Fabrication, optimization and characterization of natural dye sensitized solar cell

ABSTRACT The dyes extracted from pomegranate and berry fruits were successfully used in the fabrication of natural dye sensitized solar cells (NDSSC). The morphology, porosity, surface

roughness, thickness, absorption and emission characteristics of the pomegranate dye sensitized photo-anode were studied using various analytical techniques including FESEM, EDS, TEM, AFM,

FTIR, Raman, Fluorescence and Absorption Spectroscopy. Pomegranate dye extract has been shown to contain anthocyanin which is an excellent light harvesting pigment needed for the generation

of charge carriers for the production of electricity. The solar cell’s photovoltic performance in terms of efficiency, voltage, and current was tested with a standard illumination of

air-mass 1.5 global (AM 1.5 G) having an irradiance of 100 mW/cm2. After optimization of the photo-anode and counter electrode, a photoelectric conversion efficiency (_η_) of 2%, an

open-circuit voltage (_Voc_) of 0.39 mV, and a short-circuit current density (_Isc_) of 12.2 mA/cm2 were obtained. Impedance determination showed a relatively low charge-transfer resistance

(17.44 Ω) and a long lifetime, signifying a reduction in recombination losses. The relatively enhanced efficiency is attributable in part to the use of a highly concentrated pomegranate dye,

graphite counter electrode and TiCl4 treatment of the photo-anode. SIMILAR CONTENT BEING VIEWED BY OTHERS NATURAL SENSITIZER EXTRACTED FROM _MUSSAENDA ERYTHROPHYLLA_ FOR DYE-SENSITIZED

SOLAR CELL Article Open access 24 August 2023 PERFORMANCE OF YELLOW AND PINK OYSTER MUSHROOM DYES IN DYE SENSITIZED SOLAR CELL Article Open access 10 October 2024 USE OF CONGO RED

DYE-FORMALDEHYDE AS A NEW SENSITIZER-REDUCTANT COUPLE FOR ENHANCED SIMULTANEOUS SOLAR ENERGY CONVERSION AND STORAGE BY PHOTOGALVANIC CELLS AT THE LOW AND ARTIFICIAL SUN INTENSITY Article

Open access 06 November 2020 INTRODUCTION Solar energy is rapidly becoming the most viable, eco-friendly and sustainable alternate source of renewable energy1. There has been an exponential

growth in the production of solar cells over the past two decades1,2,3. One of the most promising means of solar energy conversion is the use of dye-sensitized solar cells (DSSC) first

developed by Grätzel _et al_. in 1991 and has attracted much attention in the last couple of decades leading to a plethora of publications on the subject4,5,6,7,8,9,10. The Interest in DSSC

and more precisely Natural Dye Sensitized Solar Cell (NDSSC) is mainly due to its low cost of fabrication and environmental friendly nature11,12. Currently, DSSC has the potential to convert

photons from sunlight to electrical energy at 13% efficiency13. An intensive effort has been directed towards the optimization of the various components of DSSC with the goal of fabricating

more efficient and stable cells. The DSSC as displayed in Fig. 1 is composed of a redox couple electrolyte system, typically iodide and triiodide complex, sandwiched between two glass

plates, a photo-anode and a counter electrode. The redox couple in the electrolyte is used to regenerate the oxidized dye. The photo-anode consist of glass plate coated with a thin layer of

transparent conductive oxide (Fluorine doped tin-oxide, FTO or Indium doped tin-oxide, ITO) and a monocrystalline semiconductor (usually titanium dioxide, TiO2) which serves as a scaffold

for the dye sensitizer. The counter electrode is also made up FTO covered glass slide coated usually with a thin film of Platinum or Carbon for the catalysis of the redox reaction with

electrolyte. The total efficiency of the DSSC is dependent on the nature, optimization and compatibility of each one of the components of the solar cell and more particularly the photo-anode

which plays a vital role in the charge generation and transfer processes. To increase the power conversion efficiency of DSSC, a nanostructured porous titanium dioxide with a wide band gap

and large exciton binding energy is typically used in constructing the photo-anode. The large surface area of the nanostructured TiO2 insures the adsorption of sufficiently large number

number of dye molecules for efficient harvesting of radiant energy. The dye, typically, with a wide and intense absorption spectrum is adsorbed on the TiO2 via anchoring groups such as

