Metallo-Dielectric Colloidal Films as SERS Substrate

A. L. González, Arturo Gomez, M. Toledo-Solano
{"title":"Metallo-Dielectric Colloidal Films as SERS Substrate","authors":"A. L. González, Arturo Gomez, M. Toledo-Solano","doi":"10.5772/intechopen.90313","DOIUrl":null,"url":null,"abstract":"Along this chapter, we probe that the discrete dipole approximation models fairly well the optical response of periodic systems. Herein, we use it to model the reflectance and transmittance, at normal incidence, of colloidal films made of SiO 2 spheres. As the thickness increases from 1 to 12 layers, the photonic band gap shifts to the blue tending to the value corresponding to a 3D opal, 442 nm. A film with more than eight layers resembles the bulk properties of a 3D opal. Our results are compared to a real sample. Besides, we show that taking advantage of the wide and asymmetrical absorbance spectrum of an opal with Au NPs is possible to identify the contribution of each component in the overall spectrum, through a deconvolution analysis. Finally, we present the electric field intensity as the content of metal NP increases in a monolayer. We consider NPs one order of magnitude smaller than the silica spheres, and then, 6, 9, and 17 NPs are hosted in the void. Similar average electric field intensities, about 11 times the incident intensity, are obtained with Au and Ag NPs. But, the spots with these intensities cover a bigger area with Ag NPs than with Au NPs. and transmittance, at normal incidence, of colloidal films made of SiO 2 spheres with a specific diameter of 200 nm. We show that as the thickness increases from 1 to 12 layers, the center of the photonic band gap shifts to the blue tending to the value of 444 nm. This value is very close to the one corresponding to a 3D opal with HCP structure, 442 nm. Analyzing the trend of the position of the BG, a film with more than eight layers resembles that of a 3D artificial opal. We also compared our results with a 3D artificial opal made with silica spheres of the same size as the one studied by us. We found a good qualitative agreement, and the differences are attributed mainly to the presence of defects in the sample.","PeriodicalId":280616,"journal":{"name":"Nanorods and Nanocomposites","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nanorods and Nanocomposites","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.5772/intechopen.90313","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2

Abstract

Along this chapter, we probe that the discrete dipole approximation models fairly well the optical response of periodic systems. Herein, we use it to model the reflectance and transmittance, at normal incidence, of colloidal films made of SiO 2 spheres. As the thickness increases from 1 to 12 layers, the photonic band gap shifts to the blue tending to the value corresponding to a 3D opal, 442 nm. A film with more than eight layers resembles the bulk properties of a 3D opal. Our results are compared to a real sample. Besides, we show that taking advantage of the wide and asymmetrical absorbance spectrum of an opal with Au NPs is possible to identify the contribution of each component in the overall spectrum, through a deconvolution analysis. Finally, we present the electric field intensity as the content of metal NP increases in a monolayer. We consider NPs one order of magnitude smaller than the silica spheres, and then, 6, 9, and 17 NPs are hosted in the void. Similar average electric field intensities, about 11 times the incident intensity, are obtained with Au and Ag NPs. But, the spots with these intensities cover a bigger area with Ag NPs than with Au NPs. and transmittance, at normal incidence, of colloidal films made of SiO 2 spheres with a specific diameter of 200 nm. We show that as the thickness increases from 1 to 12 layers, the center of the photonic band gap shifts to the blue tending to the value of 444 nm. This value is very close to the one corresponding to a 3D opal with HCP structure, 442 nm. Analyzing the trend of the position of the BG, a film with more than eight layers resembles that of a 3D artificial opal. We also compared our results with a 3D artificial opal made with silica spheres of the same size as the one studied by us. We found a good qualitative agreement, and the differences are attributed mainly to the presence of defects in the sample.
金属-介电胶体膜作为SERS衬底
在本章中,我们探讨了离散偶极子近似很好地模拟了周期系统的光学响应。在这里,我们用它来模拟由二氧化硅球制成的胶体膜在正入射下的反射率和透射率。当厚度从1层增加到12层时,光子带隙向蓝色移动,趋向于3D蛋白石对应的值,442 nm。超过八层的薄膜类似于3D蛋白石的大块特性。我们的结果与实际样本进行了比较。此外,我们表明,利用具有Au NPs的蛋白石的宽和不对称吸光度光谱,可以通过反褶积分析来确定整个光谱中每个组分的贡献。最后,我们给出了电场强度随金属NP在单层中含量的增加而变化。我们认为NPs比二氧化硅球小一个数量级,然后在空隙中有6、9和17个NPs。Au和Ag纳米粒子的平均电场强度相似,约为入射强度的11倍。但是,具有这些强度的斑点覆盖了银NPs比金NPs更大的区域。在正常入射下,由比直径为200nm的二氧化硅球制成的胶体膜的透射率。我们发现,当厚度从1层增加到12层时,光子带隙中心向蓝移,并趋向于444 nm。该值与具有HCP结构的3D蛋白石对应的值非常接近,为442 nm。分析BG位置的变化趋势,一个超过8层的膜类似于一个3D人工蛋白石。我们还将我们的结果与与我们研究的相同大小的硅球制成的3D人工蛋白石进行了比较。我们发现了很好的定性一致,差异主要归因于样品中存在缺陷。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信