# Characterization of Synthetic Ni(II)-Xylenol Complex as a Photosensitizer for Wide-Band Gap ZnO Semiconductor Electrodes

Authors: Suman Kushwaha; Lal Bahadur
Journal: International Journal of Photoenergy
 (2011)

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## Abstract

A synthetic NiIIL(H2O)2 complex (L = xylenol orange, 3,3′-bis [N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonapthalein (H2O)2), which is a water-soluble dye,  has been studied for its photosensitizing properties at n-ZnO semiconductor electrodes prepared by sol-gel techniques. The absorption spectrum of aqueous solution of this complex exhibits a strong peak at 563 nm and a shoulder at 526 nm wavelength of light. The sandwich-type dye-sensitized solar cell using ZnO semiconducting thin film with test dye anchored onto it showed the cell output as follows: VOC=0.506 V, Jsc=1.68 mA cm−2, and FF=0.41 under illumination with full spectrum of light (intensity 520 mW cm−2), while on illumination with visible light (λ>420 nm, intensity 480 mW cm−2), VOC=0.506 V, Jsc=1.4 mA cm−2, and FF=0.49 were achieved. Maximum incident photon-to-current conversion efficiency for the present system was found to be 8.7% at wavelength (λmax=563 nm).


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## Body

## 1. Introduction

Dye-sensitized solar cells (DSSCs) are unique and attractive devices for the conversion of solar energy into electricity based on sensitization of wide band gap semiconductors [1–14]. In general in DSSCs dye molecules adsorbed on the surface of nanocrystalline ZnO are photoexcited by incident light and inject electrons into the conducting band of ZnO. The oxidized dye is regenerated by the reduced species of the redox-couple, typically I-/I3-, dissolved in the electrolyte. The resulting I3- diffuses to the Pt-counter electrode, where it is reduced. Since dye plays an important role in absorbing visible light and transferring photon energy into electricity, much attention has been paid to survey the effective sensitizer dyes. It is necessary for sensitizer dyes to have suitable energy levels to transfer electrons and anchor group(s) to have affinity for semiconductors. Usually, synthetic inorganic compounds such as ruthenium (II) complexes with carboxylated polypyridyl ligands are employed as molecular sensitizers (S) in DSSCs due to their intense charge-transfer absorption in the whole visible range of solar spectrum, excellent stability, and highly efficient metal-to-ligand charge transfer [15–17]. The energies of the MLCT states can be altered systematically by modifying the anchoring ligands as well as by changing the ancillary ligands or its substituents. The wide possibilities to tune the MLCT energy led to the preparation of many different compounds that have been investigated for semiconductor sensitization. In order to replace the rare and expensive ruthenium compounds, many kinds of organic synthetic dyes have been actively studied and tested as low-cost materials [18–27]. This work is in continuation of this series of investigations in which a newly synthesized transition metal complex Na4[NiL(H2O)2], where L is 3,3 bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand [28] has been characterized for its photosensitizing properties at n-ZnO thin-film electrodes prepared by sol-gel method. The results of this investigation are reported here.


## 2. Experimental

### 2.1. Materials and Equipments

LiI (Aldrich), iodine (CDH, India) were used as redox couple. Ethanol (Merck, India) was dried following the method of Lund and Bjerrum [29] before using it for preparing ZnO-sol. Zinc acetate (CDH, India) and LiOH · H2O (Alfa product) were used as received. The platinum catalyst (T/SP) was obtained from Solaronix for counter electrode. The sealing agent (SX1170-60, 50 μm) was obtained from Solaronix. The Nickel (II)-xylenol orange metal complex studied as a photosensitizer was synthesized by Pandey and Narang [28] and made available to us for investigation.X-ray diffraction pattern of ZnO powder was obtained with X-ray diffractometer (Model 3000, SEIFERT, Germany) using CuKα radiation of 1.54 Å´ to determine the crystal structure. Current and voltage of XRD were maintained at 30 mA and 40 kV during the measurement. The XRD pattern was recorded in 2θ range. Morphology of ZnO thin film was examined by scanning electron microscope (FESEM, quanta 200 FEG). Voltammograms were recorded using a three-electrode cell consisting of Ag/Ag+ reference electrode (0.1 AgNO3 + 0.01 TBAP in acetonitrile medium), Pt wire auxiliary electrode and Pt disc working electrode. NaClO4 (0.1 M in water) was used as supporting electrolyte. Experimental solution was purged with N2 gas for 30 min before recording the voltammograms.Electrochemical measurements were made with the help of a bipotentiostat (model no. AFRDE4E, Pine Instrument Company, USA) and a computer controlled e-corder (model no. 201, e-DAQ, Australia). A 150 W xenon arc lamp with lamp housing (model no. 66057) and power supply (model no. 68752), all from Oriel Corporation, USA, was used as a light source. The semiconductor electrode was illuminated after passing the collimated light beam through a 6 inch long water column (to filter IR radiation) and condensing it with the help of fused silica lenses (Oriel Corporation, USA). This IR-filtered light is referred to as “white light” in the text. Whenever required, the UV part of the white light was cut off by using a long pass filter (model no. 51280, Oriel Corporation, USA) and the resultant light (λ>420nm) obtained this way is referred to as “visible light”. The monochromatic light was obtained with the use of a monochromator (Oriel model 77250 equipped with model 7798 grating), and the corresponding photocurrent was measured with the help of a digital multimeter (Philips model no. 2525) in combination with the potentiostat. Light intensities were measured with a digital photometer (Tektronix model J16 with model J6502 sensor) in combination with neutral density filters (model no. 50490-50570, Oriel, USA). The absorption spectrum of the test dye Ni(II) xylenol complex was recorded on Cary 2390 (Varian) spectrophotometer.


### 2.2. Synthesis of Complexes

This water soluble metal complex was prepared by mixing aqueous solutions (0.01 M) nickel (II), and the ligand, 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein (Na4H2L) (0.01 M), in 1 : 1 ratio. The pH of the mixtures was raised to 11 by addition of NaOH solution and the mixture was refluxed on a water bath for 2 h. After cooling the solution, Me2CO (ca 50 cm3) in 100 cm3 aqueous solution was added until shining microcrystals were formed. The metal (II) complex with Na4H2L was analyzed for M, C, H, N, and S content. Detailed process of the synthesis, characterization, spectral and properties of metal complex have been given somewhere else [28].


