# Synthesis and Optical Characterization of Sulfonated Polyaniline/Single-Walled Carbon Nanotube/Zinc Sulphide Nanocomposite

Authors: Rajesh K. Agrawalla; Rima Paul; Amit K. Chakraborty; Apurba K. Mitra
Journal: ISRN Nanotechnology
 (2013)

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## Abstract

Polyaniline functionalized with sulfonate groups (SPANI) shows excellent solubility in water. Single-walled carbon nanotubes functionalized with carboxylic groups (f-SWCNTs) and then hybridized with freshly prepared zinc sulphide (ZnS) nanocrystals have been found to be good luminescent material with tuned emission properties. Nanocomposite of sulfonated polyaniline with embedded SWCNT/ZnS nanohybrid fibers has been prepared by a simple solution mixing process and characterized by using high resolution transmission electron microscopy (HRTEM), X-ray diffractometry, Raman spectroscopy, FTIR spectroscopy, and thermogravimetric analysis (TGA). The study of optical properties by UV-vis absorption and photoluminescence spectroscopy reveals that the composite is a luminescent material of enhanced emission intensity in the visible region of the spectrum.


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## Body

## 1. Introduction

Since their discovery by Iijima [1] in 1991, carbon nanotubes (CNTs) have shown remarkable physical properties [2]. Polyaniline (PANI) is the most studied conducting polymer in recent years due to its numerous potential applications. The CNTs have been extensively used as reinforcing fibers in PANI matrix to improve the characteristic optical and electrical properties of the polymer. The PANI/CNT composite finds application in biosensors [3], supercapacitors [4], metal-semiconductor devices [5], and actuators [6]. Zinc sulphide (ZnS) is a wide band gap compound semiconductor and has application as luminescent material [7, 8]. ZnS has been embedded in the matrix of PANI and the resulting PANI-ZnS composite has shown improved optical, electrical, and thermal properties. Dutta et al. [9] dispersed ZnS nanoparticles in PANI matrix and investigated the optical and electrical properties of the hybrid nanostructure. Pant et al. [10] studied the DC conductivity and dielectric constant of PANI-ZnS composite and found an increase in the values compared to those of pure PANI. Bompilwar et al. [11] made thermogravimetric analysis (TGA) of PANI-ZnS nanocomposite and concluded that the PANI-ZnS composites are thermally more stable than pure PANI. Singh et al. [12] prepared and characterized hybrid composite containing polyaniline, polyethylene glycol, and zinc sulfide. The photoluminescence characteristics of CNT/ZnS hybrid nanostructures have been studied by Paul et al. [13].While there are published reports on CNT-based SPANI composites [14, 15], as well as ZnS-based PANI composites [9–12, 16], to the best of our knowledge, there is no published work to date on composites of SPANI embedded with SWCNT/ZnS hybrid nanofibers. We report here a simple chemical synthesis process of a polymer composite containing SPANI with SWCNT/ZnS nanohybrid reinforcement fibers. SPANI was prepared by sulfonation of emeraldine salt of PANI through treatment with chlorosulfonic acid in an inert solvent. This composite is a promising optical material and may find potential applications in sensor and optoelectronic devices.


## 2. Experimental

### 2.1.  Materials

The SWCNTs used in our work were supplied by Chengdu Organic Chemicals Co. Ltd., China, with average diameter, length, and purity, as stated by the manufacturer, being 1-2 nm, 1–3μm, and 95 wt%, respectively. Aniline, 1,2-dichloroethane (DCE), and ammonium persulfate were supplied by Merck Specialties Pvt. Ltd., Mumbai. The chlorosulfonic acid was supplied by LOBA Chemie Pvt. Ltd., Mumbai. Except  for SWCNTs, all other chemicals were used as received without further purification.


### 2.2. Purification and Functionalization of SWCNTs

The as-received SWCNTs were purified by heating in a muffle furnace at 350°C in air for 6 h followed by soaking and stirring in 6 M HCl for 12 h. The acid-treated SWCNTs were filtered using vacuum filtration system (Millipore, pore size~0.22 μm) and washed thoroughly with deionized water. The purified SWCNTs were further treated in a mixture of concentrated HNO3/H2SO4 in 1 : 3 volume proportion for 4 h followed by washing with dilute NaOH aqueous solution and filtration with Millipore filtration apparatus until the pH became neutral, thereby attaching carboxylic acid (–COOH) groups to obtain the functionalized single-walled carbon nanotubes (f-SWCNT).


### 2.3.  Synthesis of SWCNT/ZnS Hybrid Nanostructures

We took 30 mL of zinc nitrate solution and 0.0995 gram of f-SWCNT was dispersed in it. The solution was stirred in a magnetic stirrer for 1 h at room temperature. 15 mL of methanol with sodium sulfide flakes added to it was sonicated to obtain a saturated solution which was added dropwise to the zinc nitrate solution containing SWCNTs till the pH became 7. The solution was stirred for 1 h and filtered using Whatman filter paper. The precipitate was washed with methanol followed by deionized water and filtered again. The sample was then dried under the IR lamp.


