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The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method

We present computational studies of quasi three-dimensional nanowell (NW) and nanopost (NP) plasmonic crystals for applications in surface enhanced Raman spectroscopy (SERS). The NW and NP plasmonic crystals are metal coated arrays of cylindrical voids or posts, respectively, in a dielectric substra...

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Autores principales: Bigness, Alec, Montgomery, Jason
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5978049/
https://www.ncbi.nlm.nih.gov/pubmed/29701635
http://dx.doi.org/10.3390/ma11050672
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author Bigness, Alec
Montgomery, Jason
author_facet Bigness, Alec
Montgomery, Jason
author_sort Bigness, Alec
collection PubMed
description We present computational studies of quasi three-dimensional nanowell (NW) and nanopost (NP) plasmonic crystals for applications in surface enhanced Raman spectroscopy (SERS). The NW and NP plasmonic crystals are metal coated arrays of cylindrical voids or posts, respectively, in a dielectric substrate characterized by a well/post diameter (D), relief depth ([Formula: see text]), periodicity (P), and metal thickness ([Formula: see text]). Each plasmonic crystal is modeled using the three-dimensional finite-difference time-domain (FDTD) method with periodic boundary conditions in the x- and y-directions applied to a computational unit cell to simulate the effect of a periodic array. Relative SERS responses are calculated from time-averaged electric field intensity enhancements at [Formula: see text] and [Formula: see text] or at [Formula: see text] via [Formula: see text] or [Formula: see text] , respectively, where [Formula: see text]. Comparisons of [Formula: see text] and [Formula: see text] are made to previously reported experimental SERS measurements for NW and NP geometries. Optimized NW and NP configurations based on variations of D, P, [Formula: see text] , and [Formula: see text] using [Formula: see text] are presented, with 6× and 2× predicted increases in SERS, respectively. A novel plasmonic crystal based on square NP geometries are considered with an additional 3× increase over the optimized cylindrical NP geometry. NW geometries with imbedded spherical gold nanoparticles are considered, with 10× to 10 [Formula: see text] increases in SERS responses over the NW geometry alone. The results promote the use of FDTD as a viable in silico route to the design and optimization of SERS active devices.
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spelling pubmed-59780492018-05-31 The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method Bigness, Alec Montgomery, Jason Materials (Basel) Article We present computational studies of quasi three-dimensional nanowell (NW) and nanopost (NP) plasmonic crystals for applications in surface enhanced Raman spectroscopy (SERS). The NW and NP plasmonic crystals are metal coated arrays of cylindrical voids or posts, respectively, in a dielectric substrate characterized by a well/post diameter (D), relief depth ([Formula: see text]), periodicity (P), and metal thickness ([Formula: see text]). Each plasmonic crystal is modeled using the three-dimensional finite-difference time-domain (FDTD) method with periodic boundary conditions in the x- and y-directions applied to a computational unit cell to simulate the effect of a periodic array. Relative SERS responses are calculated from time-averaged electric field intensity enhancements at [Formula: see text] and [Formula: see text] or at [Formula: see text] via [Formula: see text] or [Formula: see text] , respectively, where [Formula: see text]. Comparisons of [Formula: see text] and [Formula: see text] are made to previously reported experimental SERS measurements for NW and NP geometries. Optimized NW and NP configurations based on variations of D, P, [Formula: see text] , and [Formula: see text] using [Formula: see text] are presented, with 6× and 2× predicted increases in SERS, respectively. A novel plasmonic crystal based on square NP geometries are considered with an additional 3× increase over the optimized cylindrical NP geometry. NW geometries with imbedded spherical gold nanoparticles are considered, with 10× to 10 [Formula: see text] increases in SERS responses over the NW geometry alone. The results promote the use of FDTD as a viable in silico route to the design and optimization of SERS active devices. MDPI 2018-04-26 /pmc/articles/PMC5978049/ /pubmed/29701635 http://dx.doi.org/10.3390/ma11050672 Text en © 2018 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Bigness, Alec
Montgomery, Jason
The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method
title The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method
title_full The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method
title_fullStr The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method
title_full_unstemmed The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method
title_short The Design and Optimization of Plasmonic Crystals for Surface Enhanced Raman Spectroscopy Using the Finite Difference Time Domain Method
title_sort design and optimization of plasmonic crystals for surface enhanced raman spectroscopy using the finite difference time domain method
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5978049/
https://www.ncbi.nlm.nih.gov/pubmed/29701635
http://dx.doi.org/10.3390/ma11050672
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