carboxylic, carbonyl and hydroxyl located on the dye molecule. A strong adsorption of the dye unto the nanostructured TiO2 is required for the efficient electron injection into the

conduction band of the TiO2 semiconductor. The dye sensitizer anchored on the surface of titanium dioxide absorbs photons and gets electronically excited. Energy is produced when the excited

electron moves from the valence band to the conduction band of the semiconductor. The electrolyte (I−/I3−) donates electron back to the dye. The sensitizers currently used in the

fabrication of solar cells are transition metal coordination complexes such as Ruthenium (II) carboxylated polypyridyl complexes, due to their intense charge-transfer absorption in the whole

visible range and highly efficient metal-ligand charge transfer transition (MLCT)14,15. Natural dyes are however more desirable than these synthetic dyes because they are more economical,

easily attainable, and abundant in supply and environmentally friendly5,16. In addition, they turn to have large absorption coefficient owing to allowed π to π* transitions. The performance

of various natural dye containing pigments such as anthocyanin17,18, xanthene14, chlorophyll, carotenoid and flavonoid have been thoroughly investigated11. These pigments are derived from

various plant parts such as flower petals, leaves, roots and fruits pulp/bark. In this study, juice extracted from pomegranate was investigated as potent sensitizer for DSSC in comparison to

other natural dyes. The pomegranate is a rich source of anthocyanin and we have deployed it as a sensitizer for the absorption of photons in DSSCs in the generation of electricity19.

Anthocyanins are polyphenolic ring-based flavonoids widely known for their antioxidant properties20. They differ from other flavonoids by the presence of a positive charge in the central

ring structure and are responsible for the intense colors of other fruits and vegetables such as the berries and red cabbages20. They have been shown to display a wide absorption/emission

band in the UV-Visible region of the spectrum as a result of electron charge transfer transitions16,21. RESULTS AND DISCUSSION ABSORPTION SPECTRA The overall performance of a DSSC is reliant

on the light absorption capability of the dye sensitizer and the diffusion of the ejected electron through the mesoporous TiO2 film. The optical properties of the dye extracted from

pomegranate were investigated using UV-vis spectrometry. The absorption spectra of pomegranate dye extract, bare TiO2 and pomegranate dye/TiO2 films are illustrated in Fig. 2a. The

Pomegranate dye extract exhibited an intense absorption broad band in the visible region with a peak at 510 nm. This intense absorption in the visible region (510 nm) matches with that

reported for anthocyanin and is the reason for the efficient harvesting of photons in NDSSC19. Plant parts containing anthocyanins have been widely investigated for use as photosensitizers

in the fabrication of NDSSC. In addition to their high absorption coefficient in the visible region of the electromagnetic spectrum, the presence of hydroxyl and carbonyl anchoring groups on

anthocyanins enable their adsorption unto the surface of the TiO2. This adsorption facilitates the transfer of the injected electron from dye to the conduction band of TiO2 which ultimately

enhances the efficiency of NDSSC5. A non-zero absorbance was observed for the spectrum corresponding to pomegranate dye/TiO2. The peak for anthocyanin in Pomegranate dye/TiO2 is not easily

visible in the spectrum, nonetheless, a shift in the maximum wavelength is observed. The absorption band of the pomegranate dye has been reported to be red shifted to about 550 nm upon

chelation to TiO222. The attachment of the anthocyanin containing dye onto TiO2 has been suggested to have an effect on the HOMO and LUMO level of anthocyanin, which consequently decreases

the band gap resulting in a redshift of the absorption peak23. The peak in the ultra-violet region is prominent and shows a bathochromic shift from 275 nm to 285 nm. A non-zero absorption

similar to that of pomegranate dye/TiO2 was also observed in spectrum of bare TiO2. The non-zero absorption has been attributed to diffused reflection of TiO2 suspended in solvent. Due to

the wideband gap of TiO2 (3.2 eV), bare TiO2 do not absorb visible light, hence, no absorption band is seen in the region extending from 400 nm to 700 nm as exhibited in Fig. 2a. Figure 2b

shows the fluorescence spectra of pomegranate dye, pomegranate dye/TiO2 and bare TiO2 employed in the fabrication of the NDSSC. The measurement was carried out with the exciting light in the

