Abstract
Compressing light into nanocavities substantially enhances light–matter interactions, which has been a major driver for nanostructured materials research. However, extreme confinement generally comes at the cost of absorption and low resonator quality factors. Here we suggest an alternative optical multimodal confinement mechanism, unlocking the potential of hyperbolic phonon polaritons in isotopically pure hexagonal boron nitride. We produce deep-subwavelength cavities and demonstrate several orders of magnitude improvement in confinement, with estimated Purcell factors exceeding 108 and quality factors in the 50–480 range, values approaching the intrinsic quality factor of hexagonal boron nitride polaritons. Intriguingly, the quality factors we obtain exceed the maximum predicted by impedance-mismatch considerations, indicating that confinement is boosted by higher-order modes. We expect that our multimodal approach to nanoscale polariton manipulation will have far-reaching implications for ultrastrong light–matter interactions, mid-infrared nonlinear optics and nanoscale sensors.
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The data that support the findings of this study are available from the corresponding author upon request.
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Acknowledgements
F.H.L.K. acknowledges support from the ERC TOPONANOP under grant agreement no. 726001, the ERC proof-of-concept grant Polarsense, the Government of Spain (FIS2016-81044; Severo Ochoa CEX2019-000910-S), Fundació Cellex, Fundació Mir-Puig and Generalitat de Catalunya (CERCA, AGAUR, SGR 1656). Furthermore, the research leading to these results has received funding from the European Union’s Horizon 2020 programme under grant agreement no. 881603 (Graphene Flagship Core3). H.H.S. acknowledges funding from the European Union’s Horizon 2020 programme under the Marie Skłodowska-Curie grant agreement no. 843830. N.C.H.H. acknowledges funding from the European Union’s Horizon 2020 programme under the Marie Skłodowska-Curie grant agreement no. 665884. R.B. acknowledges funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 847517. L.O. acknowledges support by The Secretaria d'Universitats i Recerca del Departament d'Empresa i Coneixement de la Generalitat de Catalunya, as well as the European Social Fund (L'FSE inverteix en el teu futur)—FEDER. M.C. acknowledge the support of the 'Presencia de la Agencia Estatal de Investigación' within the Convocatoria de tramitación anticipada, correspondente al año 2020, de las ayudas para contractos predoctorales (Ref. PRE2020-094864) para la formación de doctores contemplada en el Subprograma Estatal de Fromación del Programa Estatal de Promoción del Talento y su Empleabilidad en I+D+i, en el marco del Plan Estatal de Investigacón Científica y Técnica de Innovación 2017–2020, cofinanciado por el Fondo Social Europeo. J.H.E. acknowledges support from the Office of Naval Research (award N00014-20-1-2474). M.J. and G.S. acknowledge support from the Office of Naval Research (ONR) under grant no. N00014-21-1-2056, the support of the Army Research Office under award W911NF2110180 and by the National Science Foundation (NSF) under grant no. DMR-1719875. M.J. was also supported in part by the Kwanjeong Fellowship from Kwanjeong Educational Foundation. R.M. and V.P. acknowledge support from the Opto group Plan Nacional project (TUNASURF). We also wish to thank J. Osmond, H. Lozano and N. V. Hulst for help with the FIB operation, which was also supported by the European Commission under ERC Advanced Grant 670949-LightNet.
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H.H.S., L.O., M.C., D.B.R., S.C., R.M. and V.P. worked on the sample fabrication with help from A.Hötger. and A.Holleitner. The isotopic hBN crystals were grown by E.J. and J.H.E. The measurements were performed by H.H.S. and L.O. with help from D.B.R. and N.C.H.H. The analytical and semi-analytical theory was developed by H.H.S., I.T. and M.C., and the numerical calculations were performed by M.J., M.C., S.M., R.B. and G.S. The experiments were designed by H.H.S. and F.H.L.K. All authors contributed to writing the manuscript and A.Holleitner., V.P., G.S. and F.H.L.K. supervised the work.
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Supplementary Sections 1–5, Figs. 1–31 and references.
Supplementary Video 1
Simulated electric-field amplitude in an inverted cavity, for plane-wave excitation at a varying frequency (Supplementary Section 4.2). The cavity is expected to be resonant at around 1,393 cm–1, but shows no clear resonant response. The simulation dimensions are scaled for presentation purposes, the size of the MEC (inverted cavity) is 260 nm and the flake is 10 nm thin. The brighter areas in the colour map correspond to a higher signal and each subplot is separately normalized.
Supplementary Video 2
Simulated electric-field phase in an inverted cavity, for plane-wave excitation at a varying frequency (Supplementary Section 4.2). The simulation dimensions are scaled for presentation purposes, the size of the MEC (inverted cavity) is 260 nm and the flake is 10 nm thin. The colour map goes from –π (green) to π (purple).
Supplementary Video 3
Simulated electric-field amplitude in an MEC cavity, for plane-wave excitation at a varying frequency (Supplementary Section 4.2). As the frequency reaches the resonant frequency of 1,507 cm–1, the field is strongly localized inside the cavity and exhibits sharp (multimodal) ray-like features. The simulation dimensions are scaled for presentation purposes, the size of the MEC (inverted cavity) is 260 nm and the flake is 10 nm thin. The brighter areas in the colour map correspond to a higher signal and each subplot is separately normalized.
Supplementary Video 4
Simulated electric-field phase in an MEC cavity, for plane-wave excitation at a varying frequency (Supplementary Section 4.2). The simulation dimensions are scaled for presentation purposes, the size of the MEC (inverted cavity) is 260 nm and the flake is 10 nm thin. The colour map goes from –π (green) to π (purple).
Supplementary Video 5
Simulated intensity profile of a multimodal nanoray propagating inside an hBN flake (edges indicated by cyan lines) when it is incident on a single metallic corner. The ray is excited by a dipole situated outside (to the left), which is not shown to avoid colour saturation. The frequency of excitation—and therefore the angle of the nanoray—is swept throughout the video. When the ray is exactly incident on the corner, it experiences strong (enhanced) reflection, whereas for other frequencies, the ray experiences enhanced transmission (Supplementary Section 4.3).
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Herzig Sheinfux, H., Orsini, L., Jung, M. et al. High-quality nanocavities through multimodal confinement of hyperbolic polaritons in hexagonal boron nitride. Nat. Mater. 23, 499–505 (2024). https://doi.org/10.1038/s41563-023-01785-w
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DOI: https://doi.org/10.1038/s41563-023-01785-w
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