Back to Search Start Over

Nucleation mechanism during WS2 plasma enhanced atomic layer deposition on amorphous Al2O3 and sapphire substrates.

Authors :
Groven, Benjamin
Mehta, Ankit Nalin
Bender, Hugo
Smets, Quentin
Meersschaut, Johan
Franquet, Alexis
Conard, Thierry
Nuytten, Thomas
Verdonck, Patrick
Vandervorst, Wilfried
Heyns, Marc
Radu, Iuliana
Caymax, Matty
Delabie, Annelies
Source :
Journal of Vacuum Science & Technology: Part A-Vacuums, Surfaces & Films; Jan2018, Vol. 36 Issue 1, p1-N.PAG, 11p
Publication Year :
2018

Abstract

The structure, crystallinity and properties of as-deposited two-dimensional (2D) transition metal dichalcogenides are determined by nucleation mechanisms in the deposition process. 2D materials grown by atomic layer deposition (ALD) in the absence of a template are polycrystalline or amorphous. Little is known about their nucleation mechanisms. Therefore, the nucleation behavior of WS<subscript>2</subscript> during plasma enhanced ALD from WF<subscript>6</subscript>, H<subscript>2</subscript> plasma and H<subscript>2</subscript>S at 300 °C is investigated on amorphous ALD Al<subscript>2</subscript>O<subscript>3</subscript> starting surface and on monocrystalline, bulk sapphire. Preferential interaction of the precursors with the Al<subscript>2</subscript>O<subscript>3</subscript> starting surface promotes fast closure of the WS<subscript>2</subscript> layer. The WS<subscript>2</subscript> layers are fully continuous at WS<subscript>2</subscript> content corresponding to only 1.2 WS<subscript>2</subscript> monolayers. On amorphous Al<subscript>2</subscript>O<subscript>3</subscript>, (0002) textured and polycrystalline WS<subscript>2</subscript> layers form with grain size of 5 to 20 nm due to high nucleation density (∼10<superscript>14</superscript> nuclei/cm<superscript>2</superscript>). The WS<subscript>2</subscript> growth mode changes from 2D (layer-by-layer) growth on the initial Al<subscript>2</subscript>O<subscript>3</subscript> surface to three-dimensional (Volmer-Weber) growth after WS<subscript>2</subscript> layer closure. Further growth proceeds from both WS<subscript>2</subscript> basal planes in register with the underlying WS<subscript>2</subscript> grain and from or over grain boundaries of the underlying WS<subscript>2</subscript> layer with different in-plane orientation. In contrast, on monocrystalline sapphire, WS<subscript>2</subscript> crystal grains can locally align along a preferred in-plane orientation. Epitaxial seeding occurs locally albeit a large portion of crystals remain randomly oriented, presumably due to the low deposition temperature. The WS<subscript>2</subscript> sheet resistance is 168 MΩμm, suggesting that charge transport in the WS<subscript>2</subscript> layers is limited by grain boundaries. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
07342101
Volume :
36
Issue :
1
Database :
Complementary Index
Journal :
Journal of Vacuum Science & Technology: Part A-Vacuums, Surfaces & Films
Publication Type :
Academic Journal
Accession number :
127069802
Full Text :
https://doi.org/10.1116/1.5003361