### 2.3. Formation of ZnO Precursor Sol and Thin-Film Preparation

Thin films of ZnO of nanometer-sized colloidal ZnO were prepared following the method of Spanhel and Anderson [30]. In brief, the organometallic precursor was prepared by refluxing 0.1 M zinc acetate solution in absolute ethanol (dry) for about 3 h at 80°C avoiding its exposure to moisture. Then, keeping it in ice-cold water, equimolar LiOH · H2O was added to it, and the hydrolysis was allowed to continue for half an hour keeping the container in an ultrasonicator. This resulted in a dense sol consisting of ZnO colloids and is coated on conducting glass substrate by dip coating. A portion of the colloidal sol was left to get dried, and this dried powder was sintered at 450°C for X-ray crystallographic studies. Scheme 3 shows the method of preparation of ZnO sol and subsequently its thin film on conducting glass substrate. Prior to using it for film deposition, the substrate was washed with mildly heated, soapy pure water and then ultrasonically cleaned with acetone first and then with iso-propanol for 30 min each. It was further cleaned with ultra pure water for 15 min and kept in oven at 80°C for 30 minutes. A U-shaped frame of adhesive tape was put over the conducting face of the glass substrate to control the thickness of the ZnO film and to provide noncoated area for electrical contact. This process was repeated 5-6 times to get the films of the required thickness. The deposited films were air dried and then the adhesive tapes were carefully removed. These films were finally annealed in air at 450°C for l.5 h. This way ZnO thin film of approximately 2 μm thickness was obtained.


### 2.4. Photoelectrochemical Measurements

For studying the performance of test dye on ZnO thin-film electrode sandwich type cells were fabricated. For this purpose, the thin-film electrode was dipped into 0.1 mM aqueous solution (deionized water) of test dye for overnight. The dye-coated film was air dried. This was used as photoelectrode in the cell. To provide space for filling cell electrolyte and to assemble the cell, the hot-melt sheet (SX1170-60, 50μm thick, Solaronix) was used as sealing frame. The counter electrode was prepared on FTO (Flexitec, Product no. 102-020, sheet resistance 10–20 Ω/□) by screen printing method using platinum catalyst (T/SP, Solaronix) and then annealed at 450°C for 30 minutes. To assemble the cell, the counter electrode was put over the photoelectrode and sealed using spacer/sealing material and heating it at ~80°C. An electrolyte solution composed of 0.5 M LiI and 0.05 M I2 in propylene carbonate (PC) was introduced into the cell by capillary action and then sealed properly.


## 2.1. Materials and Equipments

LiI (Aldrich), iodine (CDH, India) were used as redox couple. Ethanol (Merck, India) was dried following the method of Lund and Bjerrum [29] before using it for preparing ZnO-sol. Zinc acetate (CDH, India) and LiOH · H2O (Alfa product) were used as received. The platinum catalyst (T/SP) was obtained from Solaronix for counter electrode. The sealing agent (SX1170-60, 50 μm) was obtained from Solaronix. The Nickel (II)-xylenol orange metal complex studied as a photosensitizer was synthesized by Pandey and Narang [28] and made available to us for investigation.X-ray diffraction pattern of ZnO powder was obtained with X-ray diffractometer (Model 3000, SEIFERT, Germany) using CuKα radiation of 1.54 Å´ to determine the crystal structure. Current and voltage of XRD were maintained at 30 mA and 40 kV during the measurement. The XRD pattern was recorded in 2θ range. Morphology of ZnO thin film was examined by scanning electron microscope (FESEM, quanta 200 FEG). Voltammograms were recorded using a three-electrode cell consisting of Ag/Ag+ reference electrode (0.1 AgNO3 + 0.01 TBAP in acetonitrile medium), Pt wire auxiliary electrode and Pt disc working electrode. NaClO4 (0.1 M in water) was used as supporting electrolyte. Experimental solution was purged with N2 gas for 30 min before recording the voltammograms.Electrochemical measurements were made with the help of a bipotentiostat (model no. AFRDE4E, Pine Instrument Company, USA) and a computer controlled e-corder (model no. 201, e-DAQ, Australia). A 150 W xenon arc lamp with lamp housing (model no. 66057) and power supply (model no. 68752), all from Oriel Corporation, USA, was used as a light source. The semiconductor electrode was illuminated after passing the collimated light beam through a 6 inch long water column (to filter IR radiation) and condensing it with the help of fused silica lenses (Oriel Corporation, USA). This IR-filtered light is referred to as “white light” in the text. Whenever required, the UV part of the white light was cut off by using a long pass filter (model no. 51280, Oriel Corporation, USA) and the resultant light (λ>420nm) obtained this way is referred to as “visible light”. The monochromatic light was obtained with the use of a monochromator (Oriel model 77250 equipped with model 7798 grating), and the corresponding photocurrent was measured with the help of a digital multimeter (Philips model no. 2525) in combination with the potentiostat. Light intensities were measured with a digital photometer (Tektronix model J16 with model J6502 sensor) in combination with neutral density filters (model no. 50490-50570, Oriel, USA). The absorption spectrum of the test dye Ni(II) xylenol complex was recorded on Cary 2390 (Varian) spectrophotometer.


## 2.2. Synthesis of Complexes

This water soluble metal complex was prepared by mixing aqueous solutions (0.01 M) nickel (II), and the ligand, 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein (Na4H2L) (0.01 M), in 1 : 1 ratio. The pH of the mixtures was raised to 11 by addition of NaOH solution and the mixture was refluxed on a water bath for 2 h. After cooling the solution, Me2CO (ca 50 cm3) in 100 cm3 aqueous solution was added until shining microcrystals were formed. The metal (II) complex with Na4H2L was analyzed for M, C, H, N, and S content. Detailed process of the synthesis, characterization, spectral and properties of metal complex have been given somewhere else [28].


## 2.3. Formation of ZnO Precursor Sol and Thin-Film Preparation

Thin films of ZnO of nanometer-sized colloidal ZnO were prepared following the method of Spanhel and Anderson [30]. In brief, the organometallic precursor was prepared by refluxing 0.1 M zinc acetate solution in absolute ethanol (dry) for about 3 h at 80°C avoiding its exposure to moisture. Then, keeping it in ice-cold water, equimolar LiOH · H2O was added to it, and the hydrolysis was allowed to continue for half an hour keeping the container in an ultrasonicator. This resulted in a dense sol consisting of ZnO colloids and is coated on conducting glass substrate by dip coating. A portion of the colloidal sol was left to get dried, and this dried powder was sintered at 450°C for X-ray crystallographic studies. Scheme 3 shows the method of preparation of ZnO sol and subsequently its thin film on conducting glass substrate. Prior to using it for film deposition, the substrate was washed with mildly heated, soapy pure water and then ultrasonically cleaned with acetone first and then with iso-propanol for 30 min each. It was further cleaned with ultra pure water for 15 min and kept in oven at 80°C for 30 minutes. A U-shaped frame of adhesive tape was put over the conducting face of the glass substrate to control the thickness of the ZnO film and to provide noncoated area for electrical contact. This process was repeated 5-6 times to get the films of the required thickness. The deposited films were air dried and then the adhesive tapes were carefully removed. These films were finally annealed in air at 450°C for l.5 h. This way ZnO thin film of approximately 2 μm thickness was obtained.


