Abstract

Atomic layer etching (ALE), a cyclic process of surface modification and removal of the modified layer, is an emerging damage-less etching technology for semiconductor fabrication with a feature size of less than 10 nm. Among the plasma sources, inductively coupled plasma (ICP) can be a candidate for ALE, but there is a lack of research linking discharge physics to the ALE process. In this study, we comprehensively investigated the discharge physics of ICPs with a radio frequency (RF) bias and Ar/C4F6 mixture to be considered for the ALE process. Detailed studies on the discharge physics were conducted in each step of ALE (i.e., modification step, removal step) as well as the whole cycle as follows: (1) In the general ALE cycle, plasma properties dependent on the chamber geometry and the discharge mode of the ICP were analyzed; (2) in the modification step, a plasma instability with molecular gas was observed. The timescale for molecular gas removal was also investigated; (3) in the removal step, changes in plasma characteristics with the RF bias power were studied. Based on measurements of these plasma physical parameters, the discharge condition for ALE was optimized. ALE was performed on various thin films, including a-Si, poly c-Si, SiO2, and Si3N4. For each thin film, thicknesses of 0.5–2.0 nm were etched per cycle, as in quasi-ALE. Finally, ALE was performed on a patterned wafer, and the etch thickness of 0.6 nm per cycle and fine etch profile were obtained.

Highlights

  • We comprehensively investigated the discharge physics of inductively coupled plasma (ICP) with a radio frequency (RF) bias and Ar/C4F6 mixture to be considered for the atomic layer etching (ALE) process

  • We investigated discharge characteristics for optimization of ALE using ICP with RF bias in an Ar/C4F6 mixture

  • The discharge characteristics were comprehensively studied for (1) general requirement, (2) modification step, (3) removal step, and (4) a whole cycle of ALE, and through these investigations, RF-biased ICP proved to be suitable as an ALE source

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Summary

INTRODUCTION

To optimize the ALE process using ICP, external control parameters need to be set based on a fundamental understanding of discharge characteristics and plasma physics. Because the external parameters applied in each step are different, and the plasma parameters such as electron density, ion density, neutral density, electron temperature, ion energy, and plasma potential change precise process control is difficult without a sufficient understanding of the discharge characteristics in each step and the entire cycle. The ion energy distribution, plasma potential, ion density, and electron temperature are changed by the radio frequency (RF) bias power and frequency These are correlated with the etch results (such as etch thickness per cycle and etch profile) and semiconductor device quality (durability, leakage current, and on/off characteristic).

ALE mechanism
Reactive gases for ALE
Plasma sources for ALE
ICP source for ALE source
Radio frequency biased ICP
Discharge properties for ALE process
Plasma parameters in a cycle of ALE
Chamber wall conditioning
Base pressure effect on hard mask etch
ALE of silicon
ALE in dielectric materials
ALE in patterned wafer
Findings
CONCLUSIONS
Full Text
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