WebOct 12, 2015 · with f the frequency of the sound wave, c 1 the sound speed in the medium surrounding the SPP and c 2 the sound speed in the material that constitutes the SPP. A normally incident axisymmetric acoustic wave thus emerges from the SPP with a pressure field having an azimuthal dependence of the form i.e. an acoustic vortex with topological … WebFor instance, spin waves under a Dzyaloshinkii–Moriya interaction are non-reciprocal since the eigenfrequency depends linearly on the wave vector. 14) According to these definitions, the recent experiments 4, 6, 8, 10, 12) indicate that the interaction between magnetisation dynamics and SAWs is chiral, and their transmission across magnetic ...
Phys. Rev. Lett. 124, 235502 (2024) - Isotropic Chiral …
WebJun 15, 2024 · The existence of antichiral edge states is revealed through full-wave simulations of the band structure and acoustic fields excited by a point source. Furthermore, we compare these antichiral edge states with conventional chiral edge states. It is found that the antichiral edge states are less robust than the chiral ones. WebJan 6, 2024 · The chiral edge states in graphene have been experimentally observed by harnessing the QH effect with an external magnetic field ( 7 ). Without requiring an external magnetic field, the graphene chiral edge states can also be realized by harnessing the QSH effect ( 8 ). However, because of the weak spin-orbit interaction, experimental ... philips bass
Chirality-switchable acoustic vortex emission via non-Hermitian ...
The above physics can be extended to the 3D metamaterial with the unit cell shown in Fig. 3a. The unit cell consists of three chiral resonators mutually connected with tubes, as shown in Fig. 3b. The numerically calculated band structure of the metamaterial is shown in Fig. 3c. The lowest three bands derive … See more The longitudinal nature of airborne sound (\({{{{{\boldsymbol{\nabla }}}}}}\times {{{{{\bf{v}}}}}}=0\)) dictates that the velocity field v aligns with the direction of wave vector k in general. … See more The SOIs of transverse waves can also happen in real space. One intriguing phenomenon induced by such SOIs is the spin-dependent vortex generation in the scattering of subwavelength particles, which leads to the … See more The transverse sound near the \(\Gamma\) point in Fig. 3c can be described by an effective Hamiltonian \(H=-v{{{{{\bf{S}}}}}}\cdot {{{{{\bf{k}}}}}}\) with S being the spin-1 operator defined as \({({S}_{i})}_{{jk}}= … See more WebJan 24, 2024 · (b) Screenshots of the syndiotactic chiral beam in the anti-resonance and resonance peaks, at point A of frequency of 970 Hz, at point B of frequency of 1192 Hz, at point C of frequency of 3082 Hz ... WebFeb 16, 2024 · to chiral acoustic wave transport. In this work we rst derive the dispersion relation of the metamaterial waveguide by employing the generalized Bloch-Floquet expansion formula. We nd that there are three non-trivial dispersion regimes, which respectively correspond to left/right chiral emission and band gaps. Then we trust tax return form ato