Author:
Szenes András,Vass Dávid,Bánhelyi Balázs,Csete Mária
Abstract
Plasmonic nanoresonators consisting of a gold nanorod and a spherical silica core and gold shell, both coated with a gain layer, were optimized to maximize the stimulated emission in the near-field (NF-c-type) and the outcoupling into the far-field (FF-c-type) and to enter into the spasing operation region (NF-c*-type). It was shown that in the case of a moderate dye concentration, the nanorod has more advantages: smaller lasing threshold and larger slope efficiency and larger achieved intensities in the near-field in addition to FF-c-type systems’ smaller gain and outflow threshold, earlier dip-to-peak switching in the spectrum and slightly larger far-field outcoupling efficiency. However, the near-field (far-field) bandwidth is smaller for NF-c-type (FF-c-type) core–shell nanoresonators. In the case of a larger dye concentration (NF-c*-type), although the slope efficiency and near-field intensity remain larger for the nanorod, the core–shell nanoresonator is more advantageous, considering the smaller lasing, outflow, absorption and extinction cross-section thresholds and near-field bandwidth as well as the significantly larger internal and external quantum efficiencies. It was also shown that the strong-coupling of time-competing plasmonic modes accompanies the transition from lasing to spasing occurring, when the extinction cross-section crosses zero. As a result of the most efficient enhancement in the forward direction, the most uniform far-field distribution was achieved.
Funder
National Research, Development and Innovation Office
European Social Fund
Hungarian National Laboratory program and the Eötvös Lóránd Research Network of Hungary
Subject
General Materials Science,General Chemical Engineering
Cited by
5 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献
1. Metamaterials for Enhancing Reflection and Transmission;2023 Seventeenth International Congress on Artificial Materials for Novel Wave Phenomena (Metamaterials);2023-09-11
2. Plasmonic nanoresonator distributions for uniform energy deposition in active targets;Optical Materials Express;2022-12-06
3. Energy deposition optimization via active plasmonic nanoresonator distributions;Frontiers in Optics + Laser Science 2022 (FIO, LS);2022
4. Individual plasmonic nanoresonators for lasing and spasing;Frontiers in Optics + Laser Science 2022 (FIO, LS);2022
5. Enhancement of lasing via complex plasmonic structures;Frontiers in Optics + Laser Science 2022 (FIO, LS);2022