Berry effect in acoustical polarization transport in phononic crystals
arXiv:0810.4992 · doi:10.1134/S0021364008210091
Abstract
We derive the semiclassical equations of motion of a transverse acoustical wave packet propagating in a phononic crystal subject to slowly varying perturbations. The formalism gives rise to Berry effect terms in the equations of motion, manifested as the Rytov polarization rotation law and the polarization-dependent Hall effect. We show that the formalism is also applicable to the case of non-periodic inhomogeneous media, yielding explicit expressions for the Berry effect terms.
To appear in JETP Lett
References in corpus (10)
- Dissipationless Quantum Spin Current at Room Temperature
- Hall Effect of Light
- Anomalous Hall effect in paramagnetic two dimensional systems
- Spin Hall effect and Berry phase of spinning particles
- Modified geometrical optics of a smoothly inhomogeneous isotropic medium: the anisotropy, Berry phase, and the optical Magnus effect
- Fermat Principle for spinning light
- Geometrical Aspects in Optical Wavepacket Dynamics
- Polarization Transport of Transverse Acoustic Waves: Berry Phase and Spin Hall Effect of Phonons
- Topological spin transport of photons: "magnetic monopole" gauge field in Maxwell equations and polarization splitting of rays in periodically inhomogeneous media
- Dynamical Diffraction Theory for Wave Packet Propagation in Deformed Crystals
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- Paraxial propagation in amorphous optical media with screw dislocation
- Cosmological Birefringence and the Geometric Phase of Photons
- Paraxial propagation in disclinated amorphous media
- A Quantum Mechanical Approach To The Polarization Transport of Photons
- Spin Hall effect of light in inhomogeneous axion field