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利用金天线在硅基磷化铟微盘中实现单模发射。

Single-Mode Emission in InP Microdisks on Si Using Au Antenna.

作者信息

Tiwari Preksha, Fischer Anna, Scherrer Markus, Caimi Daniele, Schmid Heinz, Moselund Kirsten E

机构信息

IBM Research Europe-Zurich, Säumerstrasse 4, 8803 Rüschlikon, Switzerland.

出版信息

ACS Photonics. 2022 Apr 20;9(4):1218-1225. doi: 10.1021/acsphotonics.1c01677. Epub 2022 Mar 17.

DOI:10.1021/acsphotonics.1c01677
PMID:35480488
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9026291/
Abstract

An important building block for on-chip photonic applications is a scaled emitter. Whispering gallery mode cavities based on III-Vs on Si allow for small device footprints and lasing with low thresholds. However, multimodal emission and wavelength stability over a wider range of temperature can be challenging. Here, we explore the use of Au nanorod antennae on InP whispering gallery mode lasers on Si for single-mode emission. We show that by proper choice of the antenna size and positioning, we can suppress the side modes of a cavity and achieve single-mode emission over a wide excitation range. We establish emission trends by varying the size of the antenna and show that the far-field radiation pattern differs significantly for devices with and without antenna. Furthermore, the antenna-induced single-mode emission is dominant from room temperature (300 K) down to 200 K, whereas the cavity without an antenna is multimodal and its dominant emission wavelength is highly temperature-dependent.

摘要

用于片上光子应用的一个重要组成部分是缩小尺寸的发射器。基于硅上的III-V族材料的回音壁模式微腔可实现小尺寸器件以及低阈值激光发射。然而,在较宽温度范围内的多模发射和波长稳定性可能具有挑战性。在此,我们探索在硅基InP回音壁模式激光器上使用金纳米棒天线来实现单模发射。我们表明,通过适当选择天线尺寸和位置,可以抑制微腔的边模,并在很宽的激发范围内实现单模发射。我们通过改变天线尺寸确定了发射趋势,并表明有无天线的器件的远场辐射模式有显著差异。此外,天线诱导的单模发射在从室温(300 K)到200 K的温度范围内占主导,而没有天线的微腔是多模的,其主导发射波长高度依赖于温度。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/d5874d7b9365/ph1c01677_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/a6bc09a2724c/ph1c01677_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/6b72d3007048/ph1c01677_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/0f35b21f9ab7/ph1c01677_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/2c15c00cb4cb/ph1c01677_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/cb62accab93e/ph1c01677_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/d5874d7b9365/ph1c01677_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/a6bc09a2724c/ph1c01677_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/6b72d3007048/ph1c01677_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/0f35b21f9ab7/ph1c01677_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/2c15c00cb4cb/ph1c01677_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/cb62accab93e/ph1c01677_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c1f/9026291/d5874d7b9365/ph1c01677_0007.jpg

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本文引用的文献

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通过拓扑界面模式的确定性放大实现电信波段的单模激光
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