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Published on: February 3, 2014
Orbital angular momentum and spectral flow in two-dimensional chiral superfluids
Yasuhiro Tada1, Wenxing Nie1,2, Masaki Oshikawa1
1Institute for Solid State Physics, The University of Tokyo, Kashiwa 277-8581, Japan.
Orbital angular momentum in chiral superfluids depends on the wave type and regime. The p+ip-wave superfluid shows consistent OAM, while higher-order chiral superfluids exhibit suppressed OAM in the BCS limit due to edge mode effects.
Area of Science:
- Condensed Matter Physics
- Quantum Fluids
- Superfluidity
Background:
- Two-dimensional chiral superfluids exhibit unique quantum properties.
- Orbital angular momentum (OAM) is a key characteristic of superfluids.
- Understanding OAM in different superfluid regimes is crucial for theoretical advancements.
Purpose of the Study:
- To investigate the orbital angular momentum (OAM) in two-dimensional chiral (p_{x}+ip_{y})^{ν}-wave superfluids.
- To analyze the OAM in both Bose-Einstein condensation and BCS limits.
- To elucidate the role of spectral asymmetry and spectral flow in determining OAM.
Main Methods:
- Utilizing spectral asymmetry and spectral flow calculations.
- Analyzing N fermions on a disk at zero temperature.
- Comparing p+ip-wave superfluids with higher-order chiral superfluids (ν≥2).
Main Results:
- In the Bose-Einstein condensation regime, OAM (L_{z}) is found to be νN/2 for any integer ν.
- In the BCS limit, p+ip-wave superfluids have OAM L_{z}=N/2.
- For chiral superfluids with ν≥2 in the BCS limit, OAM is suppressed to L_{z}=N×O(Δ_{0}/ϵ_{F})≪N.
Conclusions:
- The behavior of OAM in chiral superfluids differs significantly between the BEC and BCS regimes.
- Edge mode properties and depairing effects are responsible for the suppressed OAM in higher-order chiral superfluids within the BCS limit.
- This study highlights the nuanced dependence of superfluid properties on microscopic details and theoretical frameworks.
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