# Solvent-Mediated Eco-Friendly Synthesis and Characterization of Monodispersed Bimetallic Ag/Pd Nanocomposites for Sensing and Raman Scattering Applications

Authors: G. Sathiyadevi; B. Loganathan; B. Karthikeyan
Journal: Journal of Nanoscience
 (2014)

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## Abstract

The solvent-mediated eco-friendly monodispersed Ag/Pd bimetallic nanocomposites (BNCs) having thick core and thin shell have been prepared through novel green chemical solvent reduction method. Reducing solvent, dimethyl formamide (DMF) is employed for the controlled green synthesis. Characterization of the synthesized Ag/Pd BNCs has been done by x-ray diffraction (XRD) studies, high-resolution scanning electron microscopy (HR-SEM), energy-dispersive X-ray analysis (EDX), and high-resolution transmission electron microscopy (HR-TEM) with selected area electron diffraction (SAED) pattern. The nature of the interaction of L-cysteine with Ag/Pd BNCs has been studied by using surface plasmon spectroscopy, Fourier transform-infrared spectroscopy (FT-IR), cyclic voltammetry (CV), and theoretical methods.


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## Body

## 1. Introduction

Noble metallic nanocomposites are well known for their important applications in catalysis, biotechnology, bioengineering, surface-enhanced spectroscopy, textile engineering, nonlinear optical materials, water treatment, electronics, and optoelectronics [1–9]. However the advantage in tuning the physical and chemical properties using a bimetallic combination has triggered special interest in the synthesis and stabilization of the bimetallic over monometallic nanoparticles [10]. The bimetallic nanoparticles (BNPs) have either a core shell or different structures and the kind of this structure is decided by the method of the preparation and the control of bimetallic composition of nanoparticles. This is crucial to the improvement of essential properties of nanoparticle [11]. For instance, size-dependent core-shell Au-Ag BNPs at normal temperature had been reported [12]. Similarly, Pt-Pd BNPs having core-shell structure can be synthesized in a single-step process [13]. To validate this concept many reports were available for the synthesis of BNPs. Particularly, Ag/Pd BNCs have attracted much interest because of their superior catalytic activity in selective hydrogenation reaction [14] and the number of methods has been developed to synthesize Ag/Pd nanoparticles as a single entity [15–17].This study particularly deals with the synthesis of Ag/Pd BNPs, having core-shell structure, involving green chemical reduction of their respective metal ions using DMF as a reducing solvent. Even though the synthesis of Ag nanoparticles using DMF has already been reported [18, 19], not much is known about the BNCs. It is also equally important to analyze the interfacial properties of the BNPs; for instance, adsorption of L-cysteine molecule on the surface of Ag/Pd BNCs has also been taken into an account. Nanoparticles’ interaction with L-cysteine was reported [20–23] as sensing of L-cysteine. Among the wide range of structural variations offered by BNPs, the core-shell structure is an important one, in which one element goes to the inner core and another forms an outer shell [24–30] and the functionalization depends on the shell of the core-shell BNPs. By considering the above facts, Ag/Pd core-shell nanocomposites have been synthesized and characterized; sensing and Raman scattering applications have been presented here.


## 2. Experimental Section

### 2.1. Materials

All chemicals used were of reagent grade and used as received. Silver nitrate (AgNO3), palladium chloride (PdCl2), L-cysteine (C3H7NO2S), DMF, and distilled ethanol were purchased from Hi-Media Laboratories Pvt. Ltd. (Mumbai, India) and used as received.


### 2.2. Methods

Typically 0.02 g of AgNO3 and 50 mL of DMF were added to a beaker. Apparently the solution was turned to yellow from colourless indicating that the sol of Ag nanoparticles was formed (7 min). Then 0.02 g of PdCl2 was added to the Ag nanoparticles and shaken well to facilitate the formation of monodispersed Ag/Pd core-shell BNCs (8 min). Alcoholic solution of L-cysteine was added to Ag/Pd BNCs at the time of desired spectral studies. Scheme 1 depicts the synthetic route of the synthesis of monodispersed Ag/Pd BNCs. Synthesized sol was sonicated for 40 min to get fine dispersion of the nanoparticles with a “fast-clean” ultrasonic cleaner. Then, it was used for characterization studies. For surface-enhanced Raman spectroscopic (SERS) measurement, 1 mM of L-cysteine solution was used. The L-cysteine solution was added to as-synthesized sol at the time of desired spectral analysis.Scheme 1
Schematic representation of the synthesis of solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites.