### 2.4.  Synthesis of Sulfonated Polyaniline (SPANI)

0.2 M aniline hydrochloride and 0.25 M ammonium persulfate solution were prepared and mixed in equal volumes and left overnight for polymerization to take place. The salt precipitate (PANI) was collected by filtration using a Whatman filter paper. It was then mixed with 1,2-DCE and heated to 80°C under stirring using a magnetic stirrer (REMI 2 MLH). Chlorosulfonic acid diluted with DCE was added dropwise to the reaction mixture and stirred at 80°C for 1 h. The semisolid precipitate of sulfonated polyaniline (SPANI) obtained by filtration was then mixed with 400 mL deionized water and heated to 60°C and stirred for 2 h to promote hydrolysis. The solution was further diluted with water and filtered through a cellulose membrane using a vacuum filtration system (Millipore). The final sample (SPANI) was collected over the filter membrane and dried in air at room temperature.


### 2.5.  Synthesis of SPANI/SWCNT/ZnS Composites

The SWCNT/ZnS hybrid was dispersed in deionized water and ultrasonicated. The prepared dispersion was mixed with SPANI dispersion in deionized water with constant stirring. The resulting solution was heated at 50–60°C for 2-3 hours, with stirring. Then, it was cooled and filtered using vacuum filtration system (Millipore). The sample collected by filtration was dried in air at room temperature to get SPANI/SWCNT/ZnS composite with SWCNT content of 6 wt.% and ZnS content of 7 wt.%.


### 2.6.  Characterization of the Samples

The micrographs of the sample were obtained using high resolution transmission electron microscope (HRTEM model JEOL JEM-2010; operating acceleration voltage—200 kV). The XRD patterns were obtained using Philips PANalytical X-Pert Pro diffractometer. The molecular structures of the samples were characterized by a Perkin Elmer Spectrum RX I FTIR Spectrometer. The laser source used in the spectrometer was a He-Ne laser (633 nm). Raman spectroscopy was performed using EZ-Raman-M field portable Raman analyzer (Enwave Optronics, Inc.). A diode laser of wavelength 785 nm was used as excitation source. The thermogravimetric analysis (TGA) was carried out with Perkin-Elmer Pyris- 1 TGA thermogravimetric analyzer at a heating rate of 10°C/min in nitrogen atmosphere. The optical absorbance spectra were recorded using a HITACHI U-3010 UV-visible absorption spectrophotometer. Photoluminescence spectra of the samples were acquired using a Perkin-Elmer LS-55 fluorescence spectrophotometer.The scheme of reactions is as in Scheme1.Scheme 1


## 2.1.  Materials

The SWCNTs used in our work were supplied by Chengdu Organic Chemicals Co. Ltd., China, with average diameter, length, and purity, as stated by the manufacturer, being 1-2 nm, 1–3μm, and 95 wt%, respectively. Aniline, 1,2-dichloroethane (DCE), and ammonium persulfate were supplied by Merck Specialties Pvt. Ltd., Mumbai. The chlorosulfonic acid was supplied by LOBA Chemie Pvt. Ltd., Mumbai. Except  for SWCNTs, all other chemicals were used as received without further purification.


## 2.2. Purification and Functionalization of SWCNTs

The as-received SWCNTs were purified by heating in a muffle furnace at 350°C in air for 6 h followed by soaking and stirring in 6 M HCl for 12 h. The acid-treated SWCNTs were filtered using vacuum filtration system (Millipore, pore size~0.22 μm) and washed thoroughly with deionized water. The purified SWCNTs were further treated in a mixture of concentrated HNO3/H2SO4 in 1 : 3 volume proportion for 4 h followed by washing with dilute NaOH aqueous solution and filtration with Millipore filtration apparatus until the pH became neutral, thereby attaching carboxylic acid (–COOH) groups to obtain the functionalized single-walled carbon nanotubes (f-SWCNT).


## 2.3.  Synthesis of SWCNT/ZnS Hybrid Nanostructures

We took 30 mL of zinc nitrate solution and 0.0995 gram of f-SWCNT was dispersed in it. The solution was stirred in a magnetic stirrer for 1 h at room temperature. 15 mL of methanol with sodium sulfide flakes added to it was sonicated to obtain a saturated solution which was added dropwise to the zinc nitrate solution containing SWCNTs till the pH became 7. The solution was stirred for 1 h and filtered using Whatman filter paper. The precipitate was washed with methanol followed by deionized water and filtered again. The sample was then dried under the IR lamp.


## 2.4.  Synthesis of Sulfonated Polyaniline (SPANI)

0.2 M aniline hydrochloride and 0.25 M ammonium persulfate solution were prepared and mixed in equal volumes and left overnight for polymerization to take place. The salt precipitate (PANI) was collected by filtration using a Whatman filter paper. It was then mixed with 1,2-DCE and heated to 80°C under stirring using a magnetic stirrer (REMI 2 MLH). Chlorosulfonic acid diluted with DCE was added dropwise to the reaction mixture and stirred at 80°C for 1 h. The semisolid precipitate of sulfonated polyaniline (SPANI) obtained by filtration was then mixed with 400 mL deionized water and heated to 60°C and stirred for 2 h to promote hydrolysis. The solution was further diluted with water and filtered through a cellulose membrane using a vacuum filtration system (Millipore). The final sample (SPANI) was collected over the filter membrane and dried in air at room temperature.


