Abstract

We find that a five-phase (substrate, mixed native oxide and roughness interface layer, metal oxide thin film layer, surface ligand layer, ambient) model with two-dynamic (metal oxide thin film layer thickness and surface ligand layer void fraction) parameters (dynamic dual box model) is sufficient to explain in-situ spectroscopic ellipsometry data measured within and across multiple cycles during plasma-enhanced atomic layer deposition of metal oxide thin films. We demonstrate our dynamic dual box model for analysis of in-situ spectroscopic ellipsometry data in the photon energy range of 0.7–3.4 eV measured with time resolution of few seconds over large numbers of cycles during the growth of titanium oxide (TiO2) and tungsten oxide (WO3) thin films, as examples. We observe cyclic surface roughening with fast kinetics and subsequent roughness reduction with slow kinetics, upon cyclic exposure to precursor materials, leading to oscillations of the metal thin film thickness with small but positive growth per cycle. We explain the cyclic surface roughening by precursor-surface interactions leading to defect creation, and subsequent surface restructuring. Atomic force microscopic images before and after growth, x-ray photoelectron spectroscopy, and x-ray diffraction investigations confirm structural and chemical properties of our thin films. Our proposed dynamic dual box model may be generally applicable to monitor and control metal oxide growth in atomic layer deposition, and we include data for SiO2 and Al2O3 as further examples.

Highlights

  • We find that a five-phase model with two-dynamic parameters is sufficient to explain in-situ spectroscopic ellipsometry data measured within and across multiple cycles during plasma-enhanced atomic layer deposition of metal oxide thin films

  • We report on the use of in-situ spectroscopic ellipsometry (SE) with few-second time resolution to investigate the evolution of Transition metal oxides (TMOs) thin film properties during Atomic layer deposition (ALD) growth processes

  • In-situ SE permits the time-dependent observation of precursor-surface interactions in Plasma-enhanced ALD (PEALD) of TMO thin films, with the capability to resolve the evolution of layer thickness and surface roughness during separate steps of individual cycles

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Summary

Introduction

We find that a five-phase (substrate, mixed native oxide and roughness interface layer, metal oxide thin film layer, surface ligand layer, ambient) model with two-dynamic (metal oxide thin film layer thickness and surface ligand layer void fraction) parameters (dynamic dual box model) is sufficient to explain in-situ spectroscopic ellipsometry data measured within and across multiple cycles during plasma-enhanced atomic layer deposition of metal oxide thin films. Klaus et al suggested the application of in-situ SE during ALD growth processes[64], and accurate thickness monitoring was reported for metal nitride thin films[41,65,66] and metal oxide thin films[46,67,68,69,70,71,72,73,74,75,76,77], for example. We discuss a five-phase (substrate, mixed native oxide and roughness interface layer, metal oxide thin film layer, surface ligand layer, ambient) model with two-dynamic (metal oxide thin film layer thickness and surface ligand layer void fraction) parameters (dynamic dual box model) We use this model and explain the in-situ SE data measured within and in between multiple cycles. We suggest use of our dual dynamic box model for unraveling surface modifications during atomic layer deposition processes leading to novel compounds such as Sb2Te3, perovskite SnTiO3, and potentially for nitrides such as AlNi and TiN80–82

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