### 2.3. Characterization

UV-vis (ultraviolet and visible light) absorbance spectra were recorded over a range of 800–200 nm with a Shimadzu UV-1650 PC spectrophotometer, operated at a resolution of 0.5 nm. The samples were filled in a quartz cuvette of 1 cm light-path length, and the light absorption spectra were given in reference to DMF.Fourier transform-infrared spectra (FT-IR) were recorded using AVATAR 330 FT-IR spectrometer in KBr pellet.Wide-angle powder X-ray diffraction (XRD) pattern was recorded with XPERT-PRO diffractometer equipped with monochromatic Cu Kα radiation by using a single-step scan program.The morphology of the colloidal sample was examined using a JEOL 3010 high-resolution transmission electron microscope (HR-TEM), with an ultra-high-resolution (UHR) pole piece operating at an accelerating voltage of 300 kV and FEI Quanta FEG 200 high-resolution scanning electron microscope (HR-SEM), with an energy-dispersive X-ray (EDX) accessory operating at an accelerating voltage of 30 kV. Sample for HR-TEM characterization was prepared by depositing a drop of the colloid on a carbon-coated Cu grid and allowing it to evaporate.FT-Raman spectra were recorded with an integral microscope Raman system RFS 27 spectrometer equipped with 1024 × 256 pixels liquefied nitrogen-cooled germanium detector. The 1064 nm line of the Nd : YAG laser (red laser) was used to excite the Raman spectra. Each spectrum was recorded with an acquisition time of 18 sec. The synthesized bimetallic sol was activated by the addition of 2 M sodium chloride to promote the aggregation.


### 2.4. Electrochemical Investigations

Cyclic voltammograms (CVs) were performed by using CHI 604 C electrochemical work station. A standard three-electrode system was used to contain Ag/AgCl reference electrode, a platinum wire as an auxiliary electrode, and the modified glassy carbon electrode (GCE) as the working electrode. Before the experiment, the GCE was polished with 1 micron alpha alumina powder, 0.3 micron alpha alumina powder, and 0.05 micron gamma alumina powder. About 1 mL of Ag/Pd BNCs was added to a beaker containing 1 mL of distilled ethanol and sonicated for about 20 min. Subsequently the mixture was pipetted out onto the surface of GCE by using capillary tube and allowed to dry for 30 min at room temperature, with the simultaneous evaporation of residual ethanol, and a secondary membrane of Nafion perfluorinated ion-exchange resin was coated onto the GCE surface and then dried to 15 min. Thus the coated Nafion membrane helps the loaded sol to stick to the electrode surface and works as a proton exchange membrane. All electrocatalytic solutions were deaerated with nitrogen atmosphere before performing the CV measurements.


### 2.5. Theoretical Calculations

The density functional calculation (DFT) presented here was performed with the Gaussian-03 W program on a Pentium (IV) computer system. The molecular geometry of L-cysteine-Pd surface complex model was optimized using the method B3LYP with the basis set of Lanl2DZ. A complete geometry optimization was carried out employing Berny’s optimization algorithm, which resulted in CS symmetry. The vibrational frequencies and the corresponding normal modes were then evaluated at the optimized geometry using analytical differentiation algorithms contained within the program.


## 2.1. Materials

All chemicals used were of reagent grade and used as received. Silver nitrate (AgNO3), palladium chloride (PdCl2), L-cysteine (C3H7NO2S), DMF, and distilled ethanol were purchased from Hi-Media Laboratories Pvt. Ltd. (Mumbai, India) and used as received.


## 2.2. Methods

Typically 0.02 g of AgNO3 and 50 mL of DMF were added to a beaker. Apparently the solution was turned to yellow from colourless indicating that the sol of Ag nanoparticles was formed (7 min). Then 0.02 g of PdCl2 was added to the Ag nanoparticles and shaken well to facilitate the formation of monodispersed Ag/Pd core-shell BNCs (8 min). Alcoholic solution of L-cysteine was added to Ag/Pd BNCs at the time of desired spectral studies. Scheme 1 depicts the synthetic route of the synthesis of monodispersed Ag/Pd BNCs. Synthesized sol was sonicated for 40 min to get fine dispersion of the nanoparticles with a “fast-clean” ultrasonic cleaner. Then, it was used for characterization studies. For surface-enhanced Raman spectroscopic (SERS) measurement, 1 mM of L-cysteine solution was used. The L-cysteine solution was added to as-synthesized sol at the time of desired spectral analysis.Scheme 1
Schematic representation of the synthesis of solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites.


