Highly Controllable Surface Plasmon Resonance Property by Heights of Ordered Nanoparticle Arrays Fabricated via a Nonlithographic Route
Perfectly ordered nanoparticle arrays are fabricated on large-area substrates (>cm2) via a cost-effective nonlithographic route. Different surface plasmon resonance (SPR) modes focus consequently on their own positions due to the identical shape and uniform size and distance of these plasmonic me...
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Veröffentlicht in: | ACS nano 2015-04, Vol.9 (4), p.4583-4590 |
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description | Perfectly ordered nanoparticle arrays are fabricated on large-area substrates (>cm2) via a cost-effective nonlithographic route. Different surface plasmon resonance (SPR) modes focus consequently on their own positions due to the identical shape and uniform size and distance of these plasmonic metallic nanoparticles (Ag and Au). On the basis of this and FDTD (finite-difference time-domain) simulation, this work reveals the variation of all SPR parameters (position, intensity, width, and mode) with nanoparticle heights, which demonstrates that the effect of heights are different in various stages. On increasing the heights, the major dipole SPR mode precisely blue-shifts from the near-infrared to the visible region with intensity strengthening, a peak narrowing effect, and multipole modes excitation in the UV–vis range. The intensity of multipole modes can be manipulated to be equal to or even greater than the major dipole SPR mode. After coating conformal TiO2 shells on these nanoparticle arrays by atomic layer deposition, the strengthening of the SPR modes with increasing the heights results in the multiplying of the photocurrent (from ∼2.5 to a maximum 90 μA cm–2) in this plasmonic-metal–semiconductor-incorporated system. This simple but effective adjustment for all SPR parameters provides guidance for the future design of plasmonic metallic nanostructures, which is significant for SPR applications. |
doi_str_mv | 10.1021/acsnano.5b01226 |
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Different surface plasmon resonance (SPR) modes focus consequently on their own positions due to the identical shape and uniform size and distance of these plasmonic metallic nanoparticles (Ag and Au). On the basis of this and FDTD (finite-difference time-domain) simulation, this work reveals the variation of all SPR parameters (position, intensity, width, and mode) with nanoparticle heights, which demonstrates that the effect of heights are different in various stages. On increasing the heights, the major dipole SPR mode precisely blue-shifts from the near-infrared to the visible region with intensity strengthening, a peak narrowing effect, and multipole modes excitation in the UV–vis range. The intensity of multipole modes can be manipulated to be equal to or even greater than the major dipole SPR mode. After coating conformal TiO2 shells on these nanoparticle arrays by atomic layer deposition, the strengthening of the SPR modes with increasing the heights results in the multiplying of the photocurrent (from ∼2.5 to a maximum 90 μA cm–2) in this plasmonic-metal–semiconductor-incorporated system. 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Different surface plasmon resonance (SPR) modes focus consequently on their own positions due to the identical shape and uniform size and distance of these plasmonic metallic nanoparticles (Ag and Au). On the basis of this and FDTD (finite-difference time-domain) simulation, this work reveals the variation of all SPR parameters (position, intensity, width, and mode) with nanoparticle heights, which demonstrates that the effect of heights are different in various stages. On increasing the heights, the major dipole SPR mode precisely blue-shifts from the near-infrared to the visible region with intensity strengthening, a peak narrowing effect, and multipole modes excitation in the UV–vis range. The intensity of multipole modes can be manipulated to be equal to or even greater than the major dipole SPR mode. After coating conformal TiO2 shells on these nanoparticle arrays by atomic layer deposition, the strengthening of the SPR modes with increasing the heights results in the multiplying of the photocurrent (from ∼2.5 to a maximum 90 μA cm–2) in this plasmonic-metal–semiconductor-incorporated system. This simple but effective adjustment for all SPR parameters provides guidance for the future design of plasmonic metallic nanostructures, which is significant for SPR applications.