## 2.5.  Synthesis of SPANI/SWCNT/ZnS Composites

The SWCNT/ZnS hybrid was dispersed in deionized water and ultrasonicated. The prepared dispersion was mixed with SPANI dispersion in deionized water with constant stirring. The resulting solution was heated at 50–60°C for 2-3 hours, with stirring. Then, it was cooled and filtered using vacuum filtration system (Millipore). The sample collected by filtration was dried in air at room temperature to get SPANI/SWCNT/ZnS composite with SWCNT content of 6 wt.% and ZnS content of 7 wt.%.


## 2.6.  Characterization of the Samples

The micrographs of the sample were obtained using high resolution transmission electron microscope (HRTEM model JEOL JEM-2010; operating acceleration voltage—200 kV). The XRD patterns were obtained using Philips PANalytical X-Pert Pro diffractometer. The molecular structures of the samples were characterized by a Perkin Elmer Spectrum RX I FTIR Spectrometer. The laser source used in the spectrometer was a He-Ne laser (633 nm). Raman spectroscopy was performed using EZ-Raman-M field portable Raman analyzer (Enwave Optronics, Inc.). A diode laser of wavelength 785 nm was used as excitation source. The thermogravimetric analysis (TGA) was carried out with Perkin-Elmer Pyris- 1 TGA thermogravimetric analyzer at a heating rate of 10°C/min in nitrogen atmosphere. The optical absorbance spectra were recorded using a HITACHI U-3010 UV-visible absorption spectrophotometer. Photoluminescence spectra of the samples were acquired using a Perkin-Elmer LS-55 fluorescence spectrophotometer.The scheme of reactions is as in Scheme1.Scheme 1


## 3. Results and Discussion

### 3.1. Structural Characterization

#### 3.1.1. Microscopy

The HRTEM micrograph of SPANI/SWCNT/ZnS nanocomposite is shown in Figure1. We observe that ZnS nanocrystallites are coated on the surfaces of SWCNT bundles to form SWCNT/ZnS nanohybrids which are embedded in the matrix of sulfonated polyaniline. The average size of the zinc sulfide nanoparticles is found to be 10 nm by direct measurement in the micrograph.Figure 1
HRTEM image of SPANI/SWCNT/ZnS nanocomposite.


#### 3.1.2. XRD Pattern

The structural characteristics of SPANI, SWCNT, SPANI/SWCNT, and SPANI/SWCNT/ZnS have been analyzed by X-ray diffractograms shown in Figures2(a) and 2(b). In the XRD pattern of SPANI, there are three prominent humps at 2θ = 25°, 43.5° and 51°. No crystalline peak of SPANI was observed as SPANI is amorphous. In the pattern of SWCNT, the peaks at 26°, 42°, and 44° correspond to (002), (100), and (101) reflections of the graphitic planes of the nanotubes, respectively (JCPDS card no. 75-1621). In the XRD pattern of SPANI-SWCNT composite, no new peak appeared. In the XRD pattern of SPANI/SWCNT/ZnS, apart from the humps assigned to SPANI and peaks assigned to SWCNT, we also observe the peaks assigned to (111), (220), and (311) planes of the cubic phase of ZnS crystal structure (JCPDS card no. 05-0566).(a) XRD pattern of SWCNT, SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS. (b) Smoothened XRD pattern of SPANI/SWCNT/ZnS structure.
(a)
(b)The mean size (D) of ZnS nanoparticles of the composite system was calculated using Debye-Scherrer formula:
(1)D=Kλβcosθ,
where K=0.89, λ is the wavelength of Cu Kα radiation, β is the full width at half maximum (FWHM) of the diffraction peak, and θ is the diffraction angle. The peak assigned to plane (111) of ZnS is chosen to calculate the particle size. The average size of the ZnS nanocrystallite is estimated to be around 2 nm. The disparity in particle size between this calculation and micrograph measurement is due to the fact that the micrograph shows the aggregates of smaller particles in the matrix of SPANI.


