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Controlling Stoichiometry in Ultrathin van der Waals Films: PtTe<sub>2</sub>, Pt<sub>2</sub>Te<sub>3</sub>, Pt<sub>3</sub>Te<sub>4</sub>, and Pt<sub>2</sub>Te<sub>2</sub>

17

Citations

31

References

2022

Year

Abstract

The platinum-tellurium phase diagram exhibits various (meta)stable van der Waals (vdW) materials that can be constructed by stacking PtTe<sub>2</sub> and Pt<sub>2</sub>Te<sub>2</sub> layers. Monophase PtTe<sub>2</sub>, being the thermodynamically most stable compound, can readily be grown as thin films. Obtaining the other phases (Pt<sub>2</sub>Te<sub>3</sub>, Pt<sub>3</sub>Te<sub>4</sub>, Pt<sub>2</sub>Te<sub>2</sub>), especially in their ultimate thin form, is significantly more challenging. We show that PtTe<sub>2</sub> thin films can be transformed by vacuum annealing-induced Te-loss into Pt<sub>3</sub>Te<sub>4</sub>- and Pt<sub>2</sub>Te<sub>2</sub>-bilayers. These transformations are characterized by scanning tunneling microscopy and X-ray and angle resolved photoemission spectroscopy. Once Pt<sub>3</sub>Te<sub>4</sub> is formed, it is thermally stable up to 350°C. To transform Pt<sub>3</sub>Te<sub>4</sub> into Pt<sub>2</sub>Te<sub>2</sub>, a higher annealing temperature of 400°C is required. The experiments combined with density functional theory calculations provide insights into these transformation mechanisms and show that a combination of the thermodynamic preference of Pt<sub>3</sub>Te<sub>4</sub> over a phase segregation into PtTe<sub>2</sub> and Pt<sub>2</sub>Te<sub>2</sub> and an increase in the Te-vacancy formation energy for Pt<sub>3</sub>Te<sub>4</sub> compared to the starting PtTe<sub>2</sub> material is critical to stabilize the Pt<sub>3</sub>Te<sub>4</sub> bilayer. To desorb more tellurium from Pt<sub>3</sub>Te<sub>4</sub> and transform the material into Pt<sub>2</sub>Te<sub>2</sub>, a higher Te-vacancy formation energy has to be overcome by raising the temperature. Interestingly, bilayer Pt<sub>2</sub>Te<sub>2</sub> can be retellurized by exposure to Te-vapor. This causes the selective transformation of the topmost Pt<sub>2</sub>Te<sub>2</sub> layer into two layers of PtTe<sub>2</sub>, and consequently the synthesis of e Pt<sub>2</sub>Te<sub>3</sub>. Thus, all known Pt-telluride vdW compounds can be obtained in their ultrathin form by carefully controlling the stoichiometry of the material.

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