## 2.4. Photoelectrochemical Measurements

For studying the performance of test dye on ZnO thin-film electrode sandwich type cells were fabricated. For this purpose, the thin-film electrode was dipped into 0.1 mM aqueous solution (deionized water) of test dye for overnight. The dye-coated film was air dried. This was used as photoelectrode in the cell. To provide space for filling cell electrolyte and to assemble the cell, the hot-melt sheet (SX1170-60, 50μm thick, Solaronix) was used as sealing frame. The counter electrode was prepared on FTO (Flexitec, Product no. 102-020, sheet resistance 10–20 Ω/□) by screen printing method using platinum catalyst (T/SP, Solaronix) and then annealed at 450°C for 30 minutes. To assemble the cell, the counter electrode was put over the photoelectrode and sealed using spacer/sealing material and heating it at ~80°C. An electrolyte solution composed of 0.5 M LiI and 0.05 M I2 in propylene carbonate (PC) was introduced into the cell by capillary action and then sealed properly.


## 3. Results and Discussion

### 3.1. Structural Characterization of ZnO Thin Film

The crystalline structure of the ZnO particles was analyzed through X-ray diffraction (XRD). The XRD of ZnO powder annealed at 450°C is shown in Figure1. The diffraction peaks of the sample reveals that ZnO crystallizes well after annealing. All the diffraction peaks are in agreement with the reported data in JCPDS Card no. 36-1451 for hexagonal wurtzite phase of zinc oxide. Average grain size has been calculated using Scherrer’s equation(1)d=0.9λBcos⁡θ,
where λ,θ, and B are the X-ray wavelength (1.54 Å), Braggs diffraction angle, and full width at half maximum (FWHM), respectively. The calculated average size of zinc oxide nanoparticles was found to be ~30–35 nm, which is in agreements with that already reported using this method of sol preparation [31].Figure 1
XRD of ZnO powder prepared by Spenhel and Anderson method and sintered at 450°C.


### 3.2. Surface Morphology

Figure2 show the SEM image of ZnO thin film prepared by depositing the colloidal sol on conducting glass and annealed at 450°C. The film shows a smooth porous surface with a fine microstructure, without cracks or void.Figure 2
SEM image of the nanocrystalline thin film prepared by using zinc oxide colloidal sol (annealing conditions: at 450°C in air for 1.5 h).


### 3.3. Characterization of Ni(II) Xylenol Metal Complex

#### 3.3.1. Structure of the Complex

Ligand Na4H2L (Scheme 1) has several bonding sites, but the two acidic chelating groups on the side of its large sulphonphthalein nucleus may behave like branched donating sites enhancing the possibility of mononuclear or binuclear complex formation with metal ions. In binuclear complex formation, both sides of the sulphonphthalein nucleus are chelated by PhO-, N, and two COO- electron pairs. Empirical formulae derived from analytical data (C, H, N, S, and metal contents) suggest the formation of 1 : 1 (M : L) complexes. The assumption of 4 : 1 complex electrolyte can be confirmed by high molar conductance values (greater than 400Ω-1cm2mol-1) observed in 1 mM aqueous solution of the complex though the conductivity values are slightly lower than the value for uni-tetravalent electrolyte. The complex anion with 4- charge is voluminous and poorly mobile, considerably reducing its contribution to the molar conductivity [28]. Depending on pH, the chelation process indicates stepwise formation of stable complex species namely MH2L2-, MHL3-, and ML4- in solution.Scheme 1
Structure of ligand Na4H2L.Scheme2 represents the chemical structure of nickel (II) metal complexes with 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand as proposed by Pandey and Narang [28].Scheme 2
Structure of nickel (II) metal complex with 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand as proposed by Pandey and Narang [28].Scheme 3
Schematic presentation of preparation of ZnO sol and its thin film on conducting glass substrate.


#### 3.3.2. Redox Behaviour of Nickel (II) Xylenol Complex

The cyclic voltammograms of xylenol nickel (II) complex in aqueous solution containing 0.1 M NaClO4 obtained in the potential range of −1.5 V to 1.0 V at different scan rates (0.020–0.200Vs-1) are shown in Figure 3(a) while Figure 3(b) shows cyclic voltammograms (10 cycles) repeated at a fixed scan rate of 100 mV/s. No measurable shift in peak has been observed which shows that the complex is stable in solution. From these curves it is evident that during forward scan in anodic potential range one peak (b) (Ep,a=+0.420V) was observed. During the reverse scan cathodic peaks (c) and (d) were observed at (Ep,c)c=-0.112V and (Ep,c)d=-0.858V. The reoxidation anodic peak (a) (Ep,a=-0.732V) seems to be associated with the cathodic peak (d) but (b) has no associated cathodic peak. It is pertinent to point out here that though peaks (d) and (a) have been assigned to reduction of Ni(II) in complex cation to Ni (I) and its reversal, their separation ((Ep,a)a-(Ep,c)c) is quite large as compared to that expected for one electron transfer process and it is also not stable with the change in the scan rate from 20 to 200 mV/s. However, it can be added here that the cathodic peak potential (Ep,c=-0.858V) corresponding to (d) matches closely with the reduction potential Ep,c=-0.85V reported by Bulut [32] for the same cation in another transition metal complex. Ep,c shifting to more negative potentials (from −0.830 to −0.858 V) was observed when the scan rate was increased from 20 to 200 mV/s which confirms the irreversibility of the reduction process. The formal redox potential (Ef0=(Ep,a+Ep,c)/2) for the above mention process can be taken as −0.795 V. The oxidation potential (Ep,a)b=+0.420V provides the electron donating energy level of the test dye in its ground state with respect to reference electrode.(a) Cyclic voltammogram in aqueous medium containing 0.1 mM test dye + 0.1 M NaClO4 supporting electrolyte at different scan rates I-20, II-50, III-60, and IV-100 mV/s. (b) Cyclic voltammogram in aqueous medium containing 0.1 mM test dye + 0.1 M NaClO4  supporting electrolyte at scan rate of 100 mV/s (10 cycles).
(a)(b)


#### 3.3.3. Optical Properties of Nickel Xylenol Complex

Since the optical property of a compound, to be used as a sensitizer, plays the significant role in mediating the photoelectrochemical process at the semiconductor electrode (photosensitization) in a photoelectrochemical cell, the absorption spectrum of the test dye of 0.1 mM concentration in aqueous medium was determined and the same is shown in Figure4(a). This figure shows clearly that the dye can absorb visible light in the range of 400–620 nm wavelengths with characteristic absorption peak at 563 nm. With this sensitizer it seems possible to extend the spectral response of the ZnO electrodes well into the visible region of the solar spectrum (up to ~620 nm wavelength). Thus, this compound absorbs light of appropriate wavelength and can be used as photosensitizer for wide-band gap semiconductors such as ZnO (Eg=3.48eV) which alone cannot absorb visible light. Figure 4(b) shows the absorption spectrum of Ni(II)-xylenol complex dye coated-ZnO thin-film electrode.Figure 4
Absorption spectra of (a) aqueous solution of Ni(II) xylenol complex (0.1 mM) and (b) ZnO/Ni(II) xylenol complex thin film electrode.


