Au/Ag bimetal nanogap arrays with tunable
morphologies for surface-enhanced Raman
scattering
Yaxin Wang,
a
Xiaoyu Zhao,
a
Wenting Gao,
a
Lei Chen,
a
San Chen,
c
Maobin Wei,
a
Ming Gao,
a
Cong Wang,
a
Yongjun Zhang
*
a
and Jinghai Yang
*
ab
When Au and Ag were deposited onto two-dimensional polystyrene (PS) templates, a curved bimetallic film
composed of nanocap-shaped Au/Ag units was formed. The “Y”-shaped nanogaps and “V”-shaped
junctions were tailored between the neighbour nanocaps by changing the bilayer thickness and PS
diameters. Compared to the curved Ag, the curved Au monolayer and the flat Au/Ag bilayer on a silicon
wafer, the curved Au/Ag bimetallic film exhibited significant SERS enhancement, which was mainly
attributed to two important factors, the nanogaps between the adjacent Au/Ag nanocaps and the
composite of the Ag/Au bimetallic film. And the nanogaps generated extremely intense local
electromagnetic fields and the composite provided more possibilities for the residence of probing
molecules.
1. Introduction
Surface-enhanced Raman scattering (SERS) observed in the
1970s is a phenomenon where a Raman signal is strongly
enhanced when molecules are attached to the rough surface of
metal nanostructures.
1,2
In recent years, a tremendous amount
of studies have focused on SERS due to its single-molecule
sensitivity and excellent ngerprint effect for practical applica-
tions in detection and recognition technology elds.
3–7
Currently, the development of patterned substrates with nano-
gap arrays is an important aspect of SERS studies, because
the large electromagnetic (EM) elds can be excited at the
nanogaps, termed as “hot spots”, due to the surface plasmon
resonances (SPR) of the nanostructure, which can signicantly
amplify Raman scattering intensity of the attached mole-
cules.
8–10
A variety of nanostructures with “hot spots” have been
fabricated by different approaches including chemical func-
tionalization method,
11
electron lithography technique
12
and
salt-induced aggregation.
13,14
In comparison, nanosphere
lithography (NSL) is a simple, economic and robust route for the
fabrication of a uniformly ordered nanostructure array owing to
its good monodispersity, wide size range (nanometer-to-
micrometer) and easy availability.
15–18
In addition to the construction of the substrate with high
density of hot spots, the material composition is another
key factor for SERS enhancement. Generally, SERS-active
substrates have been restricted to some noble metals mate-
rials.
19
Comparing with other noble metals, Ag and Au nano-
particles have been widely used in SERS studies due to the
higher plasmonic enhancement for Ag and better bio-
compatibility for Au.
20,21
But the toxicity of Ag and weak SERS
active of Au have limited the development of SERS spectroscopy
for the application of the single metallic substrate. To optimize
SERS effect and other optical properties, recently, a number of
studies focus on some composites or bimetal materials system,
including Au@SiO
2
, Ag/ZnO.
22,23
Au/Ag bimetal system attracts
tremendous attentions from the SERS community because it
exhibits both the dramatic Raman enhancement and good
compatibility.
24–27
The bimetal lms composed of the Ag and Au
are preferable choices for the enhancement of SERS signal and
application in analytical technique.
In this work, we fabricate the SERS-active substrate
composed of Au/Ag metallic nanogap array by NSL. The
morphologies and the properties of the metallic nanogaps are
modied by adjusting the PS diameter and the lm thickness.
The inuences of the different morphologies and the compo-
sitions of Au/Ag on Raman effects are investigated.
2. Experimental section
Assemble of PS array
The monodisperse polystyrene colloid particles (PS) were
purchased from Duke Cooperation (10 wt% aqueous solution).
The diluted polystyrene solution was applied onto the modi ed
a
Key Laboratory of Functional Materials Physics and Chemistry, Jilin Normal
University, Ministry of Education, Siping 136000, PR China. E-mail:
zhangyongjunwyx@126.com; jhyang@jlnu.edu.cn
b
Key Laboratory of Excited State Physics, Changchun Institute of Optics Fine Mechanics
and Physics, Chinese Academy of Sciences, Changchun, 130033, PR China
c
Huaibei Normal University, Huaibei, 235000, PR China
Cite this: RSC Adv.,2015,5,7454
Received 21st September 2014
Accepted 22nd December 2014
DOI: 10.1039/c4ra10882e
www.rsc.org/advances
7454 | RSC Adv.,2015,5,7454–7460 This journal is © The Royal Society of Chemistry 2015
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