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通过局部层加热实现硅氧氮化物薄膜中的光学二次谐波产生。

Optically modified second harmonic generation in silicon oxynitride thin films via local layer heating.

机构信息

TOPTEC Research Center, Institute of Plasma Physics of the Czech Academy of Sciences, Za Slovankou 1782/3, 182 00, Prague, Czech Republic.

Technical University of Liberec, Faculty of Mechatronics, Informatics and Interdisciplinary Studies, Studentská 1402/2, 461 17, Liberec, Czech Republic.

出版信息

Sci Rep. 2023 May 29;13(1):8658. doi: 10.1038/s41598-023-35593-8.

DOI:10.1038/s41598-023-35593-8
PMID:37248249
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10227052/
Abstract

Strong second harmonic generation (SHG) in silicon nitride has been extensively studied-among others, in terms of laser-induced SHG enhancement in SiN waveguides. This enhancement has been ascribed to the all-optical poling induced by the coherent photogalvanic effect. Yet, an analogous process for SiN thin films has not been reported. Our article reports on the observation of laser-induced threefold SHG enhancement in SiN thin films. The observed enhancement has many features similar to all-optical poling, such as highly nonlinear power dependence, cumulative effect, or connection to the SiN-Si interface. However, identical experiments for low-oxygen silicon oxynitride thin films lead to complex behavior, including laser-induced SHG reduction. Following a thorough experimental study, including the effects of repetition rate or pulse length, the observed results were ascribed to heat-induced SHG variation. In addition to revealing a new mechanism of laser-induced SHG variation, our results also provide a means to identify this mechanism.

摘要

氮化硅中的强二次谐波产生(SHG)已经得到了广泛的研究——例如,在 SiN 波导中的激光诱导 SHG 增强方面。这种增强归因于相干光电离效应引起的全光极化。然而,类似的 SiN 薄膜过程尚未有报道。我们的文章报道了在 SiN 薄膜中观察到的激光诱导三倍 SHG 增强。观察到的增强具有许多与全光极化相似的特征,例如高度非线性的功率依赖性、累积效应或与 SiN-Si 界面的连接。然而,对于低氧氮化硅薄膜的相同实验导致了复杂的行为,包括激光诱导的 SHG 减少。在进行了彻底的实验研究,包括重复率或脉冲长度的影响后,观察到的结果归因于热诱导的 SHG 变化。除了揭示激光诱导 SHG 变化的新机制外,我们的结果还提供了一种识别该机制的方法。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/40275a39b4d1/41598_2023_35593_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/96e91caa9a9a/41598_2023_35593_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/efa947c1e358/41598_2023_35593_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/5d3545dca5c3/41598_2023_35593_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/40275a39b4d1/41598_2023_35593_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/96e91caa9a9a/41598_2023_35593_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/efa947c1e358/41598_2023_35593_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/5d3545dca5c3/41598_2023_35593_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e641/10227052/40275a39b4d1/41598_2023_35593_Fig4_HTML.jpg

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