#### 3.1.3. FTIR Spectra

In FTIR spectra as shown in Figure3, the stretches at different points indicate the absorption bands. The stretch near 3450 cm−1 indicates the stretching vibration arising from the absorption of water by KBr used in the analysis. The spectrum of pristine SWCNT is almost featureless. In SWCNT/ZnS hybrid, the stretches at 1110 and 1383 cm−1 arise due to the presence of sulphur compound bondings, which were absent in pristine SWCNT. The stretch at 1630 cm−1 is due to the deformation vibration originated from absorption of water by KBr matrix [13].Figure 3
FTIR spectra of SPANI, SWCNT, SWCNT/ZnS, and SPANI/SWCNT/ZnS.Pure PANI shows the characteristic stretches at 1560, 1480, 1300, and 1140 cm−1. The stretches at 1560 and 1480 cm−1 arise due to the stretching vibrations of quinoid ring (–N=quinoid=N–) and the benzenoid ring (–N-benzenoid-N–), respectively. The stretch at 1300 cm−1 is due to C–N stretching and that at 1140 cm−1 is due to C=N stretching. In SPANI, the stretches at 700 and 615 cm−1 arise due to S–O and C–S stretching vibrations, respectively. The stretch at 815 cm−1 is assigned to the aromatic C–H out-of-plane bending vibration of the 1,2,4-trisubstituted aromatic rings. Similar results have been reported earlier [14]. This suggests that –SO3H groups were directly attached to the aromatic rings. The FTIR spectra of SPANI/SWCNT/ZnS composite almost match with those of SPANI. This indicates that the surface of SWCNT/ZnS hybrid was coated with SPANI to form SPANI/SWCNT/ZnS composite. The FTIR spectrum confirms that the SWCNT/ZnS hybrid fibers are embedded in the polymer matrix.


#### 3.1.4.  Raman Spectra

The Raman spectrum of SWCNT in Figure4 shows the normal characteristic peaks, the G-band at 1589 cm−1, the D-band at 1314 cm−1, and the radial breathing mode (RBM) band at 265 cm−1. There is no appreciable shift of these bands for SWCNT/ZnS hybrid nanostructure, as reported earlier [13]. In case of SPANI, the peak at 1596 cm−1 arises from C–C stretching of the benzenoid ring. The peak at 1504 cm−1 comes from C=N stretching of the quinoid ring. The peak at 1340 arises from C–N stretching and that at 1170 arises from C–H bending of the quinoid/benzenoid ring. The ID/IG factor (ratio between the intensity of D band and that of G band) increased on coating SWCNT/ZnS hybrid with the polymer. For SWCNT/ZnS hybrid, the ID/IG factor is 0.7644, while for SPANI/SWCNT/ZnS composite, it has been found to be 1.1176. This increase in ID/IG factor indicates that the SPANI adhered to the hybrid nanostructure via chemical bonding. The RBM band observed at 265 cm−1 for SWCNT has blue-shifted to 440 cm−1 for the composite material. Such blue shift can be attributed to the charge transfer between the polymer and the nanotube. After coating of the hybrid nanostructure with SPANI, the spectrum of the polymer dominates. This observation indicates that a good coating of the SWCNT/ZnS has been achieved.Figure 4
Raman spectra of SPANI, SWCNT, SWCNT/ZnS, and SPANI/SWCNT/ZnS.


#### 3.1.5. TGA Study

The rogravimetric analysis (TGA) was done to investigate the thermal stability of the samples. Figure5 shows the TGA thermograms of SWCNT, SPANI/SWCNT and SPANI/SWCNT/ZnS composites. The SWCNT has a higher thermal stability than other samples and it shows no appreciable mass loss up to about 550°C. The thermograms of SPANI/SWCNT, and SPANI/SWCNT/ZnS composites are similar up to 450°C but beyond 450°C, the mass loss for the former is slightly lower than the latter, which indicates higher thermal stability for SPANI/SWCNT/ZnS composite. This is due to the presence of SWCNT/ZnS hybrid structures in the nanocomposite.Figure 5
TGA thermograms of SPANI, SPANI/SWCNT/ZnS, and SWCNT.


### 3.2. Optical Characterization

#### 3.2.1. UV-Visible Absorption Spectra

The UV-visible absorption spectra of SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS are compared and shown in Figure6. The spectrum of SPANI consists of a prominent peak at 285 nm and a hump around 370 nm. The peak at 285 nm is assigned to the π-π* transition. The hump around 370 nm arises because of exciton transition on the polyemeraldine chain. A blue shift of the exciton transition from 370 nm (SPANI) to 360 nm (SPANI with 6% SWCNT) was observed due to the increase in the π-conjugation of the SPANI backbone. This demonstrates an electrostatic interaction between SPANI and SWCNT. The spectrum of SPANI/SWCNT/ZnS composite shows a broad maximum from 335 nm to 365 nm. So there is a blue shift of the exciton transition band from 370 nm (SPANI) to an average of 350 nm (composite). This is due to synergetic effects of SPANI and SWCNT/ZnS hybrid by way of their electronic interaction and charge transfer.Figure 6
UV-vis absorbance spectra of SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS.The optical band gapEg is related to the absorption coefficient α by the relation
(2)α=B(hν-Eg)1/2hν,
where B is the absorption constant for a direct transition. We have plotted in Figure 7 (αhν)2 versus hν and extrapolated the linear portion of it to α=0 value and obtained the corresponding band gaps. The optical band gap of pure SPANI was estimated to be 3.73 eV. For SPANI/SWCNT/ZnS composite, there is an increase in the band gap energy, with the value being 4.49 eV. The estimated band gap of pure ZnS is 4.59 eV [9].Figure 7
Plot of (αhν)2 versus hν for SPANI and SPANI/SWCNT/ZnS composite.


