Nanosphere lithography

effect of substrate on the localized surface plasmon resonance spectrum of silver nanoparticles

Michelle Duval Malinsky, K. Lance Kelly, George C Schatz, Richard P. van Duyne

Research output: Contribution to journalArticle

385 Citations (Scopus)

Abstract

In this paper, we explore the optical contributions of the substrate to the localized surface plasmon resonance (LSPR) spectrum of surface confined Ag nanoparticles produced by nanosphere lithography (NSL). We present optical extinction spectra of Ag nanoparticles fabricated on the following substrates: fused silica, borosilicate optical glass, mica, and SF-10-a high refractive index specialty glass. For all the experiments discussed here, the Ag nanoparticles were approximately 100 nm in in-plane width and 25 nm in out-of-plane height. In a controlled N2 environment, the wavelength corresponding to the extinction maximum, λmax, shifts to the red with increasing refractive index of the substrate, nsUbstrate- The sensitivity factor, Δλmax/ΔλsUbstrate, was measured to be 87 nm per refractive index unit (RIU). Experimental extinction spectra were modeled using the discrete dipole approximation (DDA). The DBA theory qualitatively predicts the experimentally observed trend that λmax is linearly dependent on nsubstrate; however, the theory overestimates the sensitivity by approximately a factor of 2. The sensitivity of the LSPR to the refractive index of bulk external solvent, nexternal, was also examined for each of the four substrates listed above. For all the cases, the change in λmax in response to bulk external solvent was linearly dependent upon nexternal. Values of the sensitivity factors, Δλmax/Δnexternal, ranged from 206 nm RIU-1 for mica to 258 nm RIU-1 for SF-10, a difference of only 25%. From the results presented here, we conclude that there is no systematic dependence, or at most a weak dependence, which correlates the bulk solvent sensitivity of the LSPR to nsubstrate. The DDA theory overestimates the LSPR sensitivity to bulk external environment, but the ratio of solvent to substrate sensitivity factors is correct within experimental uncertainty. This ratio has a value of approximately 2, which indicates that there is greater sensitivity in the optical response to the solvent than to the substrate. This ratio is within 10% of the ratio of areas of the particles that are exposed to solvent and substrate. We suggest that chemical interactions at the interfaces between the nanoparticle and the substrate and/or the nanoparticle and the bulk environment contribute significantly to the observed difference between experimental and theoretical sensitivity factors.

Original languageEnglish
Pages (from-to)2343-2350
Number of pages8
JournalJournal of Physical Chemistry B
Volume105
Issue number12
Publication statusPublished - Mar 29 2001

Fingerprint

Nanospheres
Surface plasmon resonance
Silver
surface plasmon resonance
Lithography
lithography
silver
Nanoparticles
nanoparticles
sensitivity
Refractive index
Substrates
refractivity
extinction
Mica
mica
dipoles
Approximation theory
Optical glass
Borosilicate glass

ASJC Scopus subject areas

  • Physical and Theoretical Chemistry

Cite this

Nanosphere lithography : effect of substrate on the localized surface plasmon resonance spectrum of silver nanoparticles. / Malinsky, Michelle Duval; Lance Kelly, K.; Schatz, George C; van Duyne, Richard P.

In: Journal of Physical Chemistry B, Vol. 105, No. 12, 29.03.2001, p. 2343-2350.

Research output: Contribution to journalArticle

Malinsky, Michelle Duval ; Lance Kelly, K. ; Schatz, George C ; van Duyne, Richard P. / Nanosphere lithography : effect of substrate on the localized surface plasmon resonance spectrum of silver nanoparticles. In: Journal of Physical Chemistry B. 2001 ; Vol. 105, No. 12. pp. 2343-2350.
@article{4faa0f458e0f4e6baf32bc6de587b646,
title = "Nanosphere lithography: effect of substrate on the localized surface plasmon resonance spectrum of silver nanoparticles",
abstract = "In this paper, we explore the optical contributions of the substrate to the localized surface plasmon resonance (LSPR) spectrum of surface confined Ag nanoparticles produced by nanosphere lithography (NSL). We present optical extinction spectra of Ag nanoparticles fabricated on the following substrates: fused silica, borosilicate optical glass, mica, and SF-10-a high refractive index specialty glass. For all the experiments discussed here, the Ag nanoparticles were approximately 100 nm in in-plane width and 25 nm in out-of-plane height. In a controlled N2 environment, the wavelength corresponding to the extinction maximum, λmax, shifts to the red with increasing refractive index of the substrate, nsUbstrate- The sensitivity factor, Δλmax/ΔλsUbstrate, was measured to be 87 nm per refractive index unit (RIU). Experimental extinction spectra were modeled using the discrete dipole approximation (DDA). The DBA theory qualitatively predicts the experimentally observed trend that λmax is linearly dependent on nsubstrate; however, the theory overestimates the sensitivity by approximately a factor of 2. The sensitivity of the LSPR to the refractive index of bulk external solvent, nexternal, was also examined for each of the four substrates listed above. For all the cases, the change in λmax in response to bulk external solvent was linearly dependent upon nexternal. Values of the sensitivity factors, Δλmax/Δnexternal, ranged from 206 nm RIU-1 for mica to 258 nm RIU-1 for SF-10, a difference of only 25{\%}. From the results presented here, we conclude that there is no systematic dependence, or at most a weak dependence, which correlates the bulk solvent sensitivity of the LSPR to nsubstrate. The DDA theory overestimates the LSPR sensitivity to bulk external environment, but the ratio of solvent to substrate sensitivity factors is correct within experimental uncertainty. This ratio has a value of approximately 2, which indicates that there is greater sensitivity in the optical response to the solvent than to the substrate. This ratio is within 10{\%} of the ratio of areas of the particles that are exposed to solvent and substrate. We suggest that chemical interactions at the interfaces between the nanoparticle and the substrate and/or the nanoparticle and the bulk environment contribute significantly to the observed difference between experimental and theoretical sensitivity factors.",
author = "Malinsky, {Michelle Duval} and {Lance Kelly}, K. and Schatz, {George C} and {van Duyne}, {Richard P.}",
year = "2001",
month = "3",
day = "29",
language = "English",
volume = "105",
pages = "2343--2350",
journal = "Journal of Physical Chemistry B",
issn = "1520-6106",
publisher = "American Chemical Society",
number = "12",

