Guiding waves through a stable physical channel is essential for reliable information transport. However, energy transport in high-frequency mechanical systems, such as in signal-processing applications1, is particularly sensitive to defects and sharp turns because of back-scattering and losses2. Topological phenomena in condensed matter systems have shown immunity to defects and unidirectional energy propagation3. Topological mechanical metamaterials translate these properties into classical systems for efficient phononic energy transport. Acoustic and mechanical topological metamaterials have so far been realized only in large-scale systems, such as arrays of pendulums4, gyroscopic lattices5,6, structured plates7,8 and arrays of rods, cans and other structures acting as acoustic scatterers9,10,11,12. To fulfil their potential in device applications, mechanical topological systems need to be scaled to the on-chip level for high-frequency transport13,14,15. Here we report the experimental realization of topological nanoelectromechanical metamaterials, consisting of two-dimensional arrays of free-standing silicon nitride nanomembranes that operate at high frequencies (10–20 megahertz). We experimentally demonstrate the presence of edge states, and characterize their localization and Dirac-cone-like frequency dispersion. Our topological waveguides are also robust to waveguide distortions and pseudospin-dependent transport. The on-chip integrated acoustic components realized here could be used in unidirectional waveguides and compact delay lines for high-frequency signal-processing applications.
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The data that support the findings of this study are available from the corresponding author upon reasonable request.
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J.C. and C.D. acknowledge partial support for this project from NSF EFRI award number 1741565, and the Kavli Nanoscience Institute at Caltech. K.W.K. acknowledges support for this project from the “Overseas Research Program for Young Scientists” programme through the Korea Institute for Advanced Study (KIAS).
Nature thanks S. Iwamoto and the other anonymous reviewers for their contribution to the peer review of this work.
The authors declare no competing interests.
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended data figures and tables
a, Etch holes are periodically arranged in an extended honeycomb lattice. a is a lattice parameter and w is the distance between two neighbouring etch holes. The bottom picture shows the cross-sectional view. b, After a sample is immersed in a buffered oxide etchant, the thermal SiO2 is radially etched from the etch holes. The etching paths are illustrated by the brown circles with radius r. The overlap between two membranes affects the coupling strength, by controlling the distance w. c, Optical microscope image of a partially etched samples. The yellow circles represent free-standing SiNx membranes and the darker/purple region is SiNx/SiO2. Scale bar, 18 μm.
a–c, Unit cell geometries for w = 5.5 μm (a), w = 6.0 μm (b) and w = 6.5 μm (c). Here, r = 4.9 μm is the etching distance from the centre of the etch holes. The central hexagon and the six corners represent the regions of unetched thermal SiO2. These are modelled as fixed boundaries in finite element simulations.
a, Frequency responses (amplitude only) obtained from a spatial scan of 20 sites of the straight edge waveguide. The scanning period is 18 μm. The intensity decay around 15 MHz represents a defect mode. b, Amplitude × sin(phase) responses obtained from the spatial scan. c, Frequency dispersion obtained from Fourier transformation of the data shown in b.
a, Optical microscope image of the excitation region and the defective unit including the gold electrode. b, Experimental data for the amplitude decay of the defect mode. The red squares denote the experimental data and the black solid line represents a fitting function. Here, the fitting parameters a and b are 1.408 mV and 114.1292 μm.
a, Frequency dispersion curve along the edge waveguide. b, Frequency responses of the bulk of the non-trivial phase (left), the output of the edge waveguide (middle), and the bulk of the trivial phase (right). c, A spatiotemporal response of unfiltered propagating pulses with broadband frequencies ranging from 12.8 MHz to 15.8 MHz. d–k, Filtered spatiotemporal responses of the propagating pulses with different centre frequencies. The bandwidth of the pulses is 0.3 MHz. The centre frequencies are 13.48 MHz (d), 13.68 MHz (e), 13.85 MHz (f), 14.1 MHz (g), 14.35 MHz (h), 14.75 MHz (i), 14. 975 MHz (j) and 15.23 MHz (k).
a–e, Frequency responses of the bulk of the non-trivial phase (w = 6.5 μm; a), output 1 (b), output 2 (c), output 3 (d) and the bulk of the trivial phase (w = 5.5 μm; e), shown in Fig. 4a. The light-red and light-blue regions represent the bandgaps of the non-trivial and trivial phases, respectively.
The corresponding wavenumber and eigenfrequency are 17,453 m−1 and 14.77 MHz.
The corresponding wavenumber and eigenfrequency are -17,453 m−1 and 15.15 MHz.
The corresponding wavenumber and eigenfrequency are -17,453 m−1 and 14.77 MHz.
The corresponding wavenumber and eigenfrequency are 17,453 m−1 and 15.15 MHz.
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Cha, J., Kim, K.W. & Daraio, C. Experimental realization of on-chip topological nanoelectromechanical metamaterials. Nature 564, 229–233 (2018) doi:10.1038/s41586-018-0764-0
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