#### 3.3.4. Energy Level Diagram

In order to study that the photo induced electron injection by dye molecules into the conduction band of ZnO electrode and the dye regeneration processes are thermodynamically feasible or not, an energy level diagram has been constructed on electrochemical scale. The flat band potential of the ZnO electrode (−506 mV) has been obtained from the current-potential plot (discussed later) which provided the position of the Fermi level at the surface of the semiconductor electrode under flat band condition. Assuming the conduction band edge at 0.1 eV above the Fermi level, we getECB=-606mV. Since Eg=3.48eV for nanocrystalline ZnO, the upper edge of the valence band was taken at +2.874 V. Further, the oxidation potential of the dye (ED/D+0 = +0.420 V) determined from the cyclic voltammetry provided the electron donating energy level of the dye molecules in their ground state (D) (Figure 5). This coupled with the excitation energy of the dye (2.2 eV corresponding to λmax=563nm) provided the electron-donating energy level of the excited dye molecules (D*) as ED*/D+0=-1.78V. The redox potential of I-/I3- (0.5 V) was taken from the literature. The energy level diagram clearly demonstrates that both the processes, (i) electron injection by photoexcited dye molecules into the conduction band of the semiconductor and (ii) regeneration of dye (D++e-→D) are thermodynamically feasible. To examine the kinetic aspects of the photo-induced electron transfer processes in terms of obtainable dye-sensitized photocurrent, the following experiments were performed.Figure 5
Schematic energy level diagram for injection of electrons from an adsorbed dye molecule in excited state (D*) to the conduction band of ZnO and a subsequent regeneration of the dye.


#### 3.3.5. Current-Potential Characteristics

In order to assess the sensitizing ability of the dye, current-potential (J-V) curves were determined using dye-coated ZnO thin film as photoanode and Pt (screen-printed) as counter electrode in a sandwich type cell having I-/I3- redox couple in the cell electrolyte. The current-potential characteristics recorded under visible and white light illumination are shown in Figure 6. Open circuit cell voltage Voc=506mV and short circuit photocurrent Jsc = 1.68 mA/cm2 were observed under white light (Figure 6(a)) and open circuit cell voltage Voc=506mV and short circuit photocurrent Jsc=1.4mA/cm2  were observed under visible light (Figure 6(b)). Actual illuminated area of the working electrode was 0.23 cm2. From these curves, it is evident that photocurrent onset occurs at around 0.506 V, and hence it can be taken as the flat band potential (Vfb) of the ZnO electrode in the experimental solution. This value of Vfb has been used in constructing the energy level diagram (Figure 5).Figure 6
J-V characteristics of the dye-sensitized solar cell (nanocrystalline dye-coated ZnO thin film/electrolyte/Pt counter electrode) under illumination with (a) white light (520 mW/cm2) and (b) visible light (480 mW/cm2). Illuminated area = 0.23 cm2.


#### 3.3.6. Dependence of Photocurrent on Intensity of Light

Keeping the semiconductor electrode under at short circuit condition, it was illuminated with white light of different intensities using neutral density filters and the responded currents were measured and the results are shown in Figure 7. The linear variation in photocurrent with the intensity of light shows that the recombination of dye-injected charge carriers is almost negligible in this case.Figure 7
Short circuit photocurrent as a function of intensity of light for nanocrystalline ZnO/dye-sensitized solar cell.


#### 3.3.7. Transient Photocurrent Response

The transient current-time profiles were recorded to know the sustainability of the photocurrent observed initially on illumination of the semiconductor electrode. For such an assessment, the time dependent response of dye-sensitized ZnO electrode to light was determined in terms of short circuit photocurrent and the results are shown in Figure8. These photocurrent-time (Jphoto-t) profiles were obtained under illumination of the semiconductor electrode with white light (curve a) and visible light (curve b). Under white light illumination, the photocurrent attained initially was not sustained subsequently and it decayed to 95% of its initial value before getting stabilized (curve a). But under visible light illumination, no such decay in photocurrent was observed (curve b). The observed decay in photocurrent in the first case (curve a) is probably due to high intensity of the white light, which makes the loss due to charge carriers’ recombination more significant. This may also be the result of slowness of dye regeneration process as compared to charger carriers’ injection by excited dye molecules.Figure 8
Transient current-time (J-t) curves for nanocrystalline ZnO/dye-sensitized solar cell under short circuit condition and illumination with (a) white light and (b) visible light.


#### 3.3.8. Incident Photon-to-Current Conversion Efficiency (IPCE)

Incident photon-to-current conversion efficiency (IPCE) was evaluated for each wavelength of monochromatic light. From the value of short circuit photocurrentJsc and the intensity of the corresponding monochromatic light (Iinc), the incident photon-to-current conversion efficiency (IPCE) was calculated at each excitation wavelength (λ) using the following relation:(2)IPCE(%)=1240Jsc(mAcm-2)λ(nm)×Iinc(Wcm-2)×100.
Maximum IPCE for the present system was found to be 8.7 % (Figure 9) at wavelength (λmax=563nm) which is comparable to that reported for recently synthesized ruthenium metal complex by Funaki et al. [33]. The decrease in IPCE towards the longer wavelength region (above 563 nm) ws ascribed to the decrease of light harvesting by the dye.Figure 9
The IPCE as a function of the wavelength of incident monochromatic light
for sandwich type nanocrystalline ZnO-dye-sensitized solar cell.


#### 3.3.9. Evaluation of Fill Factor (FF)

For the determination of fill factor of the cell, current was recorded as a faction of cell voltage keeping the sandwich cell illuminated with desired light. The maximum powerPmax was determined from current-potential curve by choosing a point on the curve corresponding to which the product of the current Jmax and potential Vmax gives the maximum value. The fill factor (FF) was then calculated by using the equation(3)FF=Jmax⁡×Vmax⁡Jsc×Voc,
where Iinc is the power of incident light (520 mW/cm2 for white light and 480 mW/cm2 in visible light), Voc the open-circuit photovoltage and Jsc the short-circuit photocurrent. It was seen that DSSCs with this ZnO thin film achieved short circuit current (Jsc) of 1.68 mA/cm2, open circuit voltage of 506 mV, and a fill factor of 41% under white light and short circuit current (Jsc) of 1.4 mA/cm2, open circuit voltage of 506 mV, and a fill factor of 49% under visible light illumination conditions.Based on the findings of these investigations it can be concluded that xylenol Ni(II) metal complex can extend the spectral response of high band-gap semiconductor electrodes to visible light (up to about 600 nm wavelength). The dye used in this study was unable to harvest the majority of the energy from the solar spectrum since this dye has significant light absorption only up to~600 nm. It is due to the formation of aggregates as well as lack of harvesting ability in the longer wavelength region, that is, poor overlapping of the radiation spectrum of light source (here xenon lamp) and the absorption spectrum of the dye. Efficiency can possibly be improved on optimization of various components such as by using catalyst-coated counter electrode, kinetically more efficient redox couple, sensitizing other metal semiconducting thin films (i.e., TiO2, CdS, etc.), and so on. Another possible way of improving the performance is to use appropriate metal ion, other than Nickel (II), with proper energy levels reacting with (3,30-bis[N,N-di(carboxymethyl)aminomethyl]-o-cresolsulfonephthalein) ligand which can have absorption bands at larger wavelengths [34]. Efforts in this direction are underway.


