In this section, we have discussed the structural/morphological and optoelectronic properties of ionic liquid and polyamide dye based ZnO samples A, B and C respectively using XRD, FESEM, DLS, UV-Visible, and fluorescence spectroscopy techniques.
3.2. Characterizations of Samples A, B and C (DLS, XRD and FTIR)
The distribution of particle size of ionic liquid based sample A showed an average particle size in the range of 184 nm, as measured with DLS based particle size analyzer (
Figure 4a) by dissolving the compound in DMSO: H
2O (70:30; v/v). The particle size of sample B was also measured using a DLS, particle size analyzer, which showed size 176 nm (
Figure 4b). The particle size of sample C capped ZnO nanoparticles was also measured using a DLS, particle size analysis which showed size 166 nm (
Figure 4c). DLS spectra have shown somewhat larger particle size as compared to FESEM analysis due to the hydro-dynamic radius of nanoaggregates during DLS analysis.
The crystalline size of the synthesized ionic liquid and polyamide dye capped ZnO nanoparticles was characterized by using XRD techniques. XRD analysis of the prepared samples A, B, and C was done by a Rigaku Mini flex III diffractometer operated at 30 kV and 10 mA using CuKα X- ray radiations with a scan speed of 10
⸰/min for 2θ in a range of 10 to 75. The indexing process of the powder diffraction pattern of ZnO was done by Miller Indices
(h k l) and each peak was assigned in the first step. The X-ray diffractogram of the entire data has been shown in
Figure 5a. The average particle size of the ionic liquid and polyamide dye capped ZnO has been evaluated by using the Debye-Scherrer formula
D = 0.9λ/βcosθ, where ‘
λ’ is the wavelength of X-ray (0.1541 nm), ‘
β’ is the FWHM (full width half maximum), ‘
θ’ is the diffraction angle, and ‘
D’ is the particle diameter size [
22,
23,
24]. For samples A, B and C, the XRD spectrum (
Figure 5a) shows the presence of broad peaks of sample A at 2θ = 31.786, 34.447, 36.262, 47.533, 56.593, 62.866, 67.954 degrees, sample B at 2θ = 31.638, 34.297, 36.124, 47.416, 56.478, 62.752, 67.848, 76.844 degrees and sample C at 2θ = 32.589, 23.817, 37.983, 60.806, 72.092 degrees respectively. While comparing to the JCPDS card (36-1451) [
19,
20,
21], the average size of dye capped ZnO nanoparticles (sample A) was found to be in the range of 184.2 nm (
Figure 5a) showing that with surface capping, the XRD pattern peak of polyamide dye capped ZnO nanoparticles appeared to be widened. The average size of sample B was found to be in the range of 176.3 nm and for the sample C, its range was 160.5 nm.
It was confirmed from the graph that the main peaks were in agreement with the wurtzite structure of ZnO, which indicated that the surface capping of ZnO nanoparticles (i.e., ionic liquid electrolyte and polyamide dye capped ZnO nanoparticles (sample A, B, and C)) has no effect on the crystalline nature of ZnO nanoparticles. The surface variation removes the combined surfactants present on the ZnO. Hence, we used ionic liquid (IL) and polyamide as an effective functional group for surface capping of ZnO nanoparticles.
Table 2.
XRD calculations for dye capped ZnO nanoparticles.
Table 2.
XRD calculations for dye capped ZnO nanoparticles.
Polyamide dye capped ZnO Samples |
Peak position (in degrees) |
Reflection (h k l)
|
d-spacing (in nm)
|
Size of particle D (in nm)
|
Sample A |
36.26° |
101 |
2.47 |
184.2 |
Sample B |
36.12° |
101 |
2.48 |
176.3 |
Sample C |
24.60°
|
002 |
3.61 |
160.5 |
FTIR spectroscopy is an analytical technique used to identify the nature of materials such as organic, polymeric, and in some cases, inorganic materials. The FTIR spectroscopy method uses infrared light to scan test samples and detect their chemical properties. The FTIR absorption spectrum was recorded around 1000-4000 cm-1 suggesting the incoming and outgoing impurities. To be more particular, a large absorption band around 2500 cm-1 corresponds to the COOH stretching approach of the carboxyl group. The presence of the absorption peaks around 3000 and 3500 cm-1 is due to the COOH stretching vibration mode of the different alkyl groups. The presence of the peaks between 1800 and 1400 cm-1 is due to the balanced and unbalanced stretching mode of the zinc carboxylate group, respectively. It is obvious that as the size of the ZnO nanoparticles starts to increase, the quantity of the impurities, such as carboxyl group in the samples, will also decrease correspondingly. The FTIR is used to convey the information about the presence of incoming and outgoing impurities that may exist near to the surface of ionic liquid and polyamide dye capped ZnO nanoparticles.
