论文标题
铁电超导体中的Majorana-Weyl锥
Majorana-Weyl cones in ferroelectric superconductors
论文作者
论文摘要
预计拓扑超导体将表现出杰出的现象,包括非亚伯安人的激发,热携带边缘状态和Bogoliubov Spectra中的拓扑结节。尽管如此,尽管进行了重大的实验努力,但我们仍然缺乏这种异国情调现象的明确标志。在这种情况下,在轻度掺杂和超干净的srtio $ _3 $中,最近发现了共存的超导性和铁电性,这为新的机会打开了新的机会。确实,通往拓扑超导性的有希望的途径是强旋转轨道耦合和反转对称性断裂的结合。在这里,我们研究了带有Rashba自旋轨道耦合的三维抛物线带,其轴与铁电时矩的方向对齐。我们表明,当应用磁场时,在该模型中自然出现上述现象。在关键的Zeeman领域之上,Majorana-Weyl锥出现,无论电子密度如何。这些锥体表现出自我表现为Majorana Arcs状态出现在表面和四方域壁上。旋转磁场相对于铁电力矩的方向倾斜了Majorana-Weyl锥,最终将它们带入带有Bogoliubov Fermi表面的II型状态。然后,我们考虑轨道磁场的后果。首先,发现单个涡流被拓扑光环包围,其特征是两个Majorana零模式:一种位于涡流核心中,另一个位于拓扑晕圈的边界上。基于一个半经典论证,我们表明,将磁场提高到临界值以上时,光环重叠并最终通过系统渗透,从而导致始终先于正常状态之前的散装拓扑转换。最后,我们提出了具体实验来测试我们的预测。
Topological superconductors are predicted to exhibit outstanding phenomena, including non-abelian anyon excitations, heat-carrying edge states, and topological nodes in the Bogoliubov spectra. Nonetheless, and despite major experimental efforts, we are still lacking unambiguous signatures of such exotic phenomena. In this context, the recent discovery of coexisting superconductivity and ferroelectricity in lightly doped and ultra clean SrTiO$_3$ opens new opportunities. Indeed, a promising route to engineer topological superconductivity is the combination of strong spin-orbit coupling and inversion-symmetry breaking. Here we study a three-dimensional parabolic band minimum with Rashba spin-orbit coupling, whose axis is aligned by the direction of a ferroelectric moment. We show that all of the aforementioned phenomena naturally emerge in this model when a magnetic field is applied. Above a critical Zeeman field, Majorana-Weyl cones emerge regardless of the electronic density. These cones manifest themselves as Majorana arcs states appearing on surfaces and tetragonal domain walls. Rotating the magnetic field with respect to the direction of the ferroelectric moment tilts the Majorana-Weyl cones, eventually driving them into the type-II state with Bogoliubov Fermi surfaces. We then consider the consequences of the orbital magnetic field. First, the single vortex is found to be surrounded by a topological halo, and is characterized by two Majorana zero modes: One localized in the vortex core and the other on the boundary of the topological halo. Based on a semiclassical argument we show that upon increasing the field above a critical value the halos overlap and eventually percolate through the system, causing a bulk topological transition that always precedes the normal state. Finally, we propose concrete experiments to test our predictions.