## 3.1. Structural Characterization of ZnO Thin Film

The crystalline structure of the ZnO particles was analyzed through X-ray diffraction (XRD). The XRD of ZnO powder annealed at 450°C is shown in Figure1. The diffraction peaks of the sample reveals that ZnO crystallizes well after annealing. All the diffraction peaks are in agreement with the reported data in JCPDS Card no. 36-1451 for hexagonal wurtzite phase of zinc oxide. Average grain size has been calculated using Scherrer’s equation(1)d=0.9λBcos⁡θ,
where λ,θ, and B are the X-ray wavelength (1.54 Å), Braggs diffraction angle, and full width at half maximum (FWHM), respectively. The calculated average size of zinc oxide nanoparticles was found to be ~30–35 nm, which is in agreements with that already reported using this method of sol preparation [31].Figure 1
XRD of ZnO powder prepared by Spenhel and Anderson method and sintered at 450°C.


## 3.2. Surface Morphology

Figure2 show the SEM image of ZnO thin film prepared by depositing the colloidal sol on conducting glass and annealed at 450°C. The film shows a smooth porous surface with a fine microstructure, without cracks or void.Figure 2
SEM image of the nanocrystalline thin film prepared by using zinc oxide colloidal sol (annealing conditions: at 450°C in air for 1.5 h).


## 3.3. Characterization of Ni(II) Xylenol Metal Complex

### 3.3.1. Structure of the Complex

Ligand Na4H2L (Scheme 1) has several bonding sites, but the two acidic chelating groups on the side of its large sulphonphthalein nucleus may behave like branched donating sites enhancing the possibility of mononuclear or binuclear complex formation with metal ions. In binuclear complex formation, both sides of the sulphonphthalein nucleus are chelated by PhO-, N, and two COO- electron pairs. Empirical formulae derived from analytical data (C, H, N, S, and metal contents) suggest the formation of 1 : 1 (M : L) complexes. The assumption of 4 : 1 complex electrolyte can be confirmed by high molar conductance values (greater than 400Ω-1cm2mol-1) observed in 1 mM aqueous solution of the complex though the conductivity values are slightly lower than the value for uni-tetravalent electrolyte. The complex anion with 4- charge is voluminous and poorly mobile, considerably reducing its contribution to the molar conductivity [28]. Depending on pH, the chelation process indicates stepwise formation of stable complex species namely MH2L2-, MHL3-, and ML4- in solution.Scheme 1
Structure of ligand Na4H2L.Scheme2 represents the chemical structure of nickel (II) metal complexes with 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand as proposed by Pandey and Narang [28].Scheme 2
Structure of nickel (II) metal complex with 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand as proposed by Pandey and Narang [28].Scheme 3
Schematic presentation of preparation of ZnO sol and its thin film on conducting glass substrate.


### 3.3.2. Redox Behaviour of Nickel (II) Xylenol Complex

The cyclic voltammograms of xylenol nickel (II) complex in aqueous solution containing 0.1 M NaClO4 obtained in the potential range of −1.5 V to 1.0 V at different scan rates (0.020–0.200Vs-1) are shown in Figure 3(a) while Figure 3(b) shows cyclic voltammograms (10 cycles) repeated at a fixed scan rate of 100 mV/s. No measurable shift in peak has been observed which shows that the complex is stable in solution. From these curves it is evident that during forward scan in anodic potential range one peak (b) (Ep,a=+0.420V) was observed. During the reverse scan cathodic peaks (c) and (d) were observed at (Ep,c)c=-0.112V and (Ep,c)d=-0.858V. The reoxidation anodic peak (a) (Ep,a=-0.732V) seems to be associated with the cathodic peak (d) but (b) has no associated cathodic peak. It is pertinent to point out here that though peaks (d) and (a) have been assigned to reduction of Ni(II) in complex cation to Ni (I) and its reversal, their separation ((Ep,a)a-(Ep,c)c) is quite large as compared to that expected for one electron transfer process and it is also not stable with the change in the scan rate from 20 to 200 mV/s. However, it can be added here that the cathodic peak potential (Ep,c=-0.858V) corresponding to (d) matches closely with the reduction potential Ep,c=-0.85V reported by Bulut [32] for the same cation in another transition metal complex. Ep,c shifting to more negative potentials (from −0.830 to −0.858 V) was observed when the scan rate was increased from 20 to 200 mV/s which confirms the irreversibility of the reduction process. The formal redox potential (Ef0=(Ep,a+Ep,c)/2) for the above mention process can be taken as −0.795 V. The oxidation potential (Ep,a)b=+0.420V provides the electron donating energy level of the test dye in its ground state with respect to reference electrode.(a) Cyclic voltammogram in aqueous medium containing 0.1 mM test dye + 0.1 M NaClO4 supporting electrolyte at different scan rates I-20, II-50, III-60, and IV-100 mV/s. (b) Cyclic voltammogram in aqueous medium containing 0.1 mM test dye + 0.1 M NaClO4  supporting electrolyte at scan rate of 100 mV/s (10 cycles).
(a)(b)


### 3.3.3. Optical Properties of Nickel Xylenol Complex

Since the optical property of a compound, to be used as a sensitizer, plays the significant role in mediating the photoelectrochemical process at the semiconductor electrode (photosensitization) in a photoelectrochemical cell, the absorption spectrum of the test dye of 0.1 mM concentration in aqueous medium was determined and the same is shown in Figure4(a). This figure shows clearly that the dye can absorb visible light in the range of 400–620 nm wavelengths with characteristic absorption peak at 563 nm. With this sensitizer it seems possible to extend the spectral response of the ZnO electrodes well into the visible region of the solar spectrum (up to ~620 nm wavelength). Thus, this compound absorbs light of appropriate wavelength and can be used as photosensitizer for wide-band gap semiconductors such as ZnO (Eg=3.48eV) which alone cannot absorb visible light. Figure 4(b) shows the absorption spectrum of Ni(II)-xylenol complex dye coated-ZnO thin-film electrode.Figure 4
Absorption spectra of (a) aqueous solution of Ni(II) xylenol complex (0.1 mM) and (b) ZnO/Ni(II) xylenol complex thin film electrode.


