Abstract
Propagating light exhibits hyperbolicity in strongly anisotropic materials where the principal components of the dielectric tensor are opposite in sign. While hyperbolicity occurs naturally in anisotropic polar dielectrics, wherein optical phonons along orthogonal crystal axes are nondegenerate, such optical anisotropy can also be engineered in hyperbolic metamaterials (HMMs): thin film superlattices of alternating dielectric and metallic layers. Contrasted with the severely limited tunability of natural hyperbolic materials, the hyperbolic behavior of HMMs can be tailored significantly both through superlattice design and material selection. However, so far HMMs have suffered from high optical losses, hindering their performance. In this report, broadly tunable (λ = 2–5 µm) Type I and II hyperbolic modes with low losses (quality (Q)-factors up to 19.7) are observed through attenuated total reflectance measurements of monolithic, homoepitaxial superlattices of high- and low-doped cadmium oxide (CdO). Further, the low losses offered by CdO enable the first demonstration of real-space imaging of hyperbolic plasmon polaritons in nanoresonators by scattering-type scanning near-field optical microscopy—previously only possible for hyperbolic phonon polariton materials. Tunable, low-loss CdO HMMs promise designability for applications such as on-chip photonics, super-resolution imaging (hyperlensing), enhanced emission, novel emitter designs, and possibly quantum nanophotonic and time variant metasurfaces.
Original language | English |
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Article number | 2202137 |
Journal | Advanced Optical Materials |
Volume | 11 |
Issue number | 1 |
DOIs | |
State | Published - Jan 4 2023 |
Funding
A.J.C. and J.R.N. contributed equally to this work. A.J.C., J.‐P.M., and J.D.C. gratefully acknowledge support for this work by Office of Naval Research Grant N00014‐22‐12035, and J.R.N. through N00014‐18‐1‐2107. J.D.C., J.‐P.M, and M.H. acknowledge support from the Army Research Office Research Grant W911NF‐21‐1‐0119, and J‐P.M. and J.N. from W911NF‐16‐1‐0406. J.N. gratefully acknowledges support from the Department of Defense (DoD) through the National Defense Science and Engineering Graduate (NDSEG) Fellowship Program. Work within this program was performed at the Vanderbilt Institute for Nanoscale Science and Engineering (VINSE). K.G.W. and T.T. acknowledge support by the Deutsche Forschungsgemeinschaft (DFG No. TA848/7‐1 & SFB 917 “Nanoswitches”). A.J.C. and J.R.N. contributed equally to this work. A.J.C., J.-P.M., and J.D.C. gratefully acknowledge support for this work by Office of Naval Research Grant N00014-22-12035, and J.R.N. through N00014-18-1-2107. J.D.C., J.-P.M, and M.H. acknowledge support from the Army Research Office Research Grant W911NF-21-1-0119, and J-P.M. and J.N. from W911NF-16-1-0406. J.N. gratefully acknowledges support from the Department of Defense (DoD) through the National Defense Science and Engineering Graduate (NDSEG) Fellowship Program. Work within this program was performed at the Vanderbilt Institute for Nanoscale Science and Engineering (VINSE). K.G.W. and T.T. acknowledge support by the Deutsche Forschungsgemeinschaft (DFG No. TA848/7-1 & SFB 917 “Nanoswitches”).
Funders | Funder number |
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U.S. Department of Defense | |
Office of Naval Research | N00014‐18‐1‐2107, N00014‐22‐12035 |
Army Research Office | W911NF‐21‐1‐0119 |
California Department of Fish and Game | SFB 917 |
National Defense Science and Engineering Graduate | |
Vanderbilt Institute of Nanoscale Science and Engineering, Vanderbilt University | |
Deutsche Forschungsgemeinschaft |
Keywords
- cadmium oxide
- hyperbolic metamaterials
- infrared
- plasmonics