Materials for Information Technology: Devices, Interconnects by Ehrenfried Zschech (Editor), Caroline Whelan (Editor),

By Ehrenfried Zschech (Editor), Caroline Whelan (Editor), Thomas Mikolajick (Editor)

This publication offers an up-to-the-minute survey of the cutting-edge of study into the fabrics utilized in details expertise, and should be obtained via researchers in universities, associations in addition to learn staff within the semiconductor and IT industries.

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Most IMD surfaces have a low reactivity (reactive site density) and island-type growth is observed. To guarantee the barrier property of the ALD film, at least a continuous layer on top of the substrate is required. The amount of ALD TiN (TiCl4/NH3) required to cover the starting surface is larger than a monolayer of the expected material (Figure 4) as was found in a study using Rutherford backscattering spectroscopy (RBS) to determine the amount of deposited layers, and time-of-flight secondary ion mass spectrometry (ToF-SIMS) – for which the depth information is limited to 1–3 monolayers (<10 Å) – to determine the coverage of the substrate [17].

A decreased resistivity and low chlorine content as compared to the binary TiCl4/NH3 system has been found. Another example for ternary barrier films is TiSixNy, which consists of titanium silicon nitride material. When silane (SiH4) and NH3 were dosed together the growth-per-cycle and composition was strongly dependent on the SiH4/NH3 ratio. The growth-per-cycle decreased with increasing silicon content. 2 Å was obtained. Compared to thermal processing techniques, the activation energy of the chemisorption, ligand exchange, and redox reactions are more readily overcome in plasma-enhanced ALD (PEALD) in which the non-metal precursor is activated by a plasma source.

Phys. 94, 3403 (2003), and M. L. -Y. Ho, B. Busch, G. D. Wilk, T. , J. Appl. Phys. 92, 7168 (2002) 22. A. Satta, A. Vantomme, J. Schuhmacher, C. M. Whelan, V. Sutcliffe, and K. Maex, Appl. Phys. Lett. 84, 4571 (2004) 23. G. Scarel, C. Wiemer, S. Ferrari, G. Tallarida, and M. Fanciulli, Proc. Estonian Acad. Sci. Phys. Math. 52, 308 (2003), and G. Scarel, S. Ferrari, S. Spiga, G. Tallarida, C. Wiemer, and M. Fanciulli, J. Vac. Sci. Technol. A 21, 1359 (2003) 24. G. Scarel, S. Spiga, C. Wiemer, G.

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