}

TY - JOUR

T1 - Nanosphere lithography

T2 - effect of substrate on the localized surface plasmon resonance spectrum of silver nanoparticles

AU - Malinsky, Michelle Duval

AU - Lance Kelly, K.

AU - Schatz, George C

AU - van Duyne, Richard P.

PY - 2001/3/29

Y1 - 2001/3/29

N2 - In this paper, we explore the optical contributions of the substrate to the localized surface plasmon resonance (LSPR) spectrum of surface confined Ag nanoparticles produced by nanosphere lithography (NSL). We present optical extinction spectra of Ag nanoparticles fabricated on the following substrates: fused silica, borosilicate optical glass, mica, and SF-10-a high refractive index specialty glass. For all the experiments discussed here, the Ag nanoparticles were approximately 100 nm in in-plane width and 25 nm in out-of-plane height. In a controlled N2 environment, the wavelength corresponding to the extinction maximum, λmax, shifts to the red with increasing refractive index of the substrate, nsUbstrate- The sensitivity factor, Δλmax/ΔλsUbstrate, was measured to be 87 nm per refractive index unit (RIU). Experimental extinction spectra were modeled using the discrete dipole approximation (DDA). The DBA theory qualitatively predicts the experimentally observed trend that λmax is linearly dependent on nsubstrate; however, the theory overestimates the sensitivity by approximately a factor of 2. The sensitivity of the LSPR to the refractive index of bulk external solvent, nexternal, was also examined for each of the four substrates listed above. For all the cases, the change in λmax in response to bulk external solvent was linearly dependent upon nexternal. Values of the sensitivity factors, Δλmax/Δnexternal, ranged from 206 nm RIU-1 for mica to 258 nm RIU-1 for SF-10, a difference of only 25%. From the results presented here, we conclude that there is no systematic dependence, or at most a weak dependence, which correlates the bulk solvent sensitivity of the LSPR to nsubstrate. The DDA theory overestimates the LSPR sensitivity to bulk external environment, but the ratio of solvent to substrate sensitivity factors is correct within experimental uncertainty. This ratio has a value of approximately 2, which indicates that there is greater sensitivity in the optical response to the solvent than to the substrate. This ratio is within 10% of the ratio of areas of the particles that are exposed to solvent and substrate. We suggest that chemical interactions at the interfaces between the nanoparticle and the substrate and/or the nanoparticle and the bulk environment contribute significantly to the observed difference between experimental and theoretical sensitivity factors.

AB - In this paper, we explore the optical contributions of the substrate to the localized surface plasmon resonance (LSPR) spectrum of surface confined Ag nanoparticles produced by nanosphere lithography (NSL). We present optical extinction spectra of Ag nanoparticles fabricated on the following substrates: fused silica, borosilicate optical glass, mica, and SF-10-a high refractive index specialty glass. For all the experiments discussed here, the Ag nanoparticles were approximately 100 nm in in-plane width and 25 nm in out-of-plane height. In a controlled N2 environment, the wavelength corresponding to the extinction maximum, λmax, shifts to the red with increasing refractive index of the substrate, nsUbstrate- The sensitivity factor, Δλmax/ΔλsUbstrate, was measured to be 87 nm per refractive index unit (RIU). Experimental extinction spectra were modeled using the discrete dipole approximation (DDA). The DBA theory qualitatively predicts the experimentally observed trend that λmax is linearly dependent on nsubstrate; however, the theory overestimates the sensitivity by approximately a factor of 2. The sensitivity of the LSPR to the refractive index of bulk external solvent, nexternal, was also examined for each of the four substrates listed above. For all the cases, the change in λmax in response to bulk external solvent was linearly dependent upon nexternal. Values of the sensitivity factors, Δλmax/Δnexternal, ranged from 206 nm RIU-1 for mica to 258 nm RIU-1 for SF-10, a difference of only 25%. From the results presented here, we conclude that there is no systematic dependence, or at most a weak dependence, which correlates the bulk solvent sensitivity of the LSPR to nsubstrate. The DDA theory overestimates the LSPR sensitivity to bulk external environment, but the ratio of solvent to substrate sensitivity factors is correct within experimental uncertainty. This ratio has a value of approximately 2, which indicates that there is greater sensitivity in the optical response to the solvent than to the substrate. This ratio is within 10% of the ratio of areas of the particles that are exposed to solvent and substrate. We suggest that chemical interactions at the interfaces between the nanoparticle and the substrate and/or the nanoparticle and the bulk environment contribute significantly to the observed difference between experimental and theoretical sensitivity factors.

UR - http://www.scopus.com/inward/record.url?scp=0035967344&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=0035967344&partnerID=8YFLogxK

M3 - Article

VL - 105

SP - 2343

EP - 2350

JO - Journal of Physical Chemistry B

JF - Journal of Physical Chemistry B

SN - 1520-6106

IS - 12

ER -