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Visualizing a bosonic symmetry protected topological phase in an interacting fermion model

机译:在相互作用的费米子模型中可视化玻色子对称受保护的拓扑相

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Symmetry protected topological (SPT) phases in free fermion and interacting bosonic systems have been classified, but the physical phenomena of interacting fermionic SPT phases have not been fully explored. Here, employing large-scale quantum Monte Carlo simulation, we investigate the edge physics of a bilayer Kane-Mele-Hubbard model with zigzag ribbon geometry. Our unbiased numerical results show that the fermion edge modes are gapped out by interaction, while the bosonic edge modes remain gapless at the (1 + 1) d boundary, before the bulk quantum phase transition to a topologically trivial phase. Therefore, finite fermion gaps both in the bulk and on the edge, together with the robust gapless bosonic edge modes, prove that our system becomes an emergent bosonic SPT phase at low energy, which is directly observed in an interacting fermion lattice model.
机译:游离费米子和相互作用的玻色子系统中受对称保护的拓扑(SPT)相已被分类,但是相互作用的费米离子SPT相的物理现象尚未得到充分研究。在这里,采用大规模量子蒙特卡洛模拟,我们研究了带有锯齿形带状几何结构的双层Kane-Mele-Hubbard模型的边缘物理学。我们无偏的数值结果表明,费米子边缘模通过相互作用被隔开,而玻色子边缘模在(1 + 1)d边界处保持无间隙,直到体量子相过渡到拓扑无关紧要的相为止。因此,在主体和边缘上有限的费米子间隙,再加上健壮的无间隙玻色子边缘模式,证明了我们的系统在低能量下变成了新兴的玻色子SPT相,这可以在相互作用的费米子晶格模型中直接观察到。

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