论文标题
使用轨道诱导的合成通量的光子四极拓扑绝缘子
Photonic quadrupole topological insulator using orbital-induced synthetic flux
论文作者
论文摘要
通过原子轨道的潜在几何形状和连通性,在很大程度上确定了多型分子和晶体结构的丰富物理特性。这种轨道的自由度也已被有效地用于引入一些合成材料,包括北极星晶格非线性光子晶格和光学晶格中的超电原子。特别是,与奇偶校验的混合(例如$ s $和$ p $轨道)的混合被证明对于生成需要交替相位模式的系统特别有用,就像晶格内的耦合符号一样。在这里,我们表明,通过进一步打破这种混合轨道晶格的对称性,可以生成晶格的合成磁通螺纹。该功能允许在合成玻色子平台中生成多极的高阶拓扑阶段,其中$π$通量螺纹需要晶格的每个斑点,并且迄今为止仅使用量身定制的连接模式实现。我们使用这种见解来实验表明在波导的二维晶格中表现出四杆光子拓扑绝缘子,该晶格利用了$ s $和$ s $和$ p $ orbital型表示的模式。我们通过观察受保护的零维状态的存在,在空间上局限于角落,并确认这些状态位于带隙,从而证实了系统的非平凡四极拓扑。我们的方法还适用于不允许量身定制的连接性的更广泛的时间反向不变的合成材料,例如纳米级几何形状,其中合成通量至关重要。
The rich physical properties of multiatomic molecules and crystalline structures are determined, to a significant extent, by the underlying geometry and connectivity of atomic orbitals. This orbital degree of freedom has also been used effectively to introduce structural diversity in a few synthetic materials including polariton lattices nonlinear photonic lattices and ultracold atoms in optical lattices. In particular, the mixing of orbitals with distinct parity representations, such as $s$ and $p$ orbitals, has been shown to be especially useful for generating systems that require alternating phase patterns, as with the sign of couplings within a lattice. Here we show that by further breaking the symmetries of such mixed-orbital lattices, it is possible to generate synthetic magnetic flux threading the lattice. This capability allows the generation of multipole higher-order topological phases in synthetic bosonic platforms, in which $π$ flux threading each plaquette of the lattice is required, and which to date have only been implemented using tailored connectivity patterns. We use this insight to experimentally demonstrate a quadrupole photonic topological insulator in a two-dimensional lattice of waveguides that leverage modes with both $s$ and $p$ orbital-type representations. We confirm the nontrivial quadrupole topology of the system by observing the presence of protected zero-dimensional states, which are spatially confined to the corners, and by confirming that these states sit at the band gap. Our approach is also applicable to a broader range of time-reversal-invariant synthetic materials that do not allow for tailored connectivity, e.g. with nanoscale geometries, and in which synthetic fluxes are essential.