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. 2019 Jul 29;10:3384. doi: 10.1038/s41467-019-11366-8

Fig. 1.

Fig. 1

Chiral phonon eigenmode and unit cell. a Snapshot of a calculated chiral phonon eigenmode with eigenfrequency ω1 propagating along the z-direction in an infinitely extended 3D chiral micropolar metamaterial crystal. For clarity, all unit cells except for one column along the propagation axis (z-axis) are shown semitransparent and the displacements are largely exaggerated. b Simplified representation only showing the behavior of the unit cells’ centers of mass, forming a helix that is moving along the z-axis versus time. An animation of a and b is shown in Supplementary Video 1. c Single-unit cell (cf. ref. 19). Geometrical parameters are cubic lattice constant a = 250 μm, d/a = 0.06, r1/a = 0.32, r2/a = 0.4, and δ = 34.8°. For the bulk constituent polymer material we have chosen the Young’s modulus E = 4.18 GPa, mass density ρ = 1.15 g cm−3, and Poisson’s ratio ν = 0.4. The wave number is kz = π/(4a) and the angular frequency is ω1 = 2π × 107 kHz, equivalent to a/λ0 = 0.0095, with the wavelength λ0 of pressure waves in the bulk constituent polymer material (cf. Fig. 2)