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通过二元光刻和回流(BLR)扩大多光谱滤色器规模。

Scaling up multispectral color filters with binary lithography and reflow (BLR).

作者信息

Rahman Md Abdur, Rezaei Soroosh Daqiqeh, Arora Deepshikha, Wang Hao, Mori Tomohiro, Chia Ser Chern, Chan John You En, Nair Parvathi Nair Suseela, Uddin Siam, Pan Cheng-Feng, Zhang Wang, Wang Hongtao, Ruitao Zheng, Heng Lim Sin, Yang Joel K W

机构信息

Engineering Product Development Pillar, Singapore University of Technology and Design, 8 Somapah Road, Singapore 487372, Singapore.

Industrial Technology Center of Wakayama Prefecture, Wakayama 6496261, Japan.

出版信息

Nanophotonics. 2024 Jun 3;13(19):3671-3677. doi: 10.1515/nanoph-2024-0090. eCollection 2024 Aug.

DOI:10.1515/nanoph-2024-0090
PMID:39635033
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11465983/
Abstract

Efforts to increase the number of filters are driven by the demand for miniaturized spectrometers and multispectral imaging. However, processes that rely on sequential fabrication of each filter are cost ineffective. Herein, we introduce an approach to produce at least 16 distinct filters based on a single low-resolution lithographic step with minimum feature size of 0.6 μm. Distinct from grayscale lithography, we employ standard binary lithography but achieve height variations in polymeric resist through a post-development reflow process. The resulting transparent polymeric films were incorporated in Fabry-Perot cavity structures with cavity thickness ranging from 90 to 230 nm to produce transmittance across the visible spectrum. This binary lithography and reflow (BLR) process demonstrates control of the dielectric layer thickness down to ∼15 nm. This new process provides a cost-effective alternative to traditional techniques in fabricating microscopic transmission filters, and other applications where precise thickness variation across the substrate is required.

摘要

增加滤光片数量的努力是由对小型化光谱仪和多光谱成像的需求推动的。然而,依赖于逐个滤光片顺序制造的工艺成本效益不高。在此,我们介绍一种方法,基于单个低分辨率光刻步骤,最小特征尺寸为0.6μm,可生产至少16种不同的滤光片。与灰度光刻不同,我们采用标准二元光刻,但通过显影后回流工艺实现聚合物抗蚀剂中的高度变化。将所得的透明聚合物薄膜并入法布里-珀罗腔结构中,腔厚度范围为90至230nm,以产生整个可见光谱的透射率。这种二元光刻和回流(BLR)工艺展示了对低至约15nm的介电层厚度的控制。这种新工艺为制造微观透射滤光片以及其他需要在整个基板上精确控制厚度变化的应用提供了一种具有成本效益的传统技术替代方案。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/230e223e2079/j_nanoph-2024-0090_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/6e9c40d27413/j_nanoph-2024-0090_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/528cdab3fb74/j_nanoph-2024-0090_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/80261480fda7/j_nanoph-2024-0090_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/230e223e2079/j_nanoph-2024-0090_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/6e9c40d27413/j_nanoph-2024-0090_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/528cdab3fb74/j_nanoph-2024-0090_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/80261480fda7/j_nanoph-2024-0090_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8911/11465983/230e223e2079/j_nanoph-2024-0090_fig_004.jpg

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