#### 3.2.2. Photoluminescence Spectra

Figure8(a) shows the photoluminescence spectra of SPANI, SPANI/SWCNT and SPANI/SWCNT/ZnS composite obtained at an excitation wavelength of 300 nm. SPANI shows a broad peak at 442 nm. We observe a slight blue shift to 440 nm for SPANI with 6% SWCNT. The peak position is further blue-shifted to 416 nm for SPANI/SWCNT/ZnS composite with enhanced intensity. When the SPANI/SWCNT/ZnS composite is excited by a range of excitation wavelengths from 270 to 330 nm, the emission band is gradually blue-shifted and with further increase in wavelength, we observe a slight red shift, with a prominent emission peak at 360 nm excitation wavelength as shown in Figure 8(b). When the SPANI/SWCNT/ZnS composite is excited, the electrons transit instantly from ZnS to SWCNT, causing emission with enhanced intensity. The change in band gap causes a blue shift.(a) Photoluminescence spectra for SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS. (b) Photoluminescence spectra for SPANI/SWCNT/ZnS nanocomposite at different excitation wavelengths.
(a)
(b)


## 3.1. Structural Characterization

### 3.1.1. Microscopy

The HRTEM micrograph of SPANI/SWCNT/ZnS nanocomposite is shown in Figure1. We observe that ZnS nanocrystallites are coated on the surfaces of SWCNT bundles to form SWCNT/ZnS nanohybrids which are embedded in the matrix of sulfonated polyaniline. The average size of the zinc sulfide nanoparticles is found to be 10 nm by direct measurement in the micrograph.Figure 1
HRTEM image of SPANI/SWCNT/ZnS nanocomposite.


### 3.1.2. XRD Pattern

The structural characteristics of SPANI, SWCNT, SPANI/SWCNT, and SPANI/SWCNT/ZnS have been analyzed by X-ray diffractograms shown in Figures2(a) and 2(b). In the XRD pattern of SPANI, there are three prominent humps at 2θ = 25°, 43.5° and 51°. No crystalline peak of SPANI was observed as SPANI is amorphous. In the pattern of SWCNT, the peaks at 26°, 42°, and 44° correspond to (002), (100), and (101) reflections of the graphitic planes of the nanotubes, respectively (JCPDS card no. 75-1621). In the XRD pattern of SPANI-SWCNT composite, no new peak appeared. In the XRD pattern of SPANI/SWCNT/ZnS, apart from the humps assigned to SPANI and peaks assigned to SWCNT, we also observe the peaks assigned to (111), (220), and (311) planes of the cubic phase of ZnS crystal structure (JCPDS card no. 05-0566).(a) XRD pattern of SWCNT, SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS. (b) Smoothened XRD pattern of SPANI/SWCNT/ZnS structure.
(a)
(b)The mean size (D) of ZnS nanoparticles of the composite system was calculated using Debye-Scherrer formula:
(1)D=Kλβcosθ,
where K=0.89, λ is the wavelength of Cu Kα radiation, β is the full width at half maximum (FWHM) of the diffraction peak, and θ is the diffraction angle. The peak assigned to plane (111) of ZnS is chosen to calculate the particle size. The average size of the ZnS nanocrystallite is estimated to be around 2 nm. The disparity in particle size between this calculation and micrograph measurement is due to the fact that the micrograph shows the aggregates of smaller particles in the matrix of SPANI.


### 3.1.3. FTIR Spectra

In FTIR spectra as shown in Figure3, the stretches at different points indicate the absorption bands. The stretch near 3450 cm−1 indicates the stretching vibration arising from the absorption of water by KBr used in the analysis. The spectrum of pristine SWCNT is almost featureless. In SWCNT/ZnS hybrid, the stretches at 1110 and 1383 cm−1 arise due to the presence of sulphur compound bondings, which were absent in pristine SWCNT. The stretch at 1630 cm−1 is due to the deformation vibration originated from absorption of water by KBr matrix [13].Figure 3
FTIR spectra of SPANI, SWCNT, SWCNT/ZnS, and SPANI/SWCNT/ZnS.Pure PANI shows the characteristic stretches at 1560, 1480, 1300, and 1140 cm−1. The stretches at 1560 and 1480 cm−1 arise due to the stretching vibrations of quinoid ring (–N=quinoid=N–) and the benzenoid ring (–N-benzenoid-N–), respectively. The stretch at 1300 cm−1 is due to C–N stretching and that at 1140 cm−1 is due to C=N stretching. In SPANI, the stretches at 700 and 615 cm−1 arise due to S–O and C–S stretching vibrations, respectively. The stretch at 815 cm−1 is assigned to the aromatic C–H out-of-plane bending vibration of the 1,2,4-trisubstituted aromatic rings. Similar results have been reported earlier [14]. This suggests that –SO3H groups were directly attached to the aromatic rings. The FTIR spectra of SPANI/SWCNT/ZnS composite almost match with those of SPANI. This indicates that the surface of SWCNT/ZnS hybrid was coated with SPANI to form SPANI/SWCNT/ZnS composite. The FTIR spectrum confirms that the SWCNT/ZnS hybrid fibers are embedded in the polymer matrix.


