Influence of Magnetic Field on Surface Andreev Bound States in Superfluid He-B Studied by Mobility of Electron Bubble
arXiv:2412.08839 · doi:10.1007/s10909-024-03255-2
Abstract
The B phase of superfluid He (He-B) is topologically nontrivial and the surface Andreev bound states formed on a surface are conceived as Majorana fermions. In a magnetic field, the surface Andreev bound states acquire a Zeeman gap. How the Zeeman gap opens when a magnetic field is applied is intimately related to how the topological properties are lost. In this article, we study the mobility of an electron bubble trapped under a free surface of He-B in a magnetic field of 0.25 T to examine the influence of the magnetic field on the surface Andreev bound states. We observe experimentally and theoretically that, with decreasing temperature, the mobility at 0.25 T increases steeper than that in zero magnetic field when the thermal energy is comparable to the Zeeman energy, while the mobility is slightly smaller than that in zero magnetic field at higher temperatures. These features are understood by the opening of the Zeeman gap, the resulting change in the density of states within the bulk superfluid gap, and the distortion of the bulk superfluid gap by the magnetic field.
References in corpus (8)
- Classification of topological insulators and superconductors in three spatial dimensions
- Symmetry Protected Topological Order and Spin Susceptibility in Superfluid 3He-B
- Surface Majorana Cone of the Superfluid He B Phase
- Surface Specific Heat of He and Andreev Bound States
- Symmetry Protected Topological Superfluid He-B
- Edge Current due to Majorana Fermions in Superfluid He A- and B-Phases
- Superfluid 3He in a restricted geometry with a perpendicular magnetic field
- Electron Bubbles in Superfluid He-A: Exploring the Quasiparticle-Ion Interaction