Apr 23, 2024
1:45pm - 2:00pm
Room 340/341, Level 3, Summit
Saurabh Dixit1,Maximilian Obst2,José Cuervo3,Giulia Carini4,Ryan Kowalski1,Aitana Martín-Luengo3,Gonzalo Alvarez Perez3,Katja Diaz-Granados Santos1,Aditha Senarath1,Niclas Müller4,J. Michael Klopf5,Lukas Eng2,Susanne Kehr2,Thomas Folland6,Pablo Alonso Gonzalez3,Alex Paarmann4,Joshua Caldwell1
Vanderbilt University1,Technische Universität Dresden2,University of Oviedo3,Max Planck Society4,Helmholtz-Zentrum Dresden-Rossendorf5,The University of Iowa6
Saurabh Dixit1,Maximilian Obst2,José Cuervo3,Giulia Carini4,Ryan Kowalski1,Aitana Martín-Luengo3,Gonzalo Alvarez Perez3,Katja Diaz-Granados Santos1,Aditha Senarath1,Niclas Müller4,J. Michael Klopf5,Lukas Eng2,Susanne Kehr2,Thomas Folland6,Pablo Alonso Gonzalez3,Alex Paarmann4,Joshua Caldwell1
Vanderbilt University1,Technische Universität Dresden2,University of Oviedo3,Max Planck Society4,Helmholtz-Zentrum Dresden-Rossendorf5,The University of Iowa6
Opposite signs of the dielectric permittivity along different principal directions of optical materials (hyperbolic anisotropy) allow for exotic quasiparticles to be formed due to the hybridization of photons and phonons (phonon polariton) in the mid-infrared spectral region. Phonon-polaritons in such hyperbolic materials enable the confinement of electromagnetic waves at the nanoscale, which offers mechanisms to induce large enhancements of the optical response and reduce the footprint of photonic devices such as molecule sensors, polarizers, waveplates, optical modulators, IR sources and detectors, and many others. To design nanophotonic devices, it is necessary to engineer the characteristic features of phonon polaritons, like propagation direction and distances. It has been demonstrated that characteristic features of hyperbolic phonon polaritons can be engineered via the choice of crystal symmetry. Hyperbolic polaritons in crystals with varying symmetries from hexagonal, such as boron nitride (h-BN), exhibit isotropic propagation in plane, whereas reducing to orthorhombic structures like MoO<sub>3</sub> and V<sub>2</sub>O<sub>5</sub>, results in directional propagation. Monoclinic systems, such as β-Ga<sub>2</sub>O<sub>3</sub> or CdWO<sub>4</sub>, with further reduced symmetry exhibit exotic phenomena in the form of shear, whereby the polariton wavelength and direction of propagation disperse with changing frequency. This provides an additional degree of freedom to manipulate polariton propagation. By employing twisted low symmetry structures, such as twisted slabs of MoO<sub>3</sub>, highly directional propagation with minimal divergence can be observed (canalization) at specific ‘magic’ angles. Yet, it remains unclear if such canalization can be observed in twisted structures of different Bravais lattices. Here, we investigate heterostructures of MoO<sub>3</sub> orthorhombic) and Ga<sub>2</sub>O<sub>3</sub> (monoclinic) to determine the role of twisting with non-degenerate polariton resonances, as well as the potential influence of shear. By investigating a series of MoO<sub>3</sub> slabs twisted with respect to the a-axis of β-Ga<sub>2</sub>O<sub>3</sub> we observed the change in the direction of propagation along with asymmetric dispersion via a scattering-type SNOM coupled to a free-electron laser. It is determined that the high asymmetry in the propagation in the twisted structure is driven principally by the twist angle, rather than the inherent shear in the underlying β-Ga<sub>2</sub>O<sub>3</sub>, indicating that the propagation direction can be dictated via twist angle, making such heterostructure platforms designable for future nanophotonic devices such as sensors, chiral sources, IR imaging components, and many others.