### 3.1.4.  Raman Spectra

The Raman spectrum of SWCNT in Figure4 shows the normal characteristic peaks, the G-band at 1589 cm−1, the D-band at 1314 cm−1, and the radial breathing mode (RBM) band at 265 cm−1. There is no appreciable shift of these bands for SWCNT/ZnS hybrid nanostructure, as reported earlier [13]. In case of SPANI, the peak at 1596 cm−1 arises from C–C stretching of the benzenoid ring. The peak at 1504 cm−1 comes from C=N stretching of the quinoid ring. The peak at 1340 arises from C–N stretching and that at 1170 arises from C–H bending of the quinoid/benzenoid ring. The ID/IG factor (ratio between the intensity of D band and that of G band) increased on coating SWCNT/ZnS hybrid with the polymer. For SWCNT/ZnS hybrid, the ID/IG factor is 0.7644, while for SPANI/SWCNT/ZnS composite, it has been found to be 1.1176. This increase in ID/IG factor indicates that the SPANI adhered to the hybrid nanostructure via chemical bonding. The RBM band observed at 265 cm−1 for SWCNT has blue-shifted to 440 cm−1 for the composite material. Such blue shift can be attributed to the charge transfer between the polymer and the nanotube. After coating of the hybrid nanostructure with SPANI, the spectrum of the polymer dominates. This observation indicates that a good coating of the SWCNT/ZnS has been achieved.Figure 4
Raman spectra of SPANI, SWCNT, SWCNT/ZnS, and SPANI/SWCNT/ZnS.


### 3.1.5. TGA Study

The rogravimetric analysis (TGA) was done to investigate the thermal stability of the samples. Figure5 shows the TGA thermograms of SWCNT, SPANI/SWCNT and SPANI/SWCNT/ZnS composites. The SWCNT has a higher thermal stability than other samples and it shows no appreciable mass loss up to about 550°C. The thermograms of SPANI/SWCNT, and SPANI/SWCNT/ZnS composites are similar up to 450°C but beyond 450°C, the mass loss for the former is slightly lower than the latter, which indicates higher thermal stability for SPANI/SWCNT/ZnS composite. This is due to the presence of SWCNT/ZnS hybrid structures in the nanocomposite.Figure 5
TGA thermograms of SPANI, SPANI/SWCNT/ZnS, and SWCNT.


## 3.1.1. Microscopy

The HRTEM micrograph of SPANI/SWCNT/ZnS nanocomposite is shown in Figure1. We observe that ZnS nanocrystallites are coated on the surfaces of SWCNT bundles to form SWCNT/ZnS nanohybrids which are embedded in the matrix of sulfonated polyaniline. The average size of the zinc sulfide nanoparticles is found to be 10 nm by direct measurement in the micrograph.Figure 1
HRTEM image of SPANI/SWCNT/ZnS nanocomposite.


## 3.1.2. XRD Pattern

The structural characteristics of SPANI, SWCNT, SPANI/SWCNT, and SPANI/SWCNT/ZnS have been analyzed by X-ray diffractograms shown in Figures2(a) and 2(b). In the XRD pattern of SPANI, there are three prominent humps at 2θ = 25°, 43.5° and 51°. No crystalline peak of SPANI was observed as SPANI is amorphous. In the pattern of SWCNT, the peaks at 26°, 42°, and 44° correspond to (002), (100), and (101) reflections of the graphitic planes of the nanotubes, respectively (JCPDS card no. 75-1621). In the XRD pattern of SPANI-SWCNT composite, no new peak appeared. In the XRD pattern of SPANI/SWCNT/ZnS, apart from the humps assigned to SPANI and peaks assigned to SWCNT, we also observe the peaks assigned to (111), (220), and (311) planes of the cubic phase of ZnS crystal structure (JCPDS card no. 05-0566).(a) XRD pattern of SWCNT, SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS. (b) Smoothened XRD pattern of SPANI/SWCNT/ZnS structure.
(a)
(b)The mean size (D) of ZnS nanoparticles of the composite system was calculated using Debye-Scherrer formula:
(1)D=Kλβcosθ,
where K=0.89, λ is the wavelength of Cu Kα radiation, β is the full width at half maximum (FWHM) of the diffraction peak, and θ is the diffraction angle. The peak assigned to plane (111) of ZnS is chosen to calculate the particle size. The average size of the ZnS nanocrystallite is estimated to be around 2 nm. The disparity in particle size between this calculation and micrograph measurement is due to the fact that the micrograph shows the aggregates of smaller particles in the matrix of SPANI.