## 2.3. Characterization

UV-vis (ultraviolet and visible light) absorbance spectra were recorded over a range of 800–200 nm with a Shimadzu UV-1650 PC spectrophotometer, operated at a resolution of 0.5 nm. The samples were filled in a quartz cuvette of 1 cm light-path length, and the light absorption spectra were given in reference to DMF.Fourier transform-infrared spectra (FT-IR) were recorded using AVATAR 330 FT-IR spectrometer in KBr pellet.Wide-angle powder X-ray diffraction (XRD) pattern was recorded with XPERT-PRO diffractometer equipped with monochromatic Cu Kα radiation by using a single-step scan program.The morphology of the colloidal sample was examined using a JEOL 3010 high-resolution transmission electron microscope (HR-TEM), with an ultra-high-resolution (UHR) pole piece operating at an accelerating voltage of 300 kV and FEI Quanta FEG 200 high-resolution scanning electron microscope (HR-SEM), with an energy-dispersive X-ray (EDX) accessory operating at an accelerating voltage of 30 kV. Sample for HR-TEM characterization was prepared by depositing a drop of the colloid on a carbon-coated Cu grid and allowing it to evaporate.FT-Raman spectra were recorded with an integral microscope Raman system RFS 27 spectrometer equipped with 1024 × 256 pixels liquefied nitrogen-cooled germanium detector. The 1064 nm line of the Nd : YAG laser (red laser) was used to excite the Raman spectra. Each spectrum was recorded with an acquisition time of 18 sec. The synthesized bimetallic sol was activated by the addition of 2 M sodium chloride to promote the aggregation.


## 2.4. Electrochemical Investigations

Cyclic voltammograms (CVs) were performed by using CHI 604 C electrochemical work station. A standard three-electrode system was used to contain Ag/AgCl reference electrode, a platinum wire as an auxiliary electrode, and the modified glassy carbon electrode (GCE) as the working electrode. Before the experiment, the GCE was polished with 1 micron alpha alumina powder, 0.3 micron alpha alumina powder, and 0.05 micron gamma alumina powder. About 1 mL of Ag/Pd BNCs was added to a beaker containing 1 mL of distilled ethanol and sonicated for about 20 min. Subsequently the mixture was pipetted out onto the surface of GCE by using capillary tube and allowed to dry for 30 min at room temperature, with the simultaneous evaporation of residual ethanol, and a secondary membrane of Nafion perfluorinated ion-exchange resin was coated onto the GCE surface and then dried to 15 min. Thus the coated Nafion membrane helps the loaded sol to stick to the electrode surface and works as a proton exchange membrane. All electrocatalytic solutions were deaerated with nitrogen atmosphere before performing the CV measurements.


## 2.5. Theoretical Calculations

The density functional calculation (DFT) presented here was performed with the Gaussian-03 W program on a Pentium (IV) computer system. The molecular geometry of L-cysteine-Pd surface complex model was optimized using the method B3LYP with the basis set of Lanl2DZ. A complete geometry optimization was carried out employing Berny’s optimization algorithm, which resulted in CS symmetry. The vibrational frequencies and the corresponding normal modes were then evaluated at the optimized geometry using analytical differentiation algorithms contained within the program.


## 3. Results and Discussion

### 3.1. X-Ray Diffraction (XRD) Analysis

Figure1 depicts the XRD pattern of the solvent-mediated monodispersed Ag/Pd BNCs. The XRD showed a diffraction at 2
θ
=
45.35° (sharp). It suggests that the prepared BNCs were small-sized and of face-centered cubic (fcc) structure. The reflection peaks appeared at 2
θ
=
38.98°, 45.19°, 66.07°, and 76.67° ascribed to Ag (1 1 1), Pd (2 0 0), Ag (3 1 1), and Ag (2 0 0) planes, respectively. The sizes of BNCs were calculated by using Scherrer’s equation [26, 28, 29] and were found to be ~6 nm in size. Table 1 shows the calculated size of crystalline nanoparticles and the identified crystal planes.Table 1
Crystalline size and identification of monodispersed Ag/Pd BNCs.
S. number
2θ (°)
d spacing (Å)
FWHM
Miller’s indices
Crystalline size (nm)
1
38.98
2.3085
0.41
1 1 1 (Ag)
3.83
2
45.35
1.9980
0.44
2 0 0 (Pd)
4.26
3
66.07
1.4131
0.35
2 0 0 (Ag)
6.64
4
76.67
1.2419
0.15
3 1 1 (Ag)
8.11Figure 1
X-ray diffraction (XRD) pattern of solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites.


