journal article·2022-04Open access

Direct Transition from Ultrathin Orthorhombic Dinickel Silicides to Epitaxial Nickel Disilicide Revealed by In Situ Synthesis and Analysis

Philipp M. Wolf, Eduardo Pitthan, Zhen Zhang, Christian Lavoie, Tuan T. Tran, Daniel Primetzhofer

Small· Volume 18· Issue 14

Abstract

Abstract Understanding phase transitions of ultrathin metal silicides is crucial for the development of nanoscale silicon devices. Here, the phase transition of ultrathin (3.6 nm) Ni silicides on Si(100) substrates is investigated using an in situ synthesis and characterization approach, supplemented with ex situ transmission electron microscopy and nano‐beam electron diffraction. First, an ultrathin epitaxial layer and ordered structures at the interface are observed upon room‐temperature deposition. At 290 °C, this structure is followed by formation of an orthorhombic δ‐Ni2Si phase exhibiting long‐range order and extending to the whole film thickness. An unprecedented direct transition from this δ‐Ni2Si phase to the final NiSi2−x phase is observed at 290 °C, skipping the intermediate monosilicide phase. Additionally, the NiSi2−x phase is found epitaxial on the substrate. This transition process substantially differs from observations for thicker films. Furthermore, considering previous studies, the long‐range ordered orthorhombic δ‐Ni2Si phase is suggested to occur regardless of the initial Ni thickness. The thickness of this ordered δ‐Ni2Si layer is, however, limited due to the competition of different orientations of the δ‐Ni2Si crystal. Whether the formed δ‐Ni2Si layer consumes all deposited nickel is expected to determine whether the monosilicide phase appears before the transition to the final NiSi2−x phase.
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Research context

OpenAlex topics: Semiconductor materials and interfaces · Semiconductor materials and devices · Surface and Thin Film Phenomena

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Department of Physics and Astronomy Ångström Laboratory Uppsala University Box 516 Uppsala SE‐751 20 Sweden

Solid State Electronics Department of Electrical Engineering The Ångström Laboratory Uppsala University Uppsala SE‐751 21 Sweden

IBM Thomas J. Watson Research Center Yorktown Heights New York 10598 USA

Funding

Vetenskapsrådet

References (32)

Show source-provided references
1. 10.1063/1.332309710.1063/1.3323097 ↗
2. 10.1126/science.124435810.1126/science.1244358 ↗
3. 10.1039/C7CS00828G10.1039/C7CS00828G ↗
4. 10.1039/c1nr10847f10.1039/c1nr10847f ↗
5. 10.1021/nl900779j10.1021/nl900779j ↗
6. 10.1016/S0167-9317(03)00380-010.1016/S0167-9317(03)00380-0 ↗
7. 10.1557/JMR.1986.020510.1557/JMR.1986.0205 ↗
8. 10.1063/1.366211010.1063/1.3662110 ↗
9. 10.1103/PhysRevLett.50.42910.1103/PhysRevLett.50.429 ↗
10. 10.1149/1.358061810.1149/1.3580618 ↗
11. 10.1149/2162-8777/ab74c210.1149/2162-8777/ab74c2 ↗
12. 10.1016/j.apsusc.2020.14778110.1016/j.apsusc.2020.147781 ↗
13. 10.1103/PhysRevLett.60.115810.1103/PhysRevLett.60.1158 ↗
14. 10.1103/PhysRevLett.75.272610.1103/PhysRevLett.75.2726 ↗
15. 10.1063/1.338499710.1063/1.3384997 ↗
16. 10.1016/0368-2048(74)80024-110.1016/0368-2048(74)80024-1 ↗
17. 10.1063/1.352945910.1063/1.3529459 ↗
18. 10.1149/1.139078110.1149/1.1390781 ↗
19. 10.1103/PhysRevA.68.02290110.1103/PhysRevA.68.022901 ↗
20. 10.1103/PhysRevA.100.03270510.1103/PhysRevA.100.032705 ↗
21. 10.1063/1.332745110.1063/1.3327451 ↗
22. 10.1038/s41598-020-66464-110.1038/s41598-020-66464-1 ↗
23. 10.1533/9780857096296.1.24410.1533/9780857096296.1.244 ↗
24. 10.1088/1361-6528/ab6d2110.1088/1361-6528/ab6d21 ↗
25. 10.1088/1361-6463/abb04610.1088/1361-6463/abb046 ↗
26. 10.1016/j.vacuum.2003.12.04110.1016/j.vacuum.2003.12.041 ↗
27. 10.1103/PhysRevLett.100.21320110.1103/PhysRevLett.100.213201 ↗
28. 10.1103/PhysRevB.80.12542510.1103/PhysRevB.80.125425 ↗
29. 10.1063/1.475019510.1063/1.4750195 ↗
30. 10.1016/j.nimb.2019.11.01910.1016/j.nimb.2019.11.019 ↗
31. 10.1016/j.nimb.2014.02.06310.1016/j.nimb.2014.02.063 ↗
32. Mayer M. · 1999 · 54110.1063/1.59188 ↗