### 3.3.4. Energy Level Diagram

In order to study that the photo induced electron injection by dye molecules into the conduction band of ZnO electrode and the dye regeneration processes are thermodynamically feasible or not, an energy level diagram has been constructed on electrochemical scale. The flat band potential of the ZnO electrode (−506 mV) has been obtained from the current-potential plot (discussed later) which provided the position of the Fermi level at the surface of the semiconductor electrode under flat band condition. Assuming the conduction band edge at 0.1 eV above the Fermi level, we getECB=-606mV. Since Eg=3.48eV for nanocrystalline ZnO, the upper edge of the valence band was taken at +2.874 V. Further, the oxidation potential of the dye (ED/D+0 = +0.420 V) determined from the cyclic voltammetry provided the electron donating energy level of the dye molecules in their ground state (D) (Figure 5). This coupled with the excitation energy of the dye (2.2 eV corresponding to λmax=563nm) provided the electron-donating energy level of the excited dye molecules (D*) as ED*/D+0=-1.78V. The redox potential of I-/I3- (0.5 V) was taken from the literature. The energy level diagram clearly demonstrates that both the processes, (i) electron injection by photoexcited dye molecules into the conduction band of the semiconductor and (ii) regeneration of dye (D++e-→D) are thermodynamically feasible. To examine the kinetic aspects of the photo-induced electron transfer processes in terms of obtainable dye-sensitized photocurrent, the following experiments were performed.Figure 5
Schematic energy level diagram for injection of electrons from an adsorbed dye molecule in excited state (D*) to the conduction band of ZnO and a subsequent regeneration of the dye.


### 3.3.5. Current-Potential Characteristics

In order to assess the sensitizing ability of the dye, current-potential (J-V) curves were determined using dye-coated ZnO thin film as photoanode and Pt (screen-printed) as counter electrode in a sandwich type cell having I-/I3- redox couple in the cell electrolyte. The current-potential characteristics recorded under visible and white light illumination are shown in Figure 6. Open circuit cell voltage Voc=506mV and short circuit photocurrent Jsc = 1.68 mA/cm2 were observed under white light (Figure 6(a)) and open circuit cell voltage Voc=506mV and short circuit photocurrent Jsc=1.4mA/cm2  were observed under visible light (Figure 6(b)). Actual illuminated area of the working electrode was 0.23 cm2. From these curves, it is evident that photocurrent onset occurs at around 0.506 V, and hence it can be taken as the flat band potential (Vfb) of the ZnO electrode in the experimental solution. This value of Vfb has been used in constructing the energy level diagram (Figure 5).Figure 6
J-V characteristics of the dye-sensitized solar cell (nanocrystalline dye-coated ZnO thin film/electrolyte/Pt counter electrode) under illumination with (a) white light (520 mW/cm2) and (b) visible light (480 mW/cm2). Illuminated area = 0.23 cm2.


### 3.3.6. Dependence of Photocurrent on Intensity of Light

Keeping the semiconductor electrode under at short circuit condition, it was illuminated with white light of different intensities using neutral density filters and the responded currents were measured and the results are shown in Figure 7. The linear variation in photocurrent with the intensity of light shows that the recombination of dye-injected charge carriers is almost negligible in this case.Figure 7
Short circuit photocurrent as a function of intensity of light for nanocrystalline ZnO/dye-sensitized solar cell.


### 3.3.7. Transient Photocurrent Response

The transient current-time profiles were recorded to know the sustainability of the photocurrent observed initially on illumination of the semiconductor electrode. For such an assessment, the time dependent response of dye-sensitized ZnO electrode to light was determined in terms of short circuit photocurrent and the results are shown in Figure8. These photocurrent-time (Jphoto-t) profiles were obtained under illumination of the semiconductor electrode with white light (curve a) and visible light (curve b). Under white light illumination, the photocurrent attained initially was not sustained subsequently and it decayed to 95% of its initial value before getting stabilized (curve a). But under visible light illumination, no such decay in photocurrent was observed (curve b). The observed decay in photocurrent in the first case (curve a) is probably due to high intensity of the white light, which makes the loss due to charge carriers’ recombination more significant. This may also be the result of slowness of dye regeneration process as compared to charger carriers’ injection by excited dye molecules.Figure 8
Transient current-time (J-t) curves for nanocrystalline ZnO/dye-sensitized solar cell under short circuit condition and illumination with (a) white light and (b) visible light.


### 3.3.8. Incident Photon-to-Current Conversion Efficiency (IPCE)

Incident photon-to-current conversion efficiency (IPCE) was evaluated for each wavelength of monochromatic light. From the value of short circuit photocurrentJsc and the intensity of the corresponding monochromatic light (Iinc), the incident photon-to-current conversion efficiency (IPCE) was calculated at each excitation wavelength (λ) using the following relation:(2)IPCE(%)=1240Jsc(mAcm-2)λ(nm)×Iinc(Wcm-2)×100.
Maximum IPCE for the present system was found to be 8.7 % (Figure 9) at wavelength (λmax=563nm) which is comparable to that reported for recently synthesized ruthenium metal complex by Funaki et al. [33]. The decrease in IPCE towards the longer wavelength region (above 563 nm) ws ascribed to the decrease of light harvesting by the dye.Figure 9
The IPCE as a function of the wavelength of incident monochromatic light
for sandwich type nanocrystalline ZnO-dye-sensitized solar cell.


### 3.3.9. Evaluation of Fill Factor (FF)

For the determination of fill factor of the cell, current was recorded as a faction of cell voltage keeping the sandwich cell illuminated with desired light. The maximum powerPmax was determined from current-potential curve by choosing a point on the curve corresponding to which the product of the current Jmax and potential Vmax gives the maximum value. The fill factor (FF) was then calculated by using the equation(3)FF=Jmax⁡×Vmax⁡Jsc×Voc,
where Iinc is the power of incident light (520 mW/cm2 for white light and 480 mW/cm2 in visible light), Voc the open-circuit photovoltage and Jsc the short-circuit photocurrent. It was seen that DSSCs with this ZnO thin film achieved short circuit current (Jsc) of 1.68 mA/cm2, open circuit voltage of 506 mV, and a fill factor of 41% under white light and short circuit current (Jsc) of 1.4 mA/cm2, open circuit voltage of 506 mV, and a fill factor of 49% under visible light illumination conditions.Based on the findings of these investigations it can be concluded that xylenol Ni(II) metal complex can extend the spectral response of high band-gap semiconductor electrodes to visible light (up to about 600 nm wavelength). The dye used in this study was unable to harvest the majority of the energy from the solar spectrum since this dye has significant light absorption only up to~600 nm. It is due to the formation of aggregates as well as lack of harvesting ability in the longer wavelength region, that is, poor overlapping of the radiation spectrum of light source (here xenon lamp) and the absorption spectrum of the dye. Efficiency can possibly be improved on optimization of various components such as by using catalyst-coated counter electrode, kinetically more efficient redox couple, sensitizing other metal semiconducting thin films (i.e., TiO2, CdS, etc.), and so on. Another possible way of improving the performance is to use appropriate metal ion, other than Nickel (II), with proper energy levels reacting with (3,30-bis[N,N-di(carboxymethyl)aminomethyl]-o-cresolsulfonephthalein) ligand which can have absorption bands at larger wavelengths [34]. Efforts in this direction are underway.