### 3.2. High-Resolution Scanning Electron Microscopy (HR-SEM) and Energy-Dispersive X-Ray (EDX) Spectroscopic Analysis

Figure2 represents the HR-SEM images and EDX analysis of the solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites. The core-shell thin-shell-like structure of the synthesized Ag/Pd BNCs is clearly visible in Figures 2(a)–2(c). The EDX analysis (Figure 2(d)) of Ag/Pd BNCs reveals a higher concentration of palladium on the surface suggesting the formation of Pd shell (70% of Pd by weight and core of about 30% of Ag by weight).((a)–(c)) The high-resolution scanning electron microscopy (HR-SEM) images of bimetallic Ag/Pd core-shell nanocomposites.Scale bars: ((a)–(c)) 200 nm. (d) Energy-dispersive X-ray (EDX) elemental mapping of bimetallic Ag/Pd core-shell nanocomposites.
(a)
(b)
(c)
(d)


### 3.3. High-Resolution Transmission Electron Microscopic (HR-TEM) Analysis

HR-TEM images of the solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites are shown in Figure3, along with the particle size distribution histogram. Successive reduction strategy yields highly uniform monodispersed spherical core-shell BNCs (Figures 3(a)-3(b)). The size distributions were very narrow as shown in the histogram (Figure 3(c)). The SAED pattern (Figure 3(d)) reveals the diffraction rings from core to shell which are indexed as (1 1 1), (2 0 0), (2 0 0), and (3 1 1) confirming the fcc structure of Ag/Pd BNCs.((a)-(b)) High-resolution transmission electron microscopy (HR-TEM) images of bimetallic Ag/Pd core-shell nanocomposites.Scale bars: (a) 200 nm, (b) 10 nm. (c) Selected area electron diffraction(SAED) pattern of bimetallic Ag/Pd core-shell nanocomposites. (d) Particle size distribution histogram of bimetallic Ag/Pd core-shell nanocomposites.
(a)
(b)
(c)
(d)


### 3.4. UV-Visible Spectral Studies

The absorption spectrum of solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites exhibits a clear single absorbance at 482 nm (Figure4(a)). Furthermore the addition of L-cysteine reduced the intensity of surface plasmon with respect to time and the observed red shift is ascribed to the aggregation of BNCs in the presence of L-cysteine (Figure 4(b)). From the above observations it is concluded that the L-cysteine molecules are functionalized on the BNCs surface. This phenomenon was used for the further preparation of L-cysteine functionalized of Ag/Pd core-shell nanocomposites.Figure 4
(a) UV-visible absorption spectrum of bimetallic Ag/Pd core-shell nanocomposites and (b) absorption of L-cysteine on bimetallic Ag/Pd core-shell nanocomposites.


