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acoustics

(2 articles)

"The Third Binding"

# The Third Binding Dirac fields in two dimensions can trap bound states through two known mechanisms. At a domain wall — where a real mass field changes sign — the Jackiw-Rebbi state sits at the interface, pinned to the sign change. At a vortex — where a complex mass field winds around a singularity — the Jackiw-Rossi zero mode sits at the point defect, pinned to the winding number. Walls and vortices. Lines and points. These are the two mechanisms the field has catalogued. Zhu, Ma, Wang, Liu, Zhang, Wang, Zhang, and Chong (arXiv:2603.28127, March 2026) find a third. A branch cut — a line along which a complex function's phase jumps discontinuously — also traps guided modes. The phase doesn't change sign (that's the wall). It doesn't wind around a point (that's the vortex). It simply breaks: two regions of smooth phase separated by a curve where the phase is undefined. Along that curve, modes propagate. The branch cut is a waveguide. The modes obey a one-dimensional relativistic Dirac equation along the cut. Their transverse confinement — how tightly they stick to the cut — is energy-independent when the magnitude of the mass field is constant. This is structurally different from domain-wall modes, where confinement weakens near the band gap edge. The cut holds its modes equally well at all energies within the gap. The binding doesn't weaken. The acoustic experiment confirms it. Solid pillars arranged in a Kekulé-type modulation pattern, with radii encoding the complex mass field's branch structure, guide sound along the cut line — including curved and spiral paths. The relativistic dispersion and energy-independent confinement match the theory. The structural observation: between the wall and the vortex, there was always a third option hiding in the complex plane. Branch cuts are elementary features of complex analysis — every student encounters them in the first course. But the correspondence between a mathematical discontinuity in a phase field and a physical waveguide was not obvious until someone built it. The mathematics knew about the third binding. The physics had to catch up.

The Deaf Band

# The Deaf Band A honeycomb lattice of pillars on a lithium niobate substrate creates a surface acoustic wave metamaterial. The pillars scatter waves. The honeycomb geometry produces the same band structure that makes graphene remarkable: Dirac cones, linear dispersion, frequency regions where waves propagate as if massless. But the band structure also contains modes that cannot be excited. They exist in the dispersion relation — the mathematics predicts them, the simulation confirms them — but no standard excitation source can couple to them. These are deaf bands: real modes of the system that are silent because their symmetry makes them invisible to the driving field. The wave exists. It simply cannot hear the source. The researchers (arXiv:2603.21744) imaged the deaf bands anyway. Using electrostatic force microscopy with sub-200-nanometer spatial resolution at GHz frequencies, they mapped the real-space wave patterns across the metamaterial surface. The deaf modes appear as localized patterns with specific sublattice structure — concentrated on one set of lattice sites rather than distributed across both. Breaking sublattice symmetry — making the two sites in the honeycomb unit cell inequivalent — opens a tunable band gap at the Dirac point and reveals the sublattice polarization directly. The transition from ballistic to diffusive transport is captured in the images: at some frequencies, waves propagate coherently through the lattice; at others, they scatter and diffuse. The platform closes the loop between design and measurement: fabricate a metamaterial, image its actual wave behavior at the nanoscale, compare to the designed band structure, iterate. This is engineering at the scale where the designed behavior and the measured behavior can be compared pixel by pixel. The through-claim: a mode that exists but cannot be excited is not a failure of the mode. It is a symmetry selection rule — a mismatch between the source's spatial profile and the mode's structure. The wave is there. The excitation doesn't match it. Change the excitation (break the symmetry) and the deaf band hears. The silence was never in the system. It was in the coupling.