Direct thermal atomic layer deposition of high-<i>κ</i> dielectrics on monolayer MoS<sub>2</sub>: nucleation and growth

High dielectric constant (high-<i>κ</i>) materials must be successfully integrated with single-layer transition metal dichalcogenides for future nanoscale device technologies. With high carrier mobility and relatively strong visible light emission, monolayer molybdenum disulfide (1L MoS<sub>2</sub>) is a promising candidate for optoelectronic applications and is commonly synthesised <i>via</i> chemical vapour deposition (CVD) to enable large-area device production. The growth of uniform high-<i>κ</i> dielectrics on bulk materials is routinely achieved <i>via</i> thermal atomic layer deposition (ALD), but continuous deposition on MoS<sub>2</sub> is notoriously challenging due to the absence of dangling bonds on the basal plane. The resulting unique nucleation and growth characteristics of high-<i>κ</i> dielectrics on 1L MoS<sub>2</sub> are not fully understood, particularly on large-area CVD-1L MoS<sub>2</sub>. In this work, we investigate the nucleation and growth of aluminium oxide (Al<sub>2</sub>O<sub>3</sub>) and hafnium dioxide (HfO<sub>2</sub>) on CVD-1L MoS<sub>2</sub> films <i>via</i> direct thermal ALD at 200 °C. We vary the number of ALD cycles and monitor the morphology of the deposited high-<i>κ</i> layer <i>via</i> atomic force microscopy, observing ALD-Al<sub>2</sub>O<sub>3</sub> and ALD-HfO<sub>2</sub> films on CVD-1L MoS<sub>2</sub> to exhibit island features for all cycle numbers investigated (up to 200 cycles). We reveal the development of Al<sub>2</sub>O<sub>3</sub> on CVD-1L MoS<sub>2</sub> proceeds <i>via</i> a three-dimensional growth mode, and we estimate the vertical and lateral growth rates to be 0.09 ± 0.01 nm per cycle and 0.06 ± 0.01 nm per cycle, respectively. In contrast, we find direct ALD of HfO<sub>2</sub> on CVD-1L MoS<sub>2</sub> exhibits negligible lateral growth, with a vertical growth rate of 0.14 ± 0.01 nm per cycle. We also investigate the thickness-dependent effects of ALD-Al<sub>2</sub>O<sub>3</sub> and ALD-HfO<sub>2</sub> films on the Raman and photoluminescence character of CVD-1L MoS<sub>2</sub>, and quantify changes in electron density. Our growth study offers valuable insights into the nucleation and development of high-<i>κ</i> dielectric films on CVD-1L MoS<sub>2</sub>, enhancing the understanding of dielectric integration for MoS<sub>2</sub>-based devices.

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Journal
Nanoscale
Published
2025-01-01
DOI
https://doi.org/10.1039/d5nr01144b
Citations
1
Primary Topic
2D Materials and Applications
Type
article
Field-Weighted Citation Impact
0.52

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Direct thermal atomic layer deposition of high-κ dielectrics on monolayer MoS2: nucleation and growth

Brendan F. M. Healy, Nicholas E. Grant, Sophie L. Pain, John D. Murphy
1 citations
Nanoscale
2D Materials and Applications
0.52
article

Direct thermal atomic layer deposition of high-κ dielectrics on monolayer MoS2: nucleation and growth

Brendan F. M. Healy, Nicholas E. Grant, Sophie L. Pain, John D. Murphy
article en
1 citations

Abstract

High dielectric constant (high-<i>κ</i>) materials must be successfully integrated with single-layer transition metal dichalcogenides for future nanoscale device technologies. With high carrier mobility and relatively strong visible light emission, monolayer molybdenum disulfide (1L MoS<sub>2</sub>) is a promising candidate for optoelectronic applications and is commonly synthesised <i>via</i> chemical vapour deposition (CVD) to enable large-area device production. The growth of uniform high-<i>κ</i> dielectrics on bulk materials is routinely achieved <i>via</i> thermal atomic layer deposition (ALD), but continuous deposition on MoS<sub>2</sub> is notoriously challenging due to the absence of dangling bonds on the basal plane. The resulting unique nucleation and growth characteristics of high-<i>κ</i> dielectrics on 1L MoS<sub>2</sub> are not fully understood, particularly on large-area CVD-1L MoS<sub>2</sub>. In this work, we investigate the nucleation and growth of aluminium oxide (Al<sub>2</sub>O<sub>3</sub>) and hafnium dioxide (HfO<sub>2</sub>) on CVD-1L MoS<sub>2</sub> films <i>via</i> direct thermal ALD at 200 °C. We vary the number of ALD cycles and monitor the morphology of the deposited high-<i>κ</i> layer <i>via</i> atomic force microscopy, observing ALD-Al<sub>2</sub>O<sub>3</sub> and ALD-HfO<sub>2</sub> films on CVD-1L MoS<sub>2</sub> to exhibit island features for all cycle numbers investigated (up to 200 cycles). We reveal the development of Al<sub>2</sub>O<sub>3</sub> on CVD-1L MoS<sub>2</sub> proceeds <i>via</i> a three-dimensional growth mode, and we estimate the vertical and lateral growth rates to be 0.09 ± 0.01 nm per cycle and 0.06 ± 0.01 nm per cycle, respectively. In contrast, we find direct ALD of HfO<sub>2</sub> on CVD-1L MoS<sub>2</sub> exhibits negligible lateral growth, with a vertical growth rate of 0.14 ± 0.01 nm per cycle. We also investigate the thickness-dependent effects of ALD-Al<sub>2</sub>O<sub>3</sub> and ALD-HfO<sub>2</sub> films on the Raman and photoluminescence character of CVD-1L MoS<sub>2</sub>, and quantify changes in electron density. Our growth study offers valuable insights into the nucleation and development of high-<i>κ</i> dielectric films on CVD-1L MoS<sub>2</sub>, enhancing the understanding of dielectric integration for MoS<sub>2</sub>-based devices.

NanoscaleVol. 17(25)
University of Warwick (GB)
Royal Academy of Engineering, University of Warwick, Engineering and Physical Sciences Research Council
Openalex Percentile: Top 37%
2D Materials and Applications
0.52
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