</description><subject>Arrays</subject><subject>Dipoles</subject><subject>Multipoles</subject><subject>Nanostructure</subject><subject>Plasmonics</subject><subject>Plasmons</subject><subject>Strengthening</subject><subject>Titanium dioxide</subject><issn>1936-0851</issn><issn>1936-086X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp1kEtr4zAUhcXQoe_17AYtC0MSSY4le1lCOymUtvQB3RlJvmocHMtzJQ_4F8zfrkLS7GYlIX3n3HsOIT84m3Im-Ezb0OnOT3PDuBDyGznlZSYnrJDvR4d7zk_IWQhrxnJVKHlMTkRecKHE_JT8WzYfq3akC99F9G2rTQv0ZUCnLdCnVoeN7-gzBJ_GbF_Q94BxpGakS0jSGKh39BFrQKjpQ9ql1xgbm1yuEfUY6K022Fgd0_ffRlNNH3zXNnHlP1D3q8bSZz9EuCDfnW4DXO7Pc_J2e_O6WE7uH3_fLa7vJ1oUPE5s4WqjSqkyxaQpmJOFVXOVGQUgQdeKOWeltKWr83nppJGuNIpbW5usrIXKzsnVzrdH_2eAEKtNEyyk4B34IVRcScGkKOZbdLZDLfoQEFzVY7PROFacVdv2q3371b79pPi5Nx_MBuoD_1V3An7tgKSs1n7ALmX9r90ndmOTlA</recordid><startdate>20150428</startdate><enddate>20150428</enddate><creator>Zhan, Zhibing</creator><creator>Xu, Rui</creator><creator>Mi, Yan</creator><creator>Zhao, Huaping</creator><creator>Lei, Yong</creator><general>American Chemical Society</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20150428</creationdate><title>Highly Controllable Surface Plasmon Resonance Property by Heights of Ordered Nanoparticle Arrays Fabricated via a Nonlithographic Route</title><author>Zhan, Zhibing ; Xu, Rui ; Mi, Yan ; Zhao, Huaping ; Lei, Yong</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a281t-c8fdb79673706b80f68c7473b7ee6ead70ffc66c9fd549f6b6f9b71ccdb39d273</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Arrays</topic><topic>Dipoles</topic><topic>Multipoles</topic><topic>Nanostructure</topic><topic>Plasmonics</topic><topic>Plasmons</topic><topic>Strengthening</topic><topic>Titanium dioxide</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhan, Zhibing</creatorcontrib><creatorcontrib>Xu, Rui</creatorcontrib><creatorcontrib>Mi, Yan</creatorcontrib><creatorcontrib>Zhao, Huaping</creatorcontrib><creatorcontrib>Lei, Yong</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>ACS nano</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhan, Zhibing</au><au>Xu, Rui</au><au>Mi, Yan</au><au>Zhao, Huaping</au><au>Lei, Yong</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Highly Controllable Surface Plasmon Resonance Property by Heights of Ordered Nanoparticle Arrays Fabricated via a Nonlithographic Route</atitle><jtitle>ACS nano</jtitle><addtitle>ACS Nano</addtitle><date>2015-04-28</date><risdate>2015</risdate><volume>9</volume><issue>4</issue><spage>4583</spage><epage>4590</epage><pages>4583-4590</pages><issn>1936-0851</issn><eissn>1936-086X</eissn><abstract>Perfectly ordered nanoparticle arrays are fabricated on large-area substrates (>cm2) via a cost-effective nonlithographic route. Different surface plasmon resonance (SPR) modes focus consequently on their own positions due to the identical shape and uniform size and distance of these plasmonic metallic nanoparticles (Ag and Au). On the basis of this and FDTD (finite-difference time-domain) simulation, this work reveals the variation of all SPR parameters (position, intensity, width, and mode) with nanoparticle heights, which demonstrates that the effect of heights are different in various stages. On increasing the heights, the major dipole SPR mode precisely blue-shifts from the near-infrared to the visible region with intensity strengthening, a peak narrowing effect, and multipole modes excitation in the UV–vis range. The intensity of multipole modes can be manipulated to be equal to or even greater than the major dipole SPR mode. After coating conformal TiO2 shells on these nanoparticle arrays by atomic layer deposition, the strengthening of the SPR modes with increasing the heights results in the multiplying of the photocurrent (from ∼2.5 to a maximum 90 μA cm–2) in this plasmonic-metal–semiconductor-incorporated system. This simple but effective adjustment for all SPR parameters provides guidance for the future design of plasmonic metallic nanostructures, which is significant for SPR applications.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>25812724</pmid><doi>10.1021/acsnano.5b01226</doi><tpages>8</tpages></addata></record> |
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subjects | Arrays Dipoles Multipoles Nanostructure Plasmonics Plasmons Strengthening Titanium dioxide |
title | Highly Controllable Surface Plasmon Resonance Property by Heights of Ordered Nanoparticle Arrays Fabricated via a Nonlithographic Route |
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