Abstract

In the Reststrahlen region, between the transverse and longitudinal phonon frequencies, polar dielectric materials respond metallically to light, and the resulting strong light-matter interactions can lead to the formation of hybrid quasiparticles termed surface phonon polaritons. Recent works have demonstrated that when an optical system contains nanoscale polar elements, these excitations can acquire a longitudinal field component as a result of the material dispersion of the lattice, leading to the formation of secondary quasiparticles termed longitudinal-transverse polaritons. In this work, we build on previous macroscopic electromagnetic theories, developing a full second-quantized theory of longitudinal-transverse polaritons. Beginning from the Hamiltonian of the light-matter system, we treat distortion to the lattice, introducing an elastic free energy. We then diagonalize the Hamiltonian, demonstrating that the equations of motion for the polariton are equivalent to those of macroscopic electromagnetism and quantize the nonlocal operators. Finally, we demonstrate how to reconstruct the electromagnetic fields in terms of the polariton states and explore polariton induced enhancements of the Purcell factor. These results demonstrate how nonlocality can narrow, enhance, and spectrally tune near-field emission with applications in mid-infrared sensing.

Highlights

  • Surface phonon polaritons (SPhPs) are hybrid lightmatter excitations, formed when a photon interacts with the optical phonon modes of a polar lattice

  • In this work we have presented a full quantum theory of longitudinal transverse polaritons, derived directly from consideration of the free fields in an inhomogeneous nonlocal medium

  • We derived equations which allow for the quantisation of longitudinal-transverse polaritons (LTPs) modes

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Summary

INTRODUCTION

Surface phonon polaritons (SPhPs) are hybrid lightmatter excitations, formed when a photon interacts with the optical phonon modes of a polar lattice. A recent series of publications has studied LTPs in more general systems, demonstrating them to be a general feature of polar resonators at the nanoscale [17,18,19] and a similar phenomenology has recently been observed in a Yukawa fluid [20] These works follow the approach of nonlocal plasmonics, starting from the macroscopic Maxwell equations, introducing new macroscopic fields to describe phonon modes in the lattice and matching fields at material boundaries considering the flow of energy in the system. They have been utilised to explain the emergence of anomalous modes in complex crystal hybrid structures, macroscopic systems comprised of hundreds of nanoscopic polar layers [17, 21] and have proved able to calculate the electromagnetic response.

THEORY
Field Construction
Boundary Conditions
LTP Quantisation
PURCELL ENHANCED EMISSION NEAR AN EPSILON-NEAR-ZERO WAVEGUIDE
Modes of the System
Nonlocal Purcell Enhancement
CONCLUSION
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