Figure 5b clearly shows the FTIR spectra of ionic liquid and polyamide dye capped ZnO nanoparticles at different samples, such as samples A, B, C respectively. Annealing of the ionic liquid capped ZnO nanoparticle samples radically decreases in all samples of ZnO nanoparticles. At longer annealing time, the spectral signatures of carboxyl group essentially start to disappear, signifying the probable dissociation of zinc and its resulting in the formation of ZnO nanoparticles.
3.3. Morphological Studies (FE-SEM)
The morphology and size divisions of ionic liquid and polyamide dye capped ZnO nanoparticles (samples A, B, and C) were investigated by scanning electron microscopy technique with the SEM model JEOL Model-JSM-7610F plus at 10 kV. The SEM images of samples A, B, and C seem to be standardized as shows in
Figure 6a–c. The SEM micrograph shown that the dye capped ZnO nanoparticles i.e. sample A, B, and C are in the nano region (nano flowers like structures).
The observed length of the dye capped ZnO nanoparticles (sample A) was in the range of 187nm approximately. The width of the modified ZnO nanoparticle is 9.8 nm as appears in the high magnification FESEM image shown in
Figure 6a. The
Figure 6 (b) and (c) show the FESEM results of the dye capped ZnO nanoparticles (sample B and C). The size and morphology of ZnO nanoparticles were observed at different resolutions. The FESEM image shows the modified ZnO nanoparticles from supramolecular self-assembled structures due to the structure directed nature of the compound. The material shows almost no particle group and very standardized particle size distribution in the nanoparticle of sample B with a range of about 180 nm and width is 9.7 nm. The size and morphology of ionic liquid based sample C ranges around 170 nm and the width is approximately 9.1 nm.
Table 3.
Summary of FESEM calculations for dye capped ZnO nanoparticles (sample A, B, and C).
Table 3.
Summary of FESEM calculations for dye capped ZnO nanoparticles (sample A, B, and C).
Name of ZnO Sample |
Width of ZnO Nanoparticle |
Sample A |
9.8 nm |
Sample B |
9.7 nm |
Sample C |
9.1 nm |
Table 4 shown the comparison of the size of dye capped ZnO nanoparticles examined under different techniques: XRD, FE-SEM, and DLS for samples A, B and C. The table readings shown the similarities among the
Table 4.
Summary of XRD, FE-SEM, DLS calculations for polyamide dye capped ZnO nanoparticles (samples A, B, and C).
Table 4.
Summary of XRD, FE-SEM, DLS calculations for polyamide dye capped ZnO nanoparticles (samples A, B, and C).
Sample Name |
XRD (size of ZnO nanoparticles)
|
FE-SEM (size of ZnO nanoparticles)
|
DLS (size of ZnO nanoparticles)
|
Sample A |
184.2 nm |
187 nm |
184 nm |
Sample B |
176.3 nm |
180 nm |
176 nm |
Sample C |
160.5 nm |
170 nm |
166 nm |
Table 5.
Summary of UV-Visible spectra calculations for dyes capped ZnO nanoparticles. (for samples A, B, and C).
Table 5.
Summary of UV-Visible spectra calculations for dyes capped ZnO nanoparticles. (for samples A, B, and C).
Name of Sample |
ZnO(in mg)
|
Ionic Liquid(in mg)
|
Polyamide(in mg)
|
UV-Visible spectraPeak 1 & Peak 2
|
Sample A |
500 mg |
700 mg |
500 mg |
263 nm, 295 nm |
Sample B |
500 mg |
600 mg |
700 mg |
278 nm, 344 nm |
Sample C |
500 mg |
500 mg |
600 mg |
276 nm, 305 nm |
Table 6.
Summary of energy band gap (Eg) values of dye capped ZnO nanoparticles. (for samples A, B and C based ZnO nanoparticles).
Table 6.
Summary of energy band gap (Eg) values of dye capped ZnO nanoparticles. (for samples A, B and C based ZnO nanoparticles).
Ionic liquid based ZnO samples |
Wavelength(λ)( in nm)
|
Absorbance(α)
|
(αhν)2 |
Energy band gap(Eg)(in eV)
|
Sample A |
263.8 |
0.746 |
3.50 |
4.70 |
Sample B |
278.8 |
3.185 |
14.16 |
4.44 |
Sample C |
276.6 |
0.136 |
0.61 |
4.48 |
3.5. Photovoltaic Performances of ZnO DSSCs
The current and voltage characteristics have been recorded for three different samples A, B, and C based ZnO DSSCs at an effective surface area of 1cm
2 under simulated solar irradiations of 100 mW/cm
2 as shown in
Figure 9. The different electrical parameters for ZnO DSSC i.e., short circuit current density (
Jsc), open circuit voltage (
Voc), fill factor (
FF), and incident photon to current conversion efficiency (
η%) have been calculated and presented in
Table 7.
Figure 9 shows that the current density and photo-voltage curves of the ZnO DSSCs under the influence of samples A, B, and C. The sample A based ZnO DSSC (SC
A) shows the lowest values of short circuit current density (J
sc = 10.12 mA/cm
2), open circuit voltage (V
oc = 0.68 V), maximum value of current density (J
max = 8.82 mA/cm
2) and voltage (V
max = 0.46 V).
