Flatband Line States in Photonic Super‐Honeycomb Lattices. Issue 11 (30th March 2020)

• Record Type: Journal Article
• Authors: Yan, Wenchao; Zhong, Hua; Song, Daohong; Zhang, Yiqi; Xia, Shiqi; Tang, Liqin; Leykam, Daniel; Chen, Zhigang
• Is Part Of: Advanced optical materials. Volume 8:Issue 11(2020)
• Page Start: n/a
• Page End: n/a
• Publication Date: 2020-03-30
• Subjects: flatband states -- laser‐writing arrays -- photonic Dirac materials -- real‐space topology -- super‐honeycomb lattices; Optical materials -- Periodicals; Photonics -- Periodicals; 620.11295
• DOI: 10.1002/adom.201902174
• Languages: English
• ISSNs: 2195-1071

Abstract

Abstract: For the first time, a photonic super‐honeycomb lattice (sHCL) is established experimentally by use of a continuous‐wave laser writing technique, and thereby two distinct flatband line states that manifest as noncontractible loop states in an infinite flatband lattice are demonstrated. These localized states ("straight" and "zigzag" lines) observed in the sHCL with tailored boundaries cannot be obtained by the superposition of conventional compact localized states because they arise from real‐space topological property of certain flatband systems. In fact, the zigzag‐line states, unique to the sHCL, are in contradistinction with those previously observed in the Kagome and Lieb lattices. Their momentum‐space spectrum emerges in the high‐order Brillouin zone where the flatband touches the dispersive bands, revealing the characteristic of topologically protected band‐touching. The experimental results are corroborated by numerical simulations. This work may provide insight into Dirac‐like 2D materials beyond graphene. Abstract : A photonic super‐honeycomb lattice is established by employing a continuous‐wave laser writing technique for the first time, and thereby two distinct flatband line states ("straight" and "zigzag" lines) are experimentally demonstrated in such a lattice with tailored boundaries. These line states cannot be obtained by superposition of conventional compact localized states because they arise from nontrivial real‐space topology of the flatband lattices.