Abstract

Exploiting polaritons in natural vdW materials has been successful in achieving extreme light confinement and low-loss optical devices and enabling simplified device integration. Recently, α-MoO3 has been reported as a semiconducting biaxial vdW material capable of sustaining naturally orthogonal in-plane phonon polariton modes in IR. In this study, we investigate the polarization-dependent optical characteristics of cavities formed using α-MoO3 to extend the degrees of freedom in the design of IR photonic components exploiting the in-plane anisotropy of this material. Polarization-dependent absorption over 80% in a multilayer Fabry-Perot structure with α-MoO3 is reported without the need for nanoscale fabrication on the α-MoO3. We observe coupling between the α-MoO3 optical phonons and the Fabry-Perot cavity resonances. Using cross-polarized reflectance spectroscopy we show that the strong birefringence results in 15% of the total power converted into the orthogonal polarization with respect to incident wave. These findings can open new avenues in the quest for polarization filters and low-loss, integrated planar IR photonics and in dictating polarization control.

Highlights

  • Exploiting polaritons in natural van der Waals (vdW) materials has been successful in achieving extreme light confinement and low-loss optical devices and enabling simplified device integration

  • Hexagonal boron nitride is the most widely investigated of this class, featuring two Reststrahlen (RS) bands where hyperbolic phonon polaritons (PhP) can be supported[28,29]

  • In this work we have demonstrated the polarization-dependent optical responses of α-MoO3 FP cavities numerically and experimentally. α-MoO3 is a vdW semiconductor with strong longitudinal and transverse optical phonon resonances that give rise to high-quality absorption peaks in all the three orthogonal directions distinctly

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Summary

Results

Since OPhs dominate the optical characteristics of α-MoO3 in the mid-infrared, the complex permittivity can be described by phenomenological Lorentz function. Εj:^j; εj 1⁄4 ε1;j j1⁄4x;y;z ω2LO;j À ω2 À iωΓj ω2TO;j À ω2 À iωΓj ð1Þ where ε∞,j and Γj, respectively, stand for the high frequency permittivity and phonon damping

D-MoO3
Discussion
Methods
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