2018
DOI: 10.1002/adma.201706358
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Manipulation and Steering of Hyperbolic Surface Polaritons in Hexagonal Boron Nitride

Abstract: Hexagonal boron nitride (hBN) is a natural hyperbolic material that supports both volume-confined hyperbolic polaritons and sidewall-confined hyperbolic surface polaritons (HSPs). In this work, efficient excitation, control, and steering of HSPs are demonstrated in hBN through engineering the geometry and orientation of hBN sidewalls. By combining infrared nanoimaging and numerical simulations, the reflection, transmission, and scattering of HSPs are investigated at the hBN corners with various apex angles. It… Show more

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Cited by 70 publications
(57 citation statements)
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“…h‐BN has a uniaxial permittivity and exhibits a hyperbolic isofrequency curve in two infrared Reststrahlen bands (regions between transversal and longitudinal optical phonon frequencies, ω TO and ω LO , respectively), where ε ⊥ > 0 and ε ∥ < 0 (lower band) and ε ⊥ < 0, ε ∥ > 0 (upper band), respectively. In the upper band, two types of HPs have been found: volume‐confined HPs in extended slabs, and in resonator structures, as well as surface‐confined HPs at the edges of slabs, linear antennas and cylindrical waveguides . However, a detailed study of HP modes in long ribbons with rectangular cross section, representing canonical linear waveguide structures, has not been reported yet.…”
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confidence: 99%
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“…h‐BN has a uniaxial permittivity and exhibits a hyperbolic isofrequency curve in two infrared Reststrahlen bands (regions between transversal and longitudinal optical phonon frequencies, ω TO and ω LO , respectively), where ε ⊥ > 0 and ε ∥ < 0 (lower band) and ε ⊥ < 0, ε ∥ > 0 (upper band), respectively. In the upper band, two types of HPs have been found: volume‐confined HPs in extended slabs, and in resonator structures, as well as surface‐confined HPs at the edges of slabs, linear antennas and cylindrical waveguides . However, a detailed study of HP modes in long ribbons with rectangular cross section, representing canonical linear waveguide structures, has not been reported yet.…”
mentioning
confidence: 99%
“…All modes have a complex‐valued wavevector k = q + iγ, where q is the momentum of the mode in the propagation direction and γ is the damping. For a comprehensive understanding of the waveguide modes, we also plot the fundamental volume and surface modes that exist in an extended h‐BN slab of the same thickness: M 0 (dashed blue line) and SM 0 (dashed gray line), the latter one propagating along the edge of the semi‐infinite h‐BN slab (see Section S2 of the Supporting Information for details of electric and magnetic field components of volume and surface modes).…”
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confidence: 99%
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“…f) The s‐SNOM line traces taken from panel (e) reveal the wavelength difference in hyperbolic phonon polaritons (HP, blue) and hyperbolic surface phonon polaritons (HSP). e,f) Reproduced with permission . Copyright 2018, Wiley‐VCH.…”
Section: Phonon Polaritons In Low‐dimensional Materialsmentioning
confidence: 99%
“…HP 2 waves have been observed in hBN‐based systems by s‐SNOM and photoinduced force microscopy (PiFM) . They are typically launched or emitted by edges and features of the hBN crystal or by metallic antennas . Being volume confined modes, the HP 2 λ p is dependent on the crystal thickness and also on the dielectric function of the substrate, with λ0/λp ultimately approaching 50 .…”
Section: Introductionmentioning
confidence: 99%