### 3.5. Fourier Transform-Infrared (FT-IR) Analysis

The vibrational features of L-cysteine adsorbed Ag/Pd core-shell BNCs were examined by comparing FT-IR spectrum of L-cysteine (Figure5(a)), L-cysteine adsorbed Ag/Pd BNCs (Figure 5(b)), and only Ag/Pd BNCs (Figure 5(c)). When L-cysteine molecule attached to the surface of free BNCs, the vibrational frequencies originating from the functional groups of L-cysteine were expected to shift accordingly. In L-cysteine, the important stretching vibrational modes are assigned as follows: –NH stretching (3180 cm−1), symmetric stretching vibration of –CH (2964 cm−1), –SH (2554 cm−1), and –NH bending vibration (1587 cm−1). The –SH stretching in the L-cysteine is found to be absent in the Ag/Pd-L-cysteine surface complex which indicates the attachment of–SH group of L-cysteine on the surface of Ag/Pd core-shell BNCs. The assignments were made by the computed IR spectrum of the L-cysteine-Pd surface complex (Figure 5(d)) theoretical model (Figure 6). The possible assignments of FT-IR frequencies of L-cysteine and L-cysteine functionalized Ag/Pd BNCs along with their computed vibrational frequencies are compiled in Table 2.Table 2
The possible assignments of FT-IR frequencies of L-cysteine and L-cysteine functionalized Ag/Pd BNCs along with their computed vibrational frequencies (cm−1).
FT-IR frequencies of L-cysteine (cm−1)
Computed vibrational frequencies (cm−1)
L-cysteine functionalized Ag/Pd BNPs (cm−1)
Possible assignments
538
591
—
CC str
637
—
607
CS str
692
670
670
CS str
821
853
803
CO2bend
—
916
954
CC sym
1008
—
1011
NH2 bend
1063
1097
1100
CN str
1203
1202
1201
CH2 str
1296
1226
1247
CH2 wagg
1346
—
1355
CO2 str
1393
1395
1399
COO− str
1423
1401
1414
CH2 bend
1587
1594
—
NH bend
2554
—
—
SH str
2964
—
—
CH sym.str
3180
3205
3235
NH str
3430
3435
3488
OH strFigure 5
(a) Fourier transmission-infrared (FT-IR) spectrum of L-cysteine, (b) L-cysteine adsorbed Ag/Pd core-shell nanocomposites, (c) Ag/Pd BNCs, and (d) computed FT-IR spectrum of the L-cysteine-Pd surface complex.Figure 6
L-cysteine-Pd surface complex model.


### 3.6. Cyclic Voltammetry-Electrochemical Sensing

Figure7 represents cyclic voltammograms of L-cysteine at the Ag-Pd/GCE in 0.1 M KCl recorded in the absence (curve a) and presence (curve b) of 0.2 M L-cysteine at the scan rate of 50 mVs−1. A well-defined anodic peak at 0.68 V in the CV is attributed to the L-cysteine oxidation. There is no reduction peak in the reverse scan of the potential window −0.2 to 0.l V revealing that the process is chemically irreversible. Electrooxidation of L-cysteine involves a strong interaction of the sulphur atom with an active site on the electrode surface having noble metals [31]. This observation further confirmed that the L-cysteine functionalizes on the surface of Ag/Pd BNCs. The enhancement of anodic current may be taken as electrochemical sensing of L-cysteine. The detailed mechanism and limitations were discussed elsewhere.Figure 7
(a) Cyclic voltammogram (CV) of bimetallic Ag/Pd core-shell nanocomposites loaded on GCE and (b) CV of bimetallic Ag/Pd core-shell nanocomposites loaded on GCE in the presence of L-cysteine (2 mL).


### 3.7. Raman Scattering

The Raman spectrum of L-cysteine and the SERS of L-cysteine adsorbed on BNCs are given in Figure8. Frequencies were shifted and showed variable intensities with the normal Raman spectrum. C-S frequency can be assigned to 665 cm−1, where this mode is assigned at 690 cm−1 in the solution. But in SERS C-S frequency is located at 696 cm−1. This shift indicates that the sulphur atom of L-cysteine may be directly bonded to the Pd metal. Another aspect in the SERS spectrum is the absence of S-H stretching vibration frequency, which appears at 2554 cm−1 in the normal Raman spectrum, indicating the definite involvement of the sulphur atom.Figure 8
(a) Raman spectrum of 1 mM of aqueous L-cysteine and (b) surface-enhanced Raman scattering (SERS) of 1 mM of L-cysteine adsorbed on Ag/Pd BNCs.


## 3.1. X-Ray Diffraction (XRD) Analysis

Figure1 depicts the XRD pattern of the solvent-mediated monodispersed Ag/Pd BNCs. The XRD showed a diffraction at 2
θ
=
45.35° (sharp). It suggests that the prepared BNCs were small-sized and of face-centered cubic (fcc) structure. The reflection peaks appeared at 2
θ
=
38.98°, 45.19°, 66.07°, and 76.67° ascribed to Ag (1 1 1), Pd (2 0 0), Ag (3 1 1), and Ag (2 0 0) planes, respectively. The sizes of BNCs were calculated by using Scherrer’s equation [26, 28, 29] and were found to be ~6 nm in size. Table 1 shows the calculated size of crystalline nanoparticles and the identified crystal planes.Table 1
Crystalline size and identification of monodispersed Ag/Pd BNCs.
S. number
2θ (°)
d spacing (Å)
FWHM
Miller’s indices
Crystalline size (nm)
1
38.98
2.3085
0.41
1 1 1 (Ag)
3.83
2
45.35
1.9980
0.44
2 0 0 (Pd)
4.26
3
66.07
1.4131
0.35
2 0 0 (Ag)
6.64
4
76.67
1.2419
0.15
3 1 1 (Ag)
8.11Figure 1
X-ray diffraction (XRD) pattern of solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites.


