Dec 2, 2024
4:15pm - 4:30pm
Sheraton, Fifth Floor, The Fens
Jara Vliem1,Jesper Moes1,Pedro de Melo1,Thomas Wigmans1,Andrés Botello-Méndez1,Rafael Mendes1,Ella van Brenk1,Ingmar Swart1,Lucas Maisel Licerán2,Henk Stoof2,Christophe Delerue3,Zeila Zanolli1,Daniel Vanmaekelbergh1
Debye Institute for Nanomaterials Science1,Institute for Theoretical Physics and Center for Extreme Matter and Emergent Phenomena2,University of Lille3
Jara Vliem1,Jesper Moes1,Pedro de Melo1,Thomas Wigmans1,Andrés Botello-Méndez1,Rafael Mendes1,Ella van Brenk1,Ingmar Swart1,Lucas Maisel Licerán2,Henk Stoof2,Christophe Delerue3,Zeila Zanolli1,Daniel Vanmaekelbergh1
Debye Institute for Nanomaterials Science1,Institute for Theoretical Physics and Center for Extreme Matter and Emergent Phenomena2,University of Lille3
Nanoscale topological insulators, with bismuth selenide (Bi
2Se
3) being a prototypical example, exhibit intriguing physics due to the combination of topological properties and confinement effects. Three-dimensional Bi
2Se
3 is characterized by an insulating bulk with topologically protected quantum states at its surface. Interestingly, a reduction of the crystal thickness down to 1-6 quintuple layers (QLs) results in gapping of the surface states due to hybridization.
[1,2] Such two-dimensional crystals are predicted to host one-dimensional helical edge states,
[3,4] which can be characterized with cryogenic scanning tunneling spectroscopy (STS). To study the topological properties of 2D Bi
2Se
3, a synthesis method is required to produce nanoscale Bi
2Se
3 with controllable dimensions. By modifying the precursor reactivity in a hot injection synthesis, we were able to synthesize ultrathin, colloidally stable Bi
2Se
3 nanoplatelets (NPLs) with a well-defined lateral size and a thickness of 1-6 QLs. The improved size control and homogeneity of the Bi
2Se
3 nanocrystals enables us to measure the density of states of individual NPLs with STS. For crystals of 4-6 quintuple layers, we observe an 8 nm wide, one-dimensional state along the edge of the crystal
[5]. We use a low-energy continuum model and ab initio GW-Tight Binding theory to investigate the nature of this state.
1. Neupane, M.
et al. Observation of quantum-tunnelling-modulated spin texture in ultrathin topological insulator Bi
2Se
3 films.
Nature Communications 5, 3841 (2014).
2. Zhang, Y.
et al. Crossover of the three-dimensional topological insulator Bi
2Se
3 to the two-dimensional limit.
Nature Physics 6, 584-588 (2010).
3. Liu, C. X.
et al. Oscillatory crossover from two-dimensional to three-dimensional topological insulators.
Physical Review B 81, 041307(R) (2010).
4. Licerán, L. M., Koerhuis, S. J. H., Vanmaekelbergh, D., & Stoof, H. T. C. Topology of Bi
2Se
3 nanosheets.
Physical Review B 109 (2024).
5. Moes, Jesper R., et al. "Characterization of the Edge States in Colloidal Bi
2Se
3 Platelets."
Nano Letters 24.17, 5110-5116 (2024).