K. Avers, W. Gannon, A. Leishman, L. Debeer-Schmitt, W. Halperin, M. Eskildsen
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引用次数: 1
摘要
我们利用小角中子散射法确定了拓扑超导体UPt3在外加磁场作用下沿晶体c轴的涡点阵相图。在整个超导态中观察到一个三角形涡晶格,但其取向相对于六边形基底面,随场和温度的变化而变化。在低温下,在手性B相中,涡旋晶格随着磁场的增大而发生非单调旋转。旋转振幅随温度升高而减小,在到达A相之前消失。在A相中,Huxley等人在Nature 406, 160-164(2000)中报道了±15°旋涡晶格的突然旋转。复相图可以从超导序参量、对称破缺场和费米表面各向异性的竞争效应来理解。由Avers et al., Nature Physics 16, 531-535(2020)报道的以0.8 T为中心的低温旋转相位可以直接归因于对称破缺场。
Effects of the Order Parameter Anisotropy on the Vortex Lattice in UPt3
We have used small-angle neutron scattering to determine the vortex lattice phase diagram in the topological superconductor UPt3 for the applied magnetic field along the crystalline c-axis. A triangular vortex lattice is observed throughout the superconducting state, but with an orientation relative to the hexagonal basal plane that changes with field and temperature. At low temperature, in the chiral B phase, the vortex lattice undergoes a non-monotonic rotation with increasing magnetic field. The rotation amplitude decreases with increasing temperature and vanishes before reaching the A phase. Within the A phase an abrupt ±15° vortex lattice rotation was previously reported by Huxley et al., Nature 406, 160-164 (2000). The complex phase diagram may be understood from competing effects of the superconducting order parameter, the symmetry breaking field, and the Fermi surface anisotropy. The low-temperature rotated phase, centered around 0.8 T, reported by Avers et al., Nature Physics 16, 531-535 (2020), can be attributed directly to the symmetry breaking field.