The calculated value of fill factor (FF) for sample A based ZnO DSSC is 0.58. We obtained the lowest value of incident photon to current conversion efficiency (
η = 3.99%) for sample A based ZnO DSSC. When the dye molecules are capped on ZnO nanoparticles, the form combination among the nanoparticles absorbed the radiations in the whole of the visible region and near infrared region of the solar spectrum. In order to compare this photovoltaic performance with other ZnO DSSCs, the sample B based ZnO DSSC (SC
B) shows the highest values of short circuit current density (J
sc = 13.02 mA/cm
2) and open circuit voltage (V
oc = 0.7 V). The corresponding values of its maximum current density (J
max = 10.92 mA/cm
2) and maximum voltage (V
max = 0.52) were recorded. The calculated value of fill factor (FF) for sample B based ZnO DSSC is 0.62. For the sample B based ZnO DSSC, we obtained a significant enhanced value of incident photon to current conversion efficiency (
η = 5.65 %). Similarly the sample C based ZnO DSSC (SC
C) shows the lowest values of short circuit current density (J
sc = 11.65 mA/cm
2) and open circuit voltage (V
oc = 0.69 V). The maximum value of current density (J
max = 9.74 mA/cm
2) and voltage (V
max = 0.49 V). For the sample C + ZnO DSSC, we obtained the values of incident photon to current conversion efficiency (
η = 4.46 %). An important photo parameter of quantum efficiency or spectral response i.e., the incident to photon current conversion efficiency (IPCE) for samples A, B, and C based ZnO DSSCs had been recorded as shown in
Figure 10. The incident photon to current conversion efficiency (IPCE) was recorded using the following equation (6).
Where
λ is the wavelength,
Jsc is the short circuit current density (mA/cm
2), and
Pin is the input power (mW/cm
2) [
36]. The IPCE spectra for the samples A, B, and C based ZnO DSSCs had shown the broader peak bands between 300 nm to 700 nm. The values of IPCE spectra obtained for sample A, B and C based ZnO DSSCs at 500 nm were 57%, 61 % and 55% respectively. The comparison of IPCE spectra of samples A, B and C based ZnO DSSCs are presented in
Table 8.
From the
Table 8, it has been observed that the IPCE spectra of capped ZnO DSSCs (sample C) has lower efficiency as compared to ZnO DSSCs (sample A (57%) and sample B (61%)).
Table 9 shown that the comparison of the power conversion efficiencies between ZnO DSSCs (present results) and other DSSCs SC1, SC2, SC3 and SC4 (references [
37,
38,
39,
40]). This comparison is based on the quantity of ionic liquid electrolytes and dye used in the DSSCs. The comparison results revealed that the achieved efficiencies of ionic liquid and polyamide dye capped ZnO DSSCs were 3.99%, 5.65%, and 4.46% (for samples A, B and C based ZnO DSSCs) better than the efficiencies of ionic liquids and N-3/Z-907 dyes based other consulted DSSCs (4.4%, 3.1%, 5.3%, 5.4% and 5.17%) obtained from the above mentioned references respectively. It has been concluded that the sample B based ZnO DSSC (SC
B) shown better power conversion efficiency and IPCE spectral value than other ZnO DSSCs (SC
A and SC
C).
3.6. Conclusions
For the present research work, we have synthesized three samples (A, B, and C) of ionic liquid and polyamide dye capped ZnO nanoparticles with the wet chemical precipitation method by a reaction between trimethylamine with bromoacetic acid (for ionic liquid as an electrolyte)) and trimesoylchloride with ethylenediamine ( for Polyamide dye). The synthesized samples A, B, and C were characterized by various methods like XRD, UV-Vis, FESEM, FTIR, DLS and Fluorescence spectra. The observation for FESEM clarified a well-defined nano-flowers like structures of dye capped ZnO nanoparticles. DLS results agreed well with the FESEM results in term of the distribution of particle size for samples A, B, and C capped ZnO nanoparticles respectively. XRD pattern also specified that the polyamide dye capped ZnO nanoparticles were single crystalline structures. The optoelectronic studies of samples A, B, and C based ZnO nanoparticles indicated good light absorption in the UV-Vis band with visible discharge emission. Further these samples (dyes capped ZnO nanoparticles) were processed as photo-anode sheets to design the dye sensitized solar cells (DSSCs). The photovoltaic studies under AM (air mass) 1.5 solar irradiations showed that the overall achieved incident photon to current conversion efficiency of sample B capped ZnO DSSC was higher by 1.66 % and 1.19% than sample A and C based ZnO DSSCs. A significant improvement of 6% in the IPCE spectra for sample B based ZnO DSSC was observed when compared to IPCE spectra of sample C based ZnO DSSC. Hence such solar cell assemblies can be implemented for low cost photovoltaic applications for clean and green energies.