Graphene on hexagonal boron nitride as a tunable hyperbolic metamaterial

TL;DR

This paper demonstrates that stacking graphene on hexagonal boron nitride creates a tunable hyperbolic metamaterial with enhanced propagation length for hyperbolic polaritons, combining properties of both materials.

Contribution

It introduces a method to modulate hyperbolic phonon polaritons using graphene/h-BN heterostructures, enabling tunability and reduced losses in hyperbolic metamaterials.

Findings

Hyperbolic plasmon-phonon polaritons can be effectively modulated in graphene/h-BN heterostructures.

Propagation length of these polaritons is 1.5-2.0 times greater than in h-BN alone.

Graphene/h-BN structures act as novel electromagnetic metamaterials.

Abstract

Hexagonal boron nitride (h-BN) is a natural hyperbolic material, for which the dielectric constants are the same in the basal plane (epsilon^t = epsilon^x = epsilon^y) but have opposite signs (epsilon^t*epsilon^z < 0) from that in the normal plane (epsilon^z). Due to this property, finite-thickness slabs of h-BN act as multimode waveguides for propagation of hyperbolic phonon polaritons - collective modes that originate from the coupling between photons and electric dipoles in phonons. However, control of these hyperbolic phonon polaritons modes has remained challenging, mostly because their electrodynamic properties are dictated by the crystal lattice of h-BN. Here we show by direct nano-infrared imaging that these hyperbolic polaritons can be effectively modulated in a van der Waals heterostructure composed of monolayer graphene on h-BN. Tunability originates from the hybridization of surface plasmon polaritons in graphene with hyperbolic phonon polaritons in h-BN, so that the eigenmodes of the graphene/h-BN heterostructure are hyperbolic plasmon-phonon polaritons. Remarkably, the hyperbolic plasmon-phonon polaritons in graphene/h-BN suffer little from ohmic losses, making their propagation length 1.5-2.0 times greater than that of hyperbolic phonon polaritons in h-BN. The hyperbolic plasmon-phonon polaritons possess the combined virtues of surface plasmon polaritons in graphene and hyperbolic phonon polaritons in h-BN. Therefore, graphene/h-BN structures can be classified as electromagnetic metamaterials since the resulting properties of these devices are not present in its constituent elements alone.