Apr 24, 2024
8:30am - 8:45am
Room 344, Level 3, Summit
Kornelius Nielsch1,3,4,Jun Yang1,Dongho Shin1,Sebastian Lehmann1,Tobias Ritschel2,Jochen Geck2
IFW Dresden1,Institute of Solid State Physics, TUD2,Institute of Applied Physics, TUD3,Institute of Materials Science, TUD4
Kornelius Nielsch1,3,4,Jun Yang1,Dongho Shin1,Sebastian Lehmann1,Tobias Ritschel2,Jochen Geck2
IFW Dresden1,Institute of Solid State Physics, TUD2,Institute of Applied Physics, TUD3,Institute of Materials Science, TUD4
Atomic layer deposition is a very versatile technology for the deposition of thin films with precise thickness control on large areas, non-planar surfaces and 3D objects. The chemical reaction is surface limited, well defined and works in most cases at low temperatures (RT to 150 °C). For a number of classical van der Waals 2D materials, there have been reports on ALD of transition metal dichalcogenide (TMDC) of MoS<sub>2</sub>, SnS<sub>2</sub>, WS<sub>2</sub> and WSe<sub>2</sub>, which also included the electronic characterization as a field effect transistor (FET).<br/><br/>In this work, we have fabricated by atomic layer deposition (ALD) multilayers of layered materials based on topological insulators and van der Waals materials, called <i>ferecrystals. </i>These ferecrystals can be tailored to exhibit unusual properties such as high electrical conductivity or low thermal conductivity or magnetic properties. A detailed ferecrystal study was performed on ferecrytals of Sb<sub>2</sub>Te<sub>3</sub> and SbO<sub>x</sub>, which has been grown at the same temperature as single layers of Sb<sub>2</sub>Te<sub>3</sub>. Without post-annealing, the electrical and thermoelectric characterisation of the highly ordered samples have been performed with the ZT-chip setup. In general, the carrier mobility is very high >150 Vs<sup>2</sup>/cm<sup>2</sup> and is even improved when the thickness of the Sb<sub>2</sub>Te<sub>3</sub> layers is reduced and the number of SbO<sub>x</sub> layers (typically 2 nm thickness) is increased. Detailed XRD investigations have been performed and an enhanced crystalline order is observed in the ferecrystal system compared to individual layers of Sb<sub>2</sub>Te<sub>3</sub>. We have grown ferecrystals based on Sb<sub>2</sub>Te<sub>3</sub> and Sb<sub>2</sub>Se<sub>3</sub> with tetrahedral and orthorhombic crystal structure, respectively. The p-type hole carrier concentration of Sb<sub>2</sub>Te<sub>3</sub> films can be enhanced through the sublayer doping of Sb<sub>2</sub>Se<sub>3</sub>. The highest carrier concentration achieved was 2.5×10<sup>19</sup> cm<sup>-2</sup> when the thickness ratio of Sb<sub>2</sub>Te<sub>3</sub> to Sb<sub>2</sub>Se<sub>3</sub> was (4 nm:2 nm). Further reduction of the Sb<sub>2</sub>Te<sub>3</sub> thickness resulted in a high Seebeck coefficient of 172 μV/K at room temperature.<br/><br/>Reference: Jun Yang, Samik Mukherjee, Sebastian Lehmann, Fabian Krahl, Xiaoyu Wang, Pavel Potapov, Axel Lubk, Tobias Ritschel, Jochen Geck, Kornelius Nielsch, "Low-Temperature ALD of SbO<i><sub>x</sub></i>/Sb<sub>2</sub>Te<sub>3</sub> Multilayers with Boosted Thermoelectric Performance", Small 20, 2306350 (2024) https://doi.org/10.1002/smll.202306350