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Interacting Surface States of Three-Dimensional Topological Insulators
Titus Neupert1, Stephan Rachel2, Ronny Thomale3
1Princeton Center for Theoretical Science, Princeton University, Princeton, New Jersey 08544, USA.
We numerically investigated strong topological insulators with electron-electron interactions. We found superconducting and anomalous Hall phases, along with unique boundary modes, offering insights into topological surface states.
Area of Science:
- Condensed Matter Physics
- Topological Materials Science
- Quantum Phenomena
Background:
- Strong topological insulators exhibit unique surface states protected by time-reversal symmetry.
- Electron-electron interactions can significantly alter the properties of topological surface states.
- Understanding these interactions is crucial for realizing novel quantum phenomena.
Purpose of the Study:
- To numerically investigate the impact of strong electron-electron interactions on the surface states of a strong topological insulator.
- To explore the emergence of exotic phases and boundary modes in a spherical topological insulator model.
- To provide a framework for stabilizing topologically ordered surface terminations.
Main Methods:
- Numerical investigation of a spherical topological insulator geometry.
- Mapping the single-particle problem to Landau orbitals with a central magnetic monopole.
- Assuming density-density contact interactions (attractive and repulsive).
Main Results:
- Identification of superconducting and anomalous (quantum) Hall phases for attractive and repulsive interactions, respectively.
- Discovery of chiral fermion and chiral Majorana fermion boundary modes between different phases.
- Demonstration of a spherical geometry suitable for finite-size analysis of surface states.
Conclusions:
- Electron-electron interactions drive rich phase transitions in topological insulator surface states.
- The proposed model system is well-suited for studying topologically ordered surface terminations.
- Tailored surface interactions could microscopically stabilize desired topological phases.
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