Tunable, Homoepitaxial Hyperbolic Metamaterials Enabled by High Mobility CdO

被引:7
|
作者
Cleri, Angela J. [1 ]
Nolen, J. Ryan [2 ,3 ]
Wirth, Konstantin G. [4 ]
He, Mingze [5 ]
Runnerstrom, Evan L. [6 ]
Kelley, Kyle P. [7 ]
Nordlander, Joshua [1 ]
Taubner, Thomas [4 ]
Folland, Thomas G. [5 ,8 ]
Maria, Jon-Paul [1 ]
Caldwell, Joshua D. [5 ]
机构
[1] Penn State Univ, Dept Mat Sci & Engn, University Pk, PA 16802 USA
[2] Vanderbilt Univ, Interdisciplinary Mat Sci Program, Nashville, TN 37212 USA
[3] CUNY, Adv Sci Res Ctr, Photon Initiat, New York, NY 10031 USA
[4] Rhein Westfal TH Aachen, Inst Phys IA, D-52062 Aachen, Germany
[5] Vanderbilt Univ, Dept Mech Engn, Nashville, TN 37212 USA
[6] Army Res Off, DEVCOM US Army Res Lab, Res Triangle Pk, NC 27703 USA
[7] Oak Ridge Natl Lab, Ctr Nanophase Mat Sci, Oak Ridge, TN 37830 USA
[8] Univ Iowa, Sch Phys & Astron, Iowa City, IA 52242 USA
来源
ADVANCED OPTICAL MATERIALS | 2023年 / 11卷 / 01期
关键词
cadmium oxide; hyperbolic metamaterials; infrared; plasmonics; FIELD THERMAL EMISSION; DOPED CADMIUM-OXIDE; OPTICAL HYPERLENS; POLARITONS; RESONANCE; REALIZATION; NANOSCALE; DEVICE; INDEX;
D O I
10.1002/adom.202202137
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
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 (lambda = 2-5 mu m) 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.
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页数:9
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