It appears you don't have support to open PDFs in this web browser. To view this file, Open with your PDF reader
Abstract
Topological insulators (TIs) can host an insulating gapped bulk with conducting gapless boundary states in lower dimensions than the bulk. To date, various kinds of classical wave TIs with gapless symmetry-protected boundary states have been discovered, promising for the efficient confinement and robust guiding of waves. However, for airborne sound, an acoustic analogue of a three-dimensional TI has not been achieved due to its spinless nature. Here, we experimentally demonstrate a three-dimensional topological acoustic crystal with pseudospins using bilayer chiral structures, in which multi-order topological bandgaps are generated step by step via elaborately manipulating the corresponding spatial symmetries. We observe acoustic analogues of 1st-order (two-dimensional gapless surface Dirac cones) and 2nd-order (one-dimensional gapless hinge Dirac dispersion) TIs in three dimensions, supporting robust surface or hinge sound transport. Based solely on spatial symmetry, our work provides a route to engineer the hierarchies of TIs and explore topological devices for three-dimensional spinless systems.
An acoustic analogue of a three-dimensional topological insulator (TI) has not been achieved, despite various realizations in other kinds of TIs. Here, the authors report a three-dimensional multi-order TI in an acoustic bilayer chiral structure, with robust surface or hinge sound transport.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Details


1 Nanjing University, National Laboratory of Solid State Microstructures & Department of Materials Science and Engineering, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X); Nanjing University, Collaborative Innovation Center of Advanced Microstructures, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
2 Nanjing University, National Laboratory of Solid State Microstructures & Department of Materials Science and Engineering, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
3 Nanjing University, National Laboratory of Solid State Microstructures & Department of Materials Science and Engineering, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X); Nanjing University, Collaborative Innovation Center of Advanced Microstructures, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X); Nanjing University, Jiangsu Key Laboratory of Artificial Functional Materials, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)