bonding “inter-phase” . The surfaces to be bonded are first chemically smoothed at the nano-scale and then terminated with matching “precursor phases”. When activated, these phases exchange electrons. In other words, one surface is prepared so that it interacts preferentially with electron acceptors while the other surface is prepared to preferentially interact with electron donors. Hence, the precursor phases must be stable in air at room temperature until the surfaces are put into contact in clean-room class 10/ISO2 conditions and at low temperature (< 180°C). To bring the two surfaces into uniform contact while activating electron exchange and cross-bonding reactions, isotropic steam pressurization is applied, hence the name "Wet" Nano-Bonding™ [1,2].
The precursor phases are optimized based on insights provided by the Van Oss theory, combined with characterization of composition via Ion Beam Analysis (IBA), with surface energies via Three Liquids Contact Angle Analysis (3LCAA) and with surface topography using Atomic force Microscopy. On smooth surfaces, the Van-Oss theory separates contributions to the total surface energy γT into molecular interactions γLW, and interactions with electrons donors γ+ and acceptors γ–. These can then be each extracted accurately from 3LCAA measurements [2] using multiple (>3) drops. NanoBonding™ is observed when surface pairs complement each other for electron exchange: one surface with high γ+ and the other with high γ– leads to the formation of molecular cross-bonds. However, IBA and 3LCAA characterization results show that this criteria is not sufficient. The total surface energies γT for both GaAs, and Si must be larger than 40 mJ/m2. This is due to the fact that the contribution of interactions with electron donors and acceptors needs to amount to at least 10-15% of γT, so that total surface interaction γT is not mostly controlled by molecular interactions γLW , but exhibits significant non-molecular interactions with both acceptors and donors. Only then can the dominance of interactions with acceptors on one surface and interaction with donors on the other surface promote NanoBonding™ effectively.
[1] Herbots N. et al. US Patent 9,018,077 (2015); 9,589,801 (2017).