## 3.2. High-Resolution Scanning Electron Microscopy (HR-SEM) and Energy-Dispersive X-Ray (EDX) Spectroscopic Analysis

Figure2 represents the HR-SEM images and EDX analysis of the solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites. The core-shell thin-shell-like structure of the synthesized Ag/Pd BNCs is clearly visible in Figures 2(a)–2(c). The EDX analysis (Figure 2(d)) of Ag/Pd BNCs reveals a higher concentration of palladium on the surface suggesting the formation of Pd shell (70% of Pd by weight and core of about 30% of Ag by weight).((a)–(c)) The high-resolution scanning electron microscopy (HR-SEM) images of bimetallic Ag/Pd core-shell nanocomposites.Scale bars: ((a)–(c)) 200 nm. (d) Energy-dispersive X-ray (EDX) elemental mapping of bimetallic Ag/Pd core-shell nanocomposites.
(a)
(b)
(c)
(d)


## 3.3. High-Resolution Transmission Electron Microscopic (HR-TEM) Analysis

HR-TEM images of the solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites are shown in Figure3, along with the particle size distribution histogram. Successive reduction strategy yields highly uniform monodispersed spherical core-shell BNCs (Figures 3(a)-3(b)). The size distributions were very narrow as shown in the histogram (Figure 3(c)). The SAED pattern (Figure 3(d)) reveals the diffraction rings from core to shell which are indexed as (1 1 1), (2 0 0), (2 0 0), and (3 1 1) confirming the fcc structure of Ag/Pd BNCs.((a)-(b)) High-resolution transmission electron microscopy (HR-TEM) images of bimetallic Ag/Pd core-shell nanocomposites.Scale bars: (a) 200 nm, (b) 10 nm. (c) Selected area electron diffraction(SAED) pattern of bimetallic Ag/Pd core-shell nanocomposites. (d) Particle size distribution histogram of bimetallic Ag/Pd core-shell nanocomposites.
(a)
(b)
(c)
(d)


## 3.4. UV-Visible Spectral Studies

The absorption spectrum of solvent-mediated monodispersed bimetallic Ag/Pd core-shell nanocomposites exhibits a clear single absorbance at 482 nm (Figure4(a)). Furthermore the addition of L-cysteine reduced the intensity of surface plasmon with respect to time and the observed red shift is ascribed to the aggregation of BNCs in the presence of L-cysteine (Figure 4(b)). From the above observations it is concluded that the L-cysteine molecules are functionalized on the BNCs surface. This phenomenon was used for the further preparation of L-cysteine functionalized of Ag/Pd core-shell nanocomposites.Figure 4
(a) UV-visible absorption spectrum of bimetallic Ag/Pd core-shell nanocomposites and (b) absorption of L-cysteine on bimetallic Ag/Pd core-shell nanocomposites.