## 3.1.3. FTIR Spectra

In FTIR spectra as shown in Figure3, the stretches at different points indicate the absorption bands. The stretch near 3450 cm−1 indicates the stretching vibration arising from the absorption of water by KBr used in the analysis. The spectrum of pristine SWCNT is almost featureless. In SWCNT/ZnS hybrid, the stretches at 1110 and 1383 cm−1 arise due to the presence of sulphur compound bondings, which were absent in pristine SWCNT. The stretch at 1630 cm−1 is due to the deformation vibration originated from absorption of water by KBr matrix [13].Figure 3
FTIR spectra of SPANI, SWCNT, SWCNT/ZnS, and SPANI/SWCNT/ZnS.Pure PANI shows the characteristic stretches at 1560, 1480, 1300, and 1140 cm−1. The stretches at 1560 and 1480 cm−1 arise due to the stretching vibrations of quinoid ring (–N=quinoid=N–) and the benzenoid ring (–N-benzenoid-N–), respectively. The stretch at 1300 cm−1 is due to C–N stretching and that at 1140 cm−1 is due to C=N stretching. In SPANI, the stretches at 700 and 615 cm−1 arise due to S–O and C–S stretching vibrations, respectively. The stretch at 815 cm−1 is assigned to the aromatic C–H out-of-plane bending vibration of the 1,2,4-trisubstituted aromatic rings. Similar results have been reported earlier [14]. This suggests that –SO3H groups were directly attached to the aromatic rings. The FTIR spectra of SPANI/SWCNT/ZnS composite almost match with those of SPANI. This indicates that the surface of SWCNT/ZnS hybrid was coated with SPANI to form SPANI/SWCNT/ZnS composite. The FTIR spectrum confirms that the SWCNT/ZnS hybrid fibers are embedded in the polymer matrix.


## 3.1.4.  Raman Spectra

The Raman spectrum of SWCNT in Figure4 shows the normal characteristic peaks, the G-band at 1589 cm−1, the D-band at 1314 cm−1, and the radial breathing mode (RBM) band at 265 cm−1. There is no appreciable shift of these bands for SWCNT/ZnS hybrid nanostructure, as reported earlier [13]. In case of SPANI, the peak at 1596 cm−1 arises from C–C stretching of the benzenoid ring. The peak at 1504 cm−1 comes from C=N stretching of the quinoid ring. The peak at 1340 arises from C–N stretching and that at 1170 arises from C–H bending of the quinoid/benzenoid ring. The ID/IG factor (ratio between the intensity of D band and that of G band) increased on coating SWCNT/ZnS hybrid with the polymer. For SWCNT/ZnS hybrid, the ID/IG factor is 0.7644, while for SPANI/SWCNT/ZnS composite, it has been found to be 1.1176. This increase in ID/IG factor indicates that the SPANI adhered to the hybrid nanostructure via chemical bonding. The RBM band observed at 265 cm−1 for SWCNT has blue-shifted to 440 cm−1 for the composite material. Such blue shift can be attributed to the charge transfer between the polymer and the nanotube. After coating of the hybrid nanostructure with SPANI, the spectrum of the polymer dominates. This observation indicates that a good coating of the SWCNT/ZnS has been achieved.Figure 4
Raman spectra of SPANI, SWCNT, SWCNT/ZnS, and SPANI/SWCNT/ZnS.


## 3.1.5. TGA Study

The rogravimetric analysis (TGA) was done to investigate the thermal stability of the samples. Figure5 shows the TGA thermograms of SWCNT, SPANI/SWCNT and SPANI/SWCNT/ZnS composites. The SWCNT has a higher thermal stability than other samples and it shows no appreciable mass loss up to about 550°C. The thermograms of SPANI/SWCNT, and SPANI/SWCNT/ZnS composites are similar up to 450°C but beyond 450°C, the mass loss for the former is slightly lower than the latter, which indicates higher thermal stability for SPANI/SWCNT/ZnS composite. This is due to the presence of SWCNT/ZnS hybrid structures in the nanocomposite.Figure 5
TGA thermograms of SPANI, SPANI/SWCNT/ZnS, and SWCNT.


## 3.2. Optical Characterization

### 3.2.1. UV-Visible Absorption Spectra

The UV-visible absorption spectra of SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS are compared and shown in Figure6. The spectrum of SPANI consists of a prominent peak at 285 nm and a hump around 370 nm. The peak at 285 nm is assigned to the π-π* transition. The hump around 370 nm arises because of exciton transition on the polyemeraldine chain. A blue shift of the exciton transition from 370 nm (SPANI) to 360 nm (SPANI with 6% SWCNT) was observed due to the increase in the π-conjugation of the SPANI backbone. This demonstrates an electrostatic interaction between SPANI and SWCNT. The spectrum of SPANI/SWCNT/ZnS composite shows a broad maximum from 335 nm to 365 nm. So there is a blue shift of the exciton transition band from 370 nm (SPANI) to an average of 350 nm (composite). This is due to synergetic effects of SPANI and SWCNT/ZnS hybrid by way of their electronic interaction and charge transfer.Figure 6
UV-vis absorbance spectra of SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS.The optical band gapEg is related to the absorption coefficient α by the relation
(2)α=B(hν-Eg)1/2hν,
where B is the absorption constant for a direct transition. We have plotted in Figure 7 (αhν)2 versus hν and extrapolated the linear portion of it to α=0 value and obtained the corresponding band gaps. The optical band gap of pure SPANI was estimated to be 3.73 eV. For SPANI/SWCNT/ZnS composite, there is an increase in the band gap energy, with the value being 4.49 eV. The estimated band gap of pure ZnS is 4.59 eV [9].Figure 7
Plot of (αhν)2 versus hν for SPANI and SPANI/SWCNT/ZnS composite.


