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Topological crystalline superconductors in two dimensions.
1Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China.
Summary
We developed a framework to classify topological edge modes in 2D topological crystalline superconductors. This research identifies distinct Majorana and AIII class edge modes protected by crystalline symmetries.
Area of Science:
- Condensed Matter Physics
- Topological Materials
- Superconductivity
Background:
- Topological crystalline superconductors host exotic edge states protected by crystalline symmetries.
- Classifying these edge modes is crucial for understanding their properties and potential applications.
- Time-reversal symmetry plays a key role in the emergence of these topological phases.
Purpose of the Study:
- To propose a general framework for classifying topological edge modes in 2D topological crystalline superconductors.
- To investigate the realization of topological crystalline phases.
- To distinguish topological phases based on mirror and mirror-inversion symmetries.
Main Methods:
- Development of a theoretical framework for classifying topological edge modes.
- Analysis of superconductors with time-reversal and crystalline symmetries (mirror and mirror-inversion).
- Identification of criteria for distinguishing topological phases.
Main Results:
- A framework is established to classify topological edge modes protected by crystalline symmetries.
- Majorana edge modes are identified along mirror invariant lines in specific topological phases.
- AIII class topological edge modes are found along mirror-inversion invariant lines and in mirror-inversion parity subspaces.
Conclusions:
- The proposed framework successfully classifies topological edge modes in 2D topological crystalline superconductors.
- Distinctive topological edge modes, including Majorana and AIII class, are characterized by their symmetry protection.
- The study provides a criterion for distinguishing topological phases in crystalline superconductors with combined symmetries.
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