Journal
ACS APPLIED ELECTRONIC MATERIALS
Volume 4, Issue 12, Pages 5789-5798Publisher
AMER CHEMICAL SOC
DOI: 10.1021/acsaelm.2c00966
Keywords
topological insulators; Sb2Te3; sputtering; nanocrystallites; Seebeck coefficient; electrical resistivity; weak antilocalization
Funding
- Fundacao para a Ciencia e a Tecnologia (FCT)/MEC
- FEDER from NECL [PTDC/CTM-MAN/5414/2014, UID/CTM/50024/2019, NORTE-01-0145-FEDER-022096, UID/QUI/50006/2013-OCI/01/0145/FEDER/007265]
- FCT [PD/BD/141803/2018]
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This study investigates the structural, electrical, and thermal transport properties of ion beam sputtered Sb2Te3 thin films. The results show high resistivity and coexistence of n-type and p-type conduction in these films. Weak antilocalization peaks in magnetoconductance and magnetic localization length suggest the presence of a 2D conduction channel and features of a topological insulator surface state in these films at low temperatures.
Sb2Te3 is a topological insulator (TI) material that can be used in a wide range of applications from energy harvesting to Spin-Orbitronics. In this paper, the structural, electrical, and thermal transport properties of nanocrystalline ion beam sputtered Sb2Te3 thin films were studied. Films with thicknesses between 35 and 300 nm, with nanocrystallites of sizes 10-20 nm, have a high resistivity between 0.072 and 2.03 Omega cm at 300 K, increasing with cooling. The Seebeck coefficient demonstrates the coexistence of n-type and p-type conduction, the latter being more prominent at high temperatures and in thicker films. The morphological and transport properties reveal that the films are constituted by two layers having different majority charge carriers, with the electronic bulk conduction being described by two semiconductor layers conducting in parallel, one p-type at the surface and another n-type, each described by an activation energy-dependent conductivity. Besides these bulk contributions, weak antilocalization (WAL) cusps are observed in the magnetoconductance below 10 K and at low magnetic fields. Analysis of the WAL hints that there is one two-dimensional conduction channel open at low temperatures for the thinner films, whereas for the thicker film, this 2D conduction appears to be masked by the bulk channels. However, a magnetic localization length L Phi between 62 and 90 nm at 2 K is observed for all thin films. This behavior suggests that as the bulk activation energy conductions freeze out at low temperatures, the electrical conduction is carried by the supposed 2D state, which appears to have some of the features of a TI surface state. Through these measurements, we demonstrate that the type of dominant conduction can be controlled by the Sb2Te3 film thickness in these large area sputtered films, while the conduction at low temperatures appears to be dominated by a robust TI state.
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