## 3.5. Fourier Transform-Infrared (FT-IR) Analysis

The vibrational features of L-cysteine adsorbed Ag/Pd core-shell BNCs were examined by comparing FT-IR spectrum of L-cysteine (Figure5(a)), L-cysteine adsorbed Ag/Pd BNCs (Figure 5(b)), and only Ag/Pd BNCs (Figure 5(c)). When L-cysteine molecule attached to the surface of free BNCs, the vibrational frequencies originating from the functional groups of L-cysteine were expected to shift accordingly. In L-cysteine, the important stretching vibrational modes are assigned as follows: –NH stretching (3180 cm−1), symmetric stretching vibration of –CH (2964 cm−1), –SH (2554 cm−1), and –NH bending vibration (1587 cm−1). The –SH stretching in the L-cysteine is found to be absent in the Ag/Pd-L-cysteine surface complex which indicates the attachment of–SH group of L-cysteine on the surface of Ag/Pd core-shell BNCs. The assignments were made by the computed IR spectrum of the L-cysteine-Pd surface complex (Figure 5(d)) theoretical model (Figure 6). The possible assignments of FT-IR frequencies of L-cysteine and L-cysteine functionalized Ag/Pd BNCs along with their computed vibrational frequencies are compiled in Table 2.Table 2
The possible assignments of FT-IR frequencies of L-cysteine and L-cysteine functionalized Ag/Pd BNCs along with their computed vibrational frequencies (cm−1).
FT-IR frequencies of L-cysteine (cm−1)
Computed vibrational frequencies (cm−1)
L-cysteine functionalized Ag/Pd BNPs (cm−1)
Possible assignments
538
591
—
CC str
637
—
607
CS str
692
670
670
CS str
821
853
803
CO2bend
—
916
954
CC sym
1008
—
1011
NH2 bend
1063
1097
1100
CN str
1203
1202
1201
CH2 str
1296
1226
1247
CH2 wagg
1346
—
1355
CO2 str
1393
1395
1399
COO− str
1423
1401
1414
CH2 bend
1587
1594
—
NH bend
2554
—
—
SH str
2964
—
—
CH sym.str
3180
3205
3235
NH str
3430
3435
3488
OH strFigure 5
(a) Fourier transmission-infrared (FT-IR) spectrum of L-cysteine, (b) L-cysteine adsorbed Ag/Pd core-shell nanocomposites, (c) Ag/Pd BNCs, and (d) computed FT-IR spectrum of the L-cysteine-Pd surface complex.Figure 6
L-cysteine-Pd surface complex model.


## 3.6. Cyclic Voltammetry-Electrochemical Sensing

Figure7 represents cyclic voltammograms of L-cysteine at the Ag-Pd/GCE in 0.1 M KCl recorded in the absence (curve a) and presence (curve b) of 0.2 M L-cysteine at the scan rate of 50 mVs−1. A well-defined anodic peak at 0.68 V in the CV is attributed to the L-cysteine oxidation. There is no reduction peak in the reverse scan of the potential window −0.2 to 0.l V revealing that the process is chemically irreversible. Electrooxidation of L-cysteine involves a strong interaction of the sulphur atom with an active site on the electrode surface having noble metals [31]. This observation further confirmed that the L-cysteine functionalizes on the surface of Ag/Pd BNCs. The enhancement of anodic current may be taken as electrochemical sensing of L-cysteine. The detailed mechanism and limitations were discussed elsewhere.Figure 7
(a) Cyclic voltammogram (CV) of bimetallic Ag/Pd core-shell nanocomposites loaded on GCE and (b) CV of bimetallic Ag/Pd core-shell nanocomposites loaded on GCE in the presence of L-cysteine (2 mL).


## 3.7. Raman Scattering

The Raman spectrum of L-cysteine and the SERS of L-cysteine adsorbed on BNCs are given in Figure8. Frequencies were shifted and showed variable intensities with the normal Raman spectrum. C-S frequency can be assigned to 665 cm−1, where this mode is assigned at 690 cm−1 in the solution. But in SERS C-S frequency is located at 696 cm−1. This shift indicates that the sulphur atom of L-cysteine may be directly bonded to the Pd metal. Another aspect in the SERS spectrum is the absence of S-H stretching vibration frequency, which appears at 2554 cm−1 in the normal Raman spectrum, indicating the definite involvement of the sulphur atom.Figure 8
(a) Raman spectrum of 1 mM of aqueous L-cysteine and (b) surface-enhanced Raman scattering (SERS) of 1 mM of L-cysteine adsorbed on Ag/Pd BNCs.


## 4. Conclusion

Solvent-mediated eco-friendly monodispersed bimetallic Ag/Pd core-shell nanocomposites were successfully synthesized using DMF without any form of heating, a solvent which facilitates the formation of monodispersed BNCs. The BNCs were characterized by techniques such as XRD, HR-SEM, EDX, and HR-TEM. The obtained results confirmed that the as-synthesized BNCs possess a core shell having thick core and thin shell structure. The adsorption of L-cysteine on the bimetallic core-shell surface was ascertained by using FT-IR, Raman, UV-visible, CV, and DFT calculations. The present study showed the synthesis of Ag/Pd core-shell BNCs by the solvent controlled green reduction and the L-cysteine functionalised BNCs.



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