Hyperbolic phonon polaritons in hexagonal boron nitride
S. Dai (University of California)
Q Ma (Massachusetts Institute of Technology)
Z Fei (University of California)
M Liu (University of California)
MD Goldflam (University of California)
T Andersen (Massachusetts Institute of Technology)
W. Garnett (University of California)
W. Regan (University of California)
M Wagner (University of California)
AS McLeod (University of California)
A Rodin (National University of Singapore)
S. Zhu (TU Delft - Micro and Nano Engineering)
Kenji Watanabe (National Institute for Materials Science)
T Taniguchi (National Institute for Materials Science)
G. Dominguez (University of California)
M Thiemens (University of California)
A.H. Castro Neto (National University of Singapore)
G.C.A.M. Janssen (TU Delft - Micro and Nano Engineering)
A. Zetti (University of California)
F Keilmann (Ludwig Maximilians University)
P Jarillo-Herrero (Massachusetts Institute of Technology)
M.M. Fogler (University of California)
DN Basov (University of California)
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Abstract
Uniaxial materials whose axial and tangential permittivities have opposite signs are referred to as indefinite or hyperbolic media. While hyperbolic responses are normally achieved with metamaterials, hexagonal boron nitride (hBN) naturally possesses this property due to the anisotropic phonons in the mid-infrared. Using scattering-type scanning near-field optical microscopy, we studied polaritonic phenomena in hBN. We performed infrared nano-imaging of highly confined and low-loss hyperbolic phonon polaritons in hBN. The polariton wavelength was shown to be governed by the hBN thickness according to a linear law persisting down to few atomic layers [1]. Additionally, we carried out the modification of hyperbolic response in meta-structures comprised of a mononlayer graphene deposited on hBN [2]. Electrostatic gating of the top graphene layer allows for the modification of wavelength and intensity of hyperbolic phonon polaritons in bulk hBN. The physics of the modification originates from the plasmon-phonon coupling in the hyperbolic medium. Furthermore, we demonstrated the “hyperlens” for subdiffractional focusing and imaging using a slab of hBN [3]. References [1] S. Dai et al., Science, 343, 1125 (2014). [2] S. Dai et al., Nature Nanotechnology, 10, 682 (2015). [3] S. Dai et al., Nature Communications, 6, 6963 (2015).
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