Confinement‐Induced Phonon Softening and Hardening in Sb 2 Te 3 Thin Films
Abstract Scaling effects in Sesqui‐chalcogenides are of major interest to understand and optimize their performance in heavily scaled applications, including topological insulators and phase‐change devices. A combined experimental and theoretical study is presented for molecular beam epitaxy‐grown f...
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Published in | Advanced functional materials Vol. 34; no. 1 |
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Main Authors | , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
01.01.2024
|
Online Access | Get full text |
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Summary: | Abstract
Scaling effects in Sesqui‐chalcogenides are of major interest to understand and optimize their performance in heavily scaled applications, including topological insulators and phase‐change devices. A combined experimental and theoretical study is presented for molecular beam epitaxy‐grown films of antimony‐telluride (Sb
2
Te
3
). Structural,vibrational, optical, and bonding properties upon varying confinement are studied for thicknesses ranging from 1.3 to 56 nm. In ultrathin films, the low‐frequency coherent phonons of A
1g
1
symmetry are softened compared to the bulk (64.5 cm
−1
at 1.3 nm compared to 68 cm
−1
at 55.8 nm). A concomitant increase of the high‐frequency A
1g
2
Raman mode is seen. X‐ray diffraction analyses unravel an accompanying out of plane stretch by 5%, mainly stemming from an increase in the Te‐Te gap. This conclusion is supported by density functional theory slab models, which reveal a significant dependency of chemical bonding on film thickness. Changes in atomic arrangement, vibrational frequencies, and bonding extend over a thickness range much larger than observed for other material classes. The finding of these unexpectedly pronounced thickness‐dependent effects in quasi‐2D material Sb
2
Te
3
allows tuning of the film properties with thickness. The results are discussed in the context of a novel bond‐type, characterized by a competition between electron localization and delocalization. |
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ISSN: | 1616-301X 1616-3028 |
DOI: | 10.1002/adfm.202307681 |