Abstract

We construct a novel Lagrangian representation of acoustic field theory that describes the local vector properties of longitudinal (curl-free) acoustic fields. In particular, this approach accounts for the recently-discovered nonzero spin angular momentum density in inhomogeneous sound fields in fluids or gases. The traditional acoustic Lagrangian representation with a scalar potential is unable to describe such vector properties of acoustic fields adequately, which are however observable via local radiation forces and torques on small probe particles. By introducing a displacement vector potential analogous to the electromagnetic vector potential, we derive the appropriate canonical momentum and spin densities as conserved Noether currents. The results are consistent with recent theoretical analyses and experiments. Furthermore, by an analogy with dual-symmetric electromagnetic field theory that combines electric- and magnetic-potential representations, we put forward an acoustic spinor representation combining the scalar and vector representations. This approach also includes naturally coupling to sources. The strong analogies between electromagnetism and acoustics suggest further productive inquiry, particularly regarding the nature of the apparent spacetime symmetries inherent to acoustic fields.

Highlights

  • Linear sound waves in gases or fluids are purely longitudinal, and these are usually considered within the scalar wave theory [1,2,3]

  • Recent studies revealed the presence of nonzero local spin angular momentum density in generic acoustic fields [5,6,7,8,9,10], and this prompted interest in vector properties of acoustic waves

  • We show that by choosing different Lagrangians and different representations of the acoustic fields by scalar and vector potentials one can derive different canonical momentum and angular-momentum densities, containing both scalar and vector degrees of freedom including non-zero spin (2)

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Summary

27 May 2020

Acoustic versus electromagnetic field theory: scalar, vector, spinor representations and the emergence of acoustic spin. Lucas Burns1,2,5 , Konstantin Y Bliokh3,5 , Franco Nori and Justin Dressel

Introduction
Linear acoustic and electromagnetic theories
Electromagnetic potentials
Acoustic potentials
Equations of motion and gauge fixing
Canonical momentum and spin densities
Sources and combined spinor potentials
Symmetric spinor potential representation
Concluding remarks
Full Text
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