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Using Disorder to Identify Bogoliubov Fermi-Surface States
Hanbit Oh1, Daniel F Agterberg2, Eun-Gook Moon1
1Department of Physics, Korea Advanced Institute of Science and Technology, Daejeon 305-701, Korea.
A novel method identifies superconducting states with Bogoliubov Fermi surfaces (BG-FS) by observing how physical properties change with disorder. A linear residual density of states at low disorder is a key indicator for BG-FS states.
Area of Science:
- Condensed Matter Physics
- Superconductivity
- Materials Science
Background:
- Identifying exotic superconducting states is crucial for understanding novel electronic phenomena.
- Distinguishing between different types of nodal superconducting states, particularly those with Bogoliubov quasiparticles, remains a challenge.
- The influence of disorder on electronic properties is a key factor in characterizing superconducting states.
Purpose of the Study:
- To propose a method for identifying superconducting states with a Bogoliubov Fermi surface (BG-FS).
- To establish a unique experimental signature for BG-FS states based on their response to disorder.
- To provide a framework for analyzing candidate BG-FS materials.
Main Methods:
- Theoretical analysis of physical quantities' dependence on disorder in superconducting states.
- Focus on the residual density of states at weak disorder as a distinguishing feature.
- Investigation of supercurrent stability and optical conductivity behavior.
Main Results:
- A linear dependence of the residual density of states on weak disorder uniquely identifies a BG-FS state.
- Demonstration of supercurrent stability against impurities in BG-FS states.
- Observation of Drude-like behavior in the optical conductivity of BG-FS states.
Conclusions:
- The dependence of physical quantities on disorder provides a robust method for identifying BG-FS states.
- The proposed signatures offer direct experimental probes for candidate materials.
- These findings are applicable to materials like Sr$_{2}$RuO$_{4}$, FeSe$_{1-x}$S$_{x}$, and UBe$_{13}$.
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