### 3.2.2. Photoluminescence Spectra

Figure8(a) shows the photoluminescence spectra of SPANI, SPANI/SWCNT and SPANI/SWCNT/ZnS composite obtained at an excitation wavelength of 300 nm. SPANI shows a broad peak at 442 nm. We observe a slight blue shift to 440 nm for SPANI with 6% SWCNT. The peak position is further blue-shifted to 416 nm for SPANI/SWCNT/ZnS composite with enhanced intensity. When the SPANI/SWCNT/ZnS composite is excited by a range of excitation wavelengths from 270 to 330 nm, the emission band is gradually blue-shifted and with further increase in wavelength, we observe a slight red shift, with a prominent emission peak at 360 nm excitation wavelength as shown in Figure 8(b). When the SPANI/SWCNT/ZnS composite is excited, the electrons transit instantly from ZnS to SWCNT, causing emission with enhanced intensity. The change in band gap causes a blue shift.(a) Photoluminescence spectra for SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS. (b) Photoluminescence spectra for SPANI/SWCNT/ZnS nanocomposite at different excitation wavelengths.
(a)
(b)


## 3.2.1. UV-Visible Absorption Spectra

The UV-visible absorption spectra of SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS are compared and shown in Figure6. The spectrum of SPANI consists of a prominent peak at 285 nm and a hump around 370 nm. The peak at 285 nm is assigned to the π-π* transition. The hump around 370 nm arises because of exciton transition on the polyemeraldine chain. A blue shift of the exciton transition from 370 nm (SPANI) to 360 nm (SPANI with 6% SWCNT) was observed due to the increase in the π-conjugation of the SPANI backbone. This demonstrates an electrostatic interaction between SPANI and SWCNT. The spectrum of SPANI/SWCNT/ZnS composite shows a broad maximum from 335 nm to 365 nm. So there is a blue shift of the exciton transition band from 370 nm (SPANI) to an average of 350 nm (composite). This is due to synergetic effects of SPANI and SWCNT/ZnS hybrid by way of their electronic interaction and charge transfer.Figure 6
UV-vis absorbance spectra of SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS.The optical band gapEg is related to the absorption coefficient α by the relation
(2)α=B(hν-Eg)1/2hν,
where B is the absorption constant for a direct transition. We have plotted in Figure 7 (αhν)2 versus hν and extrapolated the linear portion of it to α=0 value and obtained the corresponding band gaps. The optical band gap of pure SPANI was estimated to be 3.73 eV. For SPANI/SWCNT/ZnS composite, there is an increase in the band gap energy, with the value being 4.49 eV. The estimated band gap of pure ZnS is 4.59 eV [9].Figure 7
Plot of (αhν)2 versus hν for SPANI and SPANI/SWCNT/ZnS composite.


## 3.2.2. Photoluminescence Spectra

Figure8(a) shows the photoluminescence spectra of SPANI, SPANI/SWCNT and SPANI/SWCNT/ZnS composite obtained at an excitation wavelength of 300 nm. SPANI shows a broad peak at 442 nm. We observe a slight blue shift to 440 nm for SPANI with 6% SWCNT. The peak position is further blue-shifted to 416 nm for SPANI/SWCNT/ZnS composite with enhanced intensity. When the SPANI/SWCNT/ZnS composite is excited by a range of excitation wavelengths from 270 to 330 nm, the emission band is gradually blue-shifted and with further increase in wavelength, we observe a slight red shift, with a prominent emission peak at 360 nm excitation wavelength as shown in Figure 8(b). When the SPANI/SWCNT/ZnS composite is excited, the electrons transit instantly from ZnS to SWCNT, causing emission with enhanced intensity. The change in band gap causes a blue shift.(a) Photoluminescence spectra for SPANI, SPANI/SWCNT, and SPANI/SWCNT/ZnS. (b) Photoluminescence spectra for SPANI/SWCNT/ZnS nanocomposite at different excitation wavelengths.
(a)
(b)


## 4. Conclusions

We reported the synthesis of a novel luminescent material containing sulfonated polyaniline, embedded with functionalized SWCNTs hybridized with ZnS nanocrystals, by a simple chemical process. Characterization established the desired nanostructure of the composite material. The energy band gap of 3.73 eV for pure SPANI was found to be increased to 4.49 eV for the composite. The PL emission from the composite showed a broad emission range in the visible region between 400 and 450 nm with the peak emission at 416 nm, with appreciable enhancement in the intensity of emission, leading to the formation of a novel luminescent polymer nanocomposite.



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*Source: 253016-2013-11-04.xml*