## 3.3.1. Structure of the Complex

Ligand Na4H2L (Scheme 1) has several bonding sites, but the two acidic chelating groups on the side of its large sulphonphthalein nucleus may behave like branched donating sites enhancing the possibility of mononuclear or binuclear complex formation with metal ions. In binuclear complex formation, both sides of the sulphonphthalein nucleus are chelated by PhO-, N, and two COO- electron pairs. Empirical formulae derived from analytical data (C, H, N, S, and metal contents) suggest the formation of 1 : 1 (M : L) complexes. The assumption of 4 : 1 complex electrolyte can be confirmed by high molar conductance values (greater than 400Ω-1cm2mol-1) observed in 1 mM aqueous solution of the complex though the conductivity values are slightly lower than the value for uni-tetravalent electrolyte. The complex anion with 4- charge is voluminous and poorly mobile, considerably reducing its contribution to the molar conductivity [28]. Depending on pH, the chelation process indicates stepwise formation of stable complex species namely MH2L2-, MHL3-, and ML4- in solution.Scheme 1
Structure of ligand Na4H2L.Scheme2 represents the chemical structure of nickel (II) metal complexes with 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand as proposed by Pandey and Narang [28].Scheme 2
Structure of nickel (II) metal complex with 3,30-bis[N,N-di(carboxymethyl)-aminomethyl]-o-cresol sulphonphthalein ligand as proposed by Pandey and Narang [28].Scheme 3
Schematic presentation of preparation of ZnO sol and its thin film on conducting glass substrate.


## 3.3.2. Redox Behaviour of Nickel (II) Xylenol Complex

The cyclic voltammograms of xylenol nickel (II) complex in aqueous solution containing 0.1 M NaClO4 obtained in the potential range of −1.5 V to 1.0 V at different scan rates (0.020–0.200Vs-1) are shown in Figure 3(a) while Figure 3(b) shows cyclic voltammograms (10 cycles) repeated at a fixed scan rate of 100 mV/s. No measurable shift in peak has been observed which shows that the complex is stable in solution. From these curves it is evident that during forward scan in anodic potential range one peak (b) (Ep,a=+0.420V) was observed. During the reverse scan cathodic peaks (c) and (d) were observed at (Ep,c)c=-0.112V and (Ep,c)d=-0.858V. The reoxidation anodic peak (a) (Ep,a=-0.732V) seems to be associated with the cathodic peak (d) but (b) has no associated cathodic peak. It is pertinent to point out here that though peaks (d) and (a) have been assigned to reduction of Ni(II) in complex cation to Ni (I) and its reversal, their separation ((Ep,a)a-(Ep,c)c) is quite large as compared to that expected for one electron transfer process and it is also not stable with the change in the scan rate from 20 to 200 mV/s. However, it can be added here that the cathodic peak potential (Ep,c=-0.858V) corresponding to (d) matches closely with the reduction potential Ep,c=-0.85V reported by Bulut [32] for the same cation in another transition metal complex. Ep,c shifting to more negative potentials (from −0.830 to −0.858 V) was observed when the scan rate was increased from 20 to 200 mV/s which confirms the irreversibility of the reduction process. The formal redox potential (Ef0=(Ep,a+Ep,c)/2) for the above mention process can be taken as −0.795 V. The oxidation potential (Ep,a)b=+0.420V provides the electron donating energy level of the test dye in its ground state with respect to reference electrode.(a) Cyclic voltammogram in aqueous medium containing 0.1 mM test dye + 0.1 M NaClO4 supporting electrolyte at different scan rates I-20, II-50, III-60, and IV-100 mV/s. (b) Cyclic voltammogram in aqueous medium containing 0.1 mM test dye + 0.1 M NaClO4  supporting electrolyte at scan rate of 100 mV/s (10 cycles).
(a)(b)


## 3.3.3. Optical Properties of Nickel Xylenol Complex

Since the optical property of a compound, to be used as a sensitizer, plays the significant role in mediating the photoelectrochemical process at the semiconductor electrode (photosensitization) in a photoelectrochemical cell, the absorption spectrum of the test dye of 0.1 mM concentration in aqueous medium was determined and the same is shown in Figure4(a). This figure shows clearly that the dye can absorb visible light in the range of 400–620 nm wavelengths with characteristic absorption peak at 563 nm. With this sensitizer it seems possible to extend the spectral response of the ZnO electrodes well into the visible region of the solar spectrum (up to ~620 nm wavelength). Thus, this compound absorbs light of appropriate wavelength and can be used as photosensitizer for wide-band gap semiconductors such as ZnO (Eg=3.48eV) which alone cannot absorb visible light. Figure 4(b) shows the absorption spectrum of Ni(II)-xylenol complex dye coated-ZnO thin-film electrode.Figure 4
Absorption spectra of (a) aqueous solution of Ni(II) xylenol complex (0.1 mM) and (b) ZnO/Ni(II) xylenol complex thin film electrode.


## 3.3.4. Energy Level Diagram

In order to study that the photo induced electron injection by dye molecules into the conduction band of ZnO electrode and the dye regeneration processes are thermodynamically feasible or not, an energy level diagram has been constructed on electrochemical scale. The flat band potential of the ZnO electrode (−506 mV) has been obtained from the current-potential plot (discussed later) which provided the position of the Fermi level at the surface of the semiconductor electrode under flat band condition. Assuming the conduction band edge at 0.1 eV above the Fermi level, we getECB=-606mV. Since Eg=3.48eV for nanocrystalline ZnO, the upper edge of the valence band was taken at +2.874 V. Further, the oxidation potential of the dye (ED/D+0 = +0.420 V) determined from the cyclic voltammetry provided the electron donating energy level of the dye molecules in their ground state (D) (Figure 5). This coupled with the excitation energy of the dye (2.2 eV corresponding to λmax=563nm) provided the electron-donating energy level of the excited dye molecules (D*) as ED*/D+0=-1.78V. The redox potential of I-/I3- (0.5 V) was taken from the literature. The energy level diagram clearly demonstrates that both the processes, (i) electron injection by photoexcited dye molecules into the conduction band of the semiconductor and (ii) regeneration of dye (D++e-→D) are thermodynamically feasible. To examine the kinetic aspects of the photo-induced electron transfer processes in terms of obtainable dye-sensitized photocurrent, the following experiments were performed.Figure 5
Schematic energy level diagram for injection of electrons from an adsorbed dye molecule in excited state (D*) to the conduction band of ZnO and a subsequent regeneration of the dye.


