AVS 64th International Symposium & Exhibition
    Thin Films Division Tuesday Sessions
       Session TF-TuM

Paper TF-TuM3
Employing Atmospheric Pressure Micro-Plasma Printer for ALD of TiO2 Thin Films

Tuesday, October 31, 2017, 8:40 am, Room 20

Session: Advanced CVD and ALD Processing, ALD Manufacturing and Spatial-ALD
Presenter: Morteza Aghaee, Eindhoven University of Technology, The Netherlands
Authors: M. Aghaee, Eindhoven University of Technology, The Netherlands
J. Verheijen, Eindhoven University of Technology, The Netherlands
A. Stevens, InnoPhysics B.V., The Netherlands
W.M.M. Kessels, Eindhoven University of Technology, The Netherlands
M. Creatore, Eindhoven University of Technology, The Netherlands
Correspondent: Click to Email

A broad range of devices such as thin film transistors (TFTs), solar cells, sensors and microfluidic channels benefit from micron-scale patterns in their structure. These micron-scale patterns are often fabricated by means of costly methods such as (photo-)lithography. For this reason, there is a large interest in alternative simple and cost-effective approaches for micron-scale to sub-millimeter patterning that reduce the number of etch and lithography process steps.

A micro-plasma printer [1], which is based on a unique needle-to-plate micro-plasma dielectric barrier discharge (DBD), has recently been developed for spatially-resolved surface functionalization [2] and deposition of organic films [3] with sub-millimeter range resolution. In this contribution, the potential of the micro-plasma printer in delivering patterned, ultra-thin inorganic films at atmospheric pressure is addressed. Specifically, the setup is adopted to carry out thin film TiO2 deposition in two configurations, namely plasma enhanced chemical vapor deposition (PE-CVD) and plasma-assisted atomic layer deposition (PA-ALD).

The properties of the TiO2 layers as well as the patterning resolution have been investigated. The TiO2 films deposited by PE-CVD mode have not shown satisfactory results in terms of purity and density of the layers (more than 5% C and refractive index of 1.8). However, the PA-ALD mode has been able to deliver patterns of amorphous TiO2 films with low level of impurity and sub-nanometer thickness control. A growth rate of 0.15 nm/cycle has been obtained for 500 ms and 400 µs of TTIP and N2/O2 plasma exposures in each PA-ALD cycle, respectively. Rutherford backscattering spectroscopy (RBS) has revealed a growth rate of 2.4 Ti atoms per nm2.cycle in saturation condition. Improvement of density and reduction of film impurities (H, C and N content) have been observed by prolonging the plasma exposure time. TiO2 films with refractive index of 2 and less than 1% C have been deposited by 2 ms of plasma exposure. The width of the smallest features deposited by PE-CVD and PA-ALD modes have been determined by XPS line scan measurements to be 1.8 mm and 900 µm, respectively, for 7 nm thick layers.


[1] T. Huiskamp, W. J. M. Brok, A. A. E. Stevens, E. J. M. van Heesch, and A. J. M. Pemen, IEEE TRANSACTIONS ON PLASMA SCIENCE, 40 (2012) 1913-1925.

[2] A. Mameli, Y. Kuang, M. Aghaee, C. K. Ande, B. Karasulu, M. Creatore, A. J. M. Mackus, W. E. M. M. Kessels, and F. Roozeboom , Chemistry of Materials, 29 (2017) 921-925.

[3] J.R.G Schalken, M. Creatore, P. Verhoven, A. Stevens, Nanoscience Nanotechnol. Letter, 7 (2015) 62-66.