Joint Workshop LANL/NIMS Quantum and Functional Materials and MANA International Symposium 2024


Session 4-1

Title

Hybrid Semiconductor and Plasmonic Nanostructures for Quantum and Coherent Multi-Photon Generation and Control

Author's photo

Authors

Andrei Piryatinski

Affiliations

Theoretical Division, Los Alamos National Laboratory

URL

https://lanlexperts.elsevierpure.com/en/persons/andrei-piryatinski

Email

apiryat@lanl.gov

Abstract

Current nanofabrication technologies enable the precise integration of semiconductor quantum emitters, such as quantum dots or nanoplatelets, with metal nanoparticles exhibiting tunable surface plasmon resonances. This integration allows for control over interaction pathways between quantum emitters and plasmonic modes, leading to new functionalities essential for on-chip optoelectronic devices.[1] A well-studied phenomenon in these hybrid materials is the acceleration of spontaneous light emission due to enhancing the photon density of states by surface plasmons, known as the plasmonic Purcell effect.[1] This talk presents theoretical studies and simulation results of optical phenomena in hybrid semiconductor-metal materials beyond the Purcell effect. Specifically, it discusses metal nanopillar arrays forming a plasmonic cavity (Inset to Fig. 1) where quantum dots experience strong coupling with collective surface lattice resonances, forming exciton-plasmon polariton states. The model calculations, supported by FDTD simulations, predict significant enhancement of second harmonic generation and second harmonic lasing above a certain exciton-plasmon coupling threshold (Fig. 1). Additionally, the study explores parametric amplification and spontaneous parametric downconversion (SPDC) in arrays of metal nanoparticles with C2v symmetry (Fig. 2a), showing that single-layer arrays of L-shaped nanoparticles can yield quantum photon production (Fig. 2b) compatible with standard SPDC sources.[3]

Fig. 1. Inset: Geometry of plasmonic lattice filled with semiconductor quantum dots forming gain medium. Main plot: Second harmonic generation efficiency indicating lasing regime above threshold.
Fig. 2. (a) Geometry of MNP subject to incident pump pulse and outgoing signal and idler photon pair. (b) Calculated energy yields vs. MNP thickness d. The inset shows yield energy distributions.

Reference

  1. J. A. Hollingsworth, H. Htoon, A. Piryatinski, S. Götzinger, and V. Sandoghdar, MRS Bulletin 40, 768 (2015). DOI: 10.1557/mrs.2015.200
  2. M. Sukharev, O. Roslyak, A. Piryatinski, J. Chem. Phys. 154, 084703 (2021). DOI: 10.1063/5.0037453
  3. S. A. Shah, M. R. Clark, J. Zyss, M. Sukharev, A. Piryatinski, Optics Lett. 49 1680, (2024). DOI: 10.1364/OL.515621