Abstract

Dielectric Barrier Discharges (DBD) are widely used for atmospheric pressure plasma generation. The possibility of their adaptation in custom-made configurations makes them potential candidate to assist deposition processes. In fact, the increased need of high-quality thin films forces to improve the deposition techniques. New processes should be able to work in less constrained conditions such as atmospheric pressure rather than vacuum and to have faster deposition rates while respecting the same high quality of the deposited films. In this paper we present the development of a surface dielectric barrier discharge plasma reactor to assist an atmospheric spatial atomic layer deposition process. The reactor was fabricated with 3D printing and the plasma was generated by a surface dielectric barrier discharge powered by a microsecond pulsed high voltage power supply. The dissipated power was measured for different configurations, and thanks to the micro discharges imaging, it was observed that the thickness and the shape of the dielectric barrier influenced the micro discharges distribution on the dielectric surface. The plasma reactor exhaust gas was chemically analyzed by FTIR spectroscopy and micro gas chromatography. The ozone concentration was determined as function of frequency of the power supply.

Highlights

  • High quality thin films become the essential component in many technological applications such as photovoltaics and microelectronics

  • While Pons et al showed that increasing the thickness of the barrier by 50 % leads to a 40 % decrease in the dissipated power [[11]. This is consistent with our results showing 40 % less dissipated power when the thickness increases between DBD1 and DBD3

  • The reactor was designed to be compatible with our Spatial Atomic Layer Deposition (SALD) head

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Summary

Introduction

High quality thin films become the essential component in many technological applications such as photovoltaics and microelectronics. The conventional ALD is based on a time sequenced injection of precursors and co-reactants to the deposition zone. It enables an accurate control of the film growth. It requires time for pumping before every sequence leading to slow deposition rates [1, 2]. An atmospheric plasma can be integrated to the SALD as source of reactive species, such as ozone, replacing the co-reactants [4], [5] This process, so-called Plasma Enhanced Atmospheric Pressure SALD (PE-AP-SALD), permits more flexibility in processing conditions such as working at lower temperature (

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