2020
DOI: 10.1038/s41563-020-0641-8
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Fermionic time-reversal symmetry in a photonic topological insulator

Abstract: Much of the recent enthusiasm directed towards topological insulators [1][2][3][4][5][6][7][8][9][10][11][12][13] as a new state of matter is motivated by their hallmark feature of protected chiral edge states. In fermionic systems, Kramers degeneracy gives rise to these entities in the presence of time-reversal symmetry (TRS) [1-3, 14, 15]. In contrast, bosonic systems obeying TRS are generally assumed to be fundamentally precluded from supporting edge states [3,16]. In this work, we dispel this perception an… Show more

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Cited by 46 publications
(42 citation statements)
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“…Ref. [37] documents the photonic lattice implementation of the driving protocol with fermionic time-reversal symmetry, and reports the observation of a topological phase with scatter-free counterpropagating boundary states. These states are protected by the fermionic time-reversal symmetry prescribed by the protocol, even though the underlying photonic system is of bosonic nature.…”
Section: Discussionmentioning
confidence: 99%
“…Ref. [37] documents the photonic lattice implementation of the driving protocol with fermionic time-reversal symmetry, and reports the observation of a topological phase with scatter-free counterpropagating boundary states. These states are protected by the fermionic time-reversal symmetry prescribed by the protocol, even though the underlying photonic system is of bosonic nature.…”
Section: Discussionmentioning
confidence: 99%
“…[125][126][127] WG photonic lattices are frequently adopted to build photonic topological structures for investigating the interplay of topology and interparticle interactions. [128][129][130][131] For example, the helicity of the evanescently coupled helical WG array would break the z-reversal symmetry in a honeycomb photonic lattice [Figs. 10(a) and 10(b)], which leads to formation of Floquet topological insulators, and topologically protected transport of visible light is observed on the lattice edges.…”
Section: Topological Physics and Quantum Information Processingmentioning
confidence: 99%
“…In our model, we add a second honeycomb layer on which an inverse copy of the driving protocol is implemented, similiar to the procedure in references [10,33]. The two layers (indicated by red circles and blue diamonds in Fig.…”
Section: Stacked Honeycomb Modelmentioning
confidence: 99%
“…In total, one period T in our model cycles through five time steps of equal length T /5 with pairwise coupling in each step. This precise control over the couplings becomes possible in photonic waveguides [10,14,15].…”
Section: Stacked Honeycomb Modelmentioning
confidence: 99%
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