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Experimental - Spectroscopy

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www.spectroscopyonline.com June 2011 <strong>Spectroscopy</strong> 26(6) 39<br />

Raman and SERS spectra were recorded<br />

with a Raman microscopic spectrometer<br />

(Renishaw RM-1000, New Mills, United<br />

Kingdom) composed of an optical microscope,<br />

a CCD video camera, and a spectrometer.<br />

A 632.8-nm HeNe laser was<br />

used as the excitation source. The SERS<br />

spectra of the probed molecules were measured<br />

with an accumulation time of 10 s<br />

using a 20× object lens. The laser power<br />

focused on the sample was ~5 mW, and the<br />

spectral resolution was set to 3 cm -1 . The<br />

analysis of the spectra for all pH values<br />

was performed by nonlinear curve fitting<br />

using Origin 7.0 software (OriginLab Corporation,<br />

Northampton, Massachusetts).<br />

Curve fitting was carried out considering<br />

the band as a Lorentzian curve.<br />

(a)<br />

(b)<br />

Results and Discussion<br />

Figure 2a shows the UV–vis absorption<br />

spectrum of the silver solution. The silver<br />

solution absorbs light at λ max<br />

= 432 nm.<br />

The absorption spectrum of methyl yellow<br />

solution (in ethanol) is shown in Figure<br />

2b. The absorption peak appears at λ max<br />

= 403 nm, which is near the absorption<br />

peak of the silver solution. Figure 2c shows<br />

the absorption spectrum of the combined<br />

system of silver solution and methyl yellow.<br />

The addition of methyl yellow to the<br />

silver solution resulted in a decreased intensity<br />

of the absorption peak, along with<br />

an appearance of a new wide band in the<br />

range of 600–800 nm resulting from the<br />

aggregated silver particles. It was found<br />

that a significant enhancement of the band<br />

intensities may be obtained when aggregates<br />

of two or more nanoparticles oscillate<br />

collectively and these collective oscillations<br />

of nanoparticles extend the range<br />

of useful localized surface plasmon effects<br />

throughout the visible and near-infrared<br />

region of the spectrum (6). The excitation<br />

wavelength of the laser, 632.8 nm, is far<br />

away from the absorption peak of methyl<br />

yellow, thus there are no surface-enhanced<br />

Raman resonance scattering components<br />

in the SERS spectra in this study. The contribution<br />

of molecular resonance to the<br />

SERS enhancement is small.<br />

Figure 3 shows the normal Raman<br />

spectrum of methyl yellow powder. Figures<br />

4 and 5 show the SERS spectra of<br />

methyl yellow in silver colloid solution<br />

with varied pH values. We have recorded<br />

SERS spectra of methyl yellow by changing<br />

the pH values in one-unit increments<br />

from 1 to 7. However, in Figures 4 and 5<br />

we have shown a few characteristic spectra.<br />

The Raman bands are labeled and the<br />

assignments of the Raman bands are listed<br />

in Table I (15,18–23).<br />

Compared with the normal Raman<br />

spectrum, the Raman signals of the molecules<br />

have been significantly enhanced<br />

in SERS. Some new bands appear in the<br />

SERS spectra, including bands at 892,<br />

997, 428, 474, 510, and 977 cm -1 (Table I).<br />

According to a unified approach to SERS<br />

(6), the presence of non-totally symmetric<br />

bands in the excitation profile indicates the<br />

presence of charge-transfer contributions<br />

to the enhancement. Although these molecules<br />

do not have enough symmetry for<br />

a definitive test of the strong changes in<br />

N<br />

N<br />

N<br />

H<br />

N<br />

Figure 1: Schematic structure of methyl yellow as (a) the azo-form in organic phase and as (b) the<br />

hydrazo-form in acidified aqueous phase.<br />

Absorbance (a.u)<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

N<br />

N<br />

CH 3<br />

CH 3<br />

CH 3<br />

CH 3<br />

(b)<br />

(a)<br />

0.0<br />

300 400 500 600 700 800<br />

Wavelength (nm)<br />

Figure 2: UV–vis absorption spectra of (a) silver solution, (b) methyl yellow solution, and (c) the<br />

combined system of silver solution and methyl yellow.<br />

(c)<br />

spectral lines, the presence of the Raman<br />

lines mentioned above in the SERS spectra<br />

indicates strong charge-transfer effects between<br />

the molecules and the silver surface.<br />

When the pH levels are varied from 4 to<br />

7, no new Raman bands appear in the SERS<br />

spectra. At pH 2 and pH 3, however, new<br />

Raman bands appear at 892 cm -1 (Figure<br />

4a), 979 cm -1 (Figure 4b), 1222 cm -1 (Figure<br />

5a), and 1492 cm -1 (Figure 5a). Although the<br />

assignments of these bands are not clear, the<br />

presence of the bands could be attributed<br />

to the vibrational modes of hydrazo form<br />

(MYH + ). MYH + is dominant when the pH<br />

of the solution is less than 3.3, the pK a<br />

of<br />

methyl yellow. The characteristic Raman<br />

bands of MYH + , 1619 and 1174 cm -1 , were<br />

observed (Figure 5a) and are attributed to<br />

υ(C=C) and υ(N-N), respectively (18).

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