## 3.3.5. Current-Potential Characteristics

In order to assess the sensitizing ability of the dye, current-potential (J-V) curves were determined using dye-coated ZnO thin film as photoanode and Pt (screen-printed) as counter electrode in a sandwich type cell having I-/I3- redox couple in the cell electrolyte. The current-potential characteristics recorded under visible and white light illumination are shown in Figure 6. Open circuit cell voltage Voc=506mV and short circuit photocurrent Jsc = 1.68 mA/cm2 were observed under white light (Figure 6(a)) and open circuit cell voltage Voc=506mV and short circuit photocurrent Jsc=1.4mA/cm2  were observed under visible light (Figure 6(b)). Actual illuminated area of the working electrode was 0.23 cm2. From these curves, it is evident that photocurrent onset occurs at around 0.506 V, and hence it can be taken as the flat band potential (Vfb) of the ZnO electrode in the experimental solution. This value of Vfb has been used in constructing the energy level diagram (Figure 5).Figure 6
J-V characteristics of the dye-sensitized solar cell (nanocrystalline dye-coated ZnO thin film/electrolyte/Pt counter electrode) under illumination with (a) white light (520 mW/cm2) and (b) visible light (480 mW/cm2). Illuminated area = 0.23 cm2.


## 3.3.6. Dependence of Photocurrent on Intensity of Light

Keeping the semiconductor electrode under at short circuit condition, it was illuminated with white light of different intensities using neutral density filters and the responded currents were measured and the results are shown in Figure 7. The linear variation in photocurrent with the intensity of light shows that the recombination of dye-injected charge carriers is almost negligible in this case.Figure 7
Short circuit photocurrent as a function of intensity of light for nanocrystalline ZnO/dye-sensitized solar cell.


## 3.3.7. Transient Photocurrent Response

The transient current-time profiles were recorded to know the sustainability of the photocurrent observed initially on illumination of the semiconductor electrode. For such an assessment, the time dependent response of dye-sensitized ZnO electrode to light was determined in terms of short circuit photocurrent and the results are shown in Figure8. These photocurrent-time (Jphoto-t) profiles were obtained under illumination of the semiconductor electrode with white light (curve a) and visible light (curve b). Under white light illumination, the photocurrent attained initially was not sustained subsequently and it decayed to 95% of its initial value before getting stabilized (curve a). But under visible light illumination, no such decay in photocurrent was observed (curve b). The observed decay in photocurrent in the first case (curve a) is probably due to high intensity of the white light, which makes the loss due to charge carriers’ recombination more significant. This may also be the result of slowness of dye regeneration process as compared to charger carriers’ injection by excited dye molecules.Figure 8
Transient current-time (J-t) curves for nanocrystalline ZnO/dye-sensitized solar cell under short circuit condition and illumination with (a) white light and (b) visible light.


## 3.3.8. Incident Photon-to-Current Conversion Efficiency (IPCE)

Incident photon-to-current conversion efficiency (IPCE) was evaluated for each wavelength of monochromatic light. From the value of short circuit photocurrentJsc and the intensity of the corresponding monochromatic light (Iinc), the incident photon-to-current conversion efficiency (IPCE) was calculated at each excitation wavelength (λ) using the following relation:(2)IPCE(%)=1240Jsc(mAcm-2)λ(nm)×Iinc(Wcm-2)×100.
Maximum IPCE for the present system was found to be 8.7 % (Figure 9) at wavelength (λmax=563nm) which is comparable to that reported for recently synthesized ruthenium metal complex by Funaki et al. [33]. The decrease in IPCE towards the longer wavelength region (above 563 nm) ws ascribed to the decrease of light harvesting by the dye.Figure 9
The IPCE as a function of the wavelength of incident monochromatic light
for sandwich type nanocrystalline ZnO-dye-sensitized solar cell.


## 3.3.9. Evaluation of Fill Factor (FF)

For the determination of fill factor of the cell, current was recorded as a faction of cell voltage keeping the sandwich cell illuminated with desired light. The maximum powerPmax was determined from current-potential curve by choosing a point on the curve corresponding to which the product of the current Jmax and potential Vmax gives the maximum value. The fill factor (FF) was then calculated by using the equation(3)FF=Jmax⁡×Vmax⁡Jsc×Voc,
where Iinc is the power of incident light (520 mW/cm2 for white light and 480 mW/cm2 in visible light), Voc the open-circuit photovoltage and Jsc the short-circuit photocurrent. It was seen that DSSCs with this ZnO thin film achieved short circuit current (Jsc) of 1.68 mA/cm2, open circuit voltage of 506 mV, and a fill factor of 41% under white light and short circuit current (Jsc) of 1.4 mA/cm2, open circuit voltage of 506 mV, and a fill factor of 49% under visible light illumination conditions.Based on the findings of these investigations it can be concluded that xylenol Ni(II) metal complex can extend the spectral response of high band-gap semiconductor electrodes to visible light (up to about 600 nm wavelength). The dye used in this study was unable to harvest the majority of the energy from the solar spectrum since this dye has significant light absorption only up to~600 nm. It is due to the formation of aggregates as well as lack of harvesting ability in the longer wavelength region, that is, poor overlapping of the radiation spectrum of light source (here xenon lamp) and the absorption spectrum of the dye. Efficiency can possibly be improved on optimization of various components such as by using catalyst-coated counter electrode, kinetically more efficient redox couple, sensitizing other metal semiconducting thin films (i.e., TiO2, CdS, etc.), and so on. Another possible way of improving the performance is to use appropriate metal ion, other than Nickel (II), with proper energy levels reacting with (3,30-bis[N,N-di(carboxymethyl)aminomethyl]-o-cresolsulfonephthalein) ligand which can have absorption bands at larger wavelengths [34]. Efforts in this direction are underway.


## 4. Conclusion

A new transition metal complex has been studied for its photosensitizing properties by using it in dye-sensitized solar cell. Based on the findings of the present investigations, it can be concluded that Ni(II) xylenol metal complex acts as a donor-type sensitizer, and it is capable of extending the spectral response of ZnO electrode up to~600 nm wavelength of visible light. The absorption spectrum of aqueous solution of this complex exhibits a strong peak at 563 nm and a shoulder at 526 nm wavelength of light. The sandwich-type dye-sensitized solar cell using ZnO semiconducting thin film with test dye anchored onto it showed the cell output as follows: Voc=0.506V,Jsc=1.68mAcm-2, and FF=0.41 under illumination with full spectrum of light (intensity = 520 mW cm-2) while on illumination with visible light (λ>420nm, intensity 480 mW cm-2) Voc=0.506V,Jsc=1.4mAcm-2, and FF=0.49 were achieved. Maximum incident photon-to-current conversion efficiency for the present system was found to be 8.7% at wavelength (λmax=563nm).



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*Source: 980560-2011-04-05.xml*