Symmetry-enforced three-dimension Dirac phononic crystals

Symmetry-enforced three-dimension Dirac phononic crystals
Schematics of the bcc unit (left panel) of the phononic crystal and its (010) surface (right panel) featured with two glide mirrors Gx and Gz. b, 3D bcc BZ and its (010) surface BZ. The coloured spheres highlight the bulk Dirac points with equal frequency and their projections onto the surface BZ. c, Bulk bands simulated along several high-symmetry directions. d, Schematic of the quad-helicoid surface state dispersions (colour surfaces), where the grey cone labels the projection of bulk states. e, Surface bands simulated along a circular momentum loop of radius 0.4π/a (as shown in f) centred at P . The shadow regions indicate the projected bulk states. (f) 3D plot of the surface dispersion simulated in the first quadrant of the surface BZ. Bulk band projections are not shown for clarity. Credit: BY Xiangxi Cai, Liping Ye, Chunyin Qiu, Meng Xiao, Rui Yu, Manzhu Ke, Zhengyou Liu

Dirac semimetals are critical states of topologically distinct phases. Such gapless topological states have been accomplished by a band-inversion mechanism, in which the Dirac points can be annihilated pairwise by perturbations without changing the symmetry of the system. Here, scientists in China report an experimental observation of Dirac points that are enforced completely by the crystal symmetry using a nonsymmorphic phononic crystal. Novel topological surface states are demonstrated in their experiments.

The discovery of new topological states of matter has become a vital goal in and . A three-dimensional (3-D) Dirac semimetal (DSM), accommodating many exotic transport properties such as anomalous magnetoresistance and ultrahigh mobility, is an exceptional platform for exploring topological phase transitions and other novel topological quantum states. It is also of fundamental interest to serve as a solid-state realization of a (3+1)-dimensional Dirac vacuum. So far the realized Dirac points always come in pairs and could be eliminated by their merger and pairwise annihilation through the continuous tuning of parameters that preserve the symmetry of the system.

In a new paper published in Light Science & Applications, scientists from the Key Laboratory of Artificial Micro- and Nano-Structures of the Ministry of Education and School of Physics and Technology, Wuhan University, China, we report an experimental realization of a 3-D phononic crystal that hosts symmetry-enforced Dirac points at the Brillouin zone corners. Markedly different from existing DSMs, the occurrence of Dirac points is an unavoidable result of the nonsymmorphic space group of the material, which cannot be removed without changing the crystal symmetry. In addition to the Dirac points identified directly by angle-resolved transmission measurements, highly intricate quad-helicoid surface states are unveiled by our surface measurements and associated Fourier spectra. Specifically, the surface states are composed of four gaplessly crossed spiral branches and thus are strikingly different than the double Fermi arc surface states observed recently in electronic and photonic systems.

"This study may open up new manners for controlling sound, such as realizing unusual sound scattering and radiation, considering the conical dispersion and vanishing density of states around the Dirac points. The dispersion around the Dirac point is isotropic, and thus, our macroscopic system serves as a good platform to simulate relativistic Dirac physics," the scientists forecast.


Explore further

Exotic new topological state discovered in Dirac semimetals

More information: Xiangxi Cai et al, Symmetry-enforced three-dimensional Dirac phononic crystals, Light: Science & Applications (2020). DOI: 10.1038/s41377-020-0273-4
Journal information: Light: Science & Applications

Citation: Symmetry-enforced three-dimension Dirac phononic crystals (2020, March 20) retrieved 2 April 2020 from https://phys.org/news/2020-03-symmetry-enforced-three-dimension-dirac-phononic-crystals.html
This document is subject to copyright. Apart from any fair dealing for the purpose of private study or research, no part may be reproduced without the written permission. The content is provided for information purposes only.
279 shares

Feedback to editors

User comments