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1.School of Engineering, College of Engineering, Computing & Cybernetics, the Australian National University, Canberra, ACT 2601, Australia
2.Department of Electrical and Computer Engineering, University of WisconsinMadison, Madison, WI 53706, USA
3.Department of Physics, Imperial College London, London SW7 2AZ, UK
4.ARC Centre of Excellence in Quantum Computation and Communication Technology ANU node, Canberra, ACT 2601, Australia
5.School of Physics and Astronomy, Monash University Clayton Campus, Melbourne, VIC 3800, Australia
Zongfu Yu (zyu54@wisc.edu)
Yuerui Lu (yuerui.lu@anu.edu.au)
Received:11 September 2024,
Revised:2025-04-16,
Accepted:20 June 2025,
Published Online:26 July 2025,
Published:30 September 2025
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Suriyage, M. et al. Long-propagating ghost phonon polaritons enabled by selective mode excitation. Light: Science & Applications, 14, 2685-2695 (2025).
Suriyage, M. et al. Long-propagating ghost phonon polaritons enabled by selective mode excitation. Light: Science & Applications, 14, 2685-2695 (2025). DOI: 10.1038/s41377-025-01925-8.
The ability to precisely control the excitation of phonon polaritons (PhPs) provides unique opportunities for various nanophotonic applications
such as on-chip optical communication
quantum information processing
and controlled thermal radiation. Recently
ghost hyperbolic phonon polaritons (g-HPs) have been discovered
which exhibit in-plane hyperbolic dispersion on the surface and oblique wavefronts in the bulk. These g-HPs exhibit long-range
ray-like propagation
which is highly desirable. However
selective excitation of polaritonic modes and flexible control over the directionality of g-HPs remains an open problem. In this work
we experimentally demonstrate that changing the shape of the launching micro/nano antenna allows for control over the polariton mode excitation. Using a single asymmetric triangular gold antenna fabricated on a calcite crystal surface
we showcase highly directional g-HP excitation through selectively exciting desirable polariton modes. Our near-field imaging experiments verify that the g-HP excited by the triangular antenna can propagate over 80 microns
which is consistent with our numerical predictions. Overall
by combining g-HP theory with structural engineering
our work has further developed the potential of such anisotropic materials
enabling unexpected control over g-HPs
thus opening opportunities for various applications in mid-IR optoelectronics.
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