range of 320 nm ≤ λexc ≤ 600 nm. FOURIER TRANSFORMED INFRARED (FTIR) ANALYSIS The IR spectra of the films annealed at room temperature shows three vibrational modes (Fig. 3a) which are

ascribed to TiO2 for υO-H at 3413 cm−1, δO-H at 1622 cm−1, and υTi-O at 580 cm−1 as a broad stretching. The presence of pomegranate organic groups (Fig. 3b) such as hydroxyl, ethyl, acetyl

and ethoxide in the films23, shows stretching’s for υOH at 3649 cm−1, υO-H(water) at 3445 cm−1, υCH2, υCH3 at 2912, 2840 cm−1, δCH2, δCH3 at 1463, 1367 cm−1, δC-C at 1710 cm−1, δC=Cbenz at

1627 cm−1, υC–O at 1052 cm−1, and υTi-O-C at 654 cm−1, respectively. An interesting observation in these studies was that the stretching intensities were increased with the deposition of

pomegranate dye, with a significant change on the TiO2 IR modes, which indicates that there occurred an interaction that shift to low energies the initially TiO2 stretching. This observation

shows that the deposition of pomegranate dye undergoes strong phase transition due to an electronic environment change around the TiO2 energies24,25,26. RAMAN SPECTROSCOPY To further

evaluate the Pomegranate dye/TiO2 interaction in the nanocrystalline prepared films, Raman studies were performed in the range of 0–2500 cm−1 and the results are shown in Fig. 4. The D and G

bands at 1470 cm−1 and 1960 cm−1, respectively, have been previously attributed to the high disorder encountered for sp3 carbons27,28. The intense peak at 130 cm−1 assigned E(g) is present

in both of TiO2 (blue) and the hybrid of TiO2 and pomegranate (green), but it is absent in the measurement for pomegranate dye only. However, an interesting observation is that this 130 cm−1

peak, which is as a result of the symmetric stretching vibration of O−Ti−O in TiO2, is enhanced after the adsorption of the pomegranate dye. This observation proves that there is an

interaction between the TiO2 nanoparticles and the pomegranate dye. We speculate that the adsorbed pomegranate dye excited by the light source causes the enhancement of the E(g) peak of

TiO2. MORPHOLOGICAL STUDIES OF THE FABRICATED POMEGRANATE SENSITIZED SOLAR CELL Atomic force microscopy (AFM) images of the TiO2 electrode, before and after the addition of pomegranate dye

extract were obtained in order to examine the surface morphological characteristics of the nanocrystalline TiO2. The Fig. 5 shows the AFM images of bare TiO2 and pomegranate dye sensitized

TiO2 on FTO glass (dye/TiO2). The images were obtained in 5 μm × 5 μm and 2 μm × 2 μm areas (Fig. 5a and b), analyzed to obtain insight the roughness and topographic features of the samples.

Details of the surface structure of TiO2 at the nanometer scale were observed. A high degree of roughness was observed on the surface of both bare TiO2 and pomegranate dye/TiO2. The Root

mean square roughness of bare TiO2 was about 197.6 nm in the 5 μm × 5 μm scan area (Fig. 5a). Many TiO2 clusters and cracks were found as exhibited in the topographic image and the image

profile shown in Fig. 5(a–e). The rough surface of the TiO2 increases the surface area of the film enabling more pomegranate dye to be adsorbed, which consequently increases the absorption

of the incident light. The color distribution in the phase image of the dye/TiO2 was very uniform as shown in Fig. 5f, which is an indication that the pomegranate dye is uniformly

distributed over the whole TiO2 layer. FIELD EMISSION SCANNING ELECTRON MICROSCOPY IMAGING The morphological characteristics and elemental analysis of the TiO2 photo-anode were investigated

using Field-Emission Scanning Electron Microscopy (JSM 7100F, JEOL.COM) and Energy dispersive X-ray spectroscopy (EDS), respectively. No significant changes were observed in the surface

morphology of the samples before and after dye sensitization. The Fig. 6a displays the FESEM image of the TiO2 film with an adsorbed layer of pomegranate dye (pomegranate dye/TiO2). A highly

porous network of nanocrystalline TiO2 on FTO glass can be observed from the FESEM image. The EDS mapping analysis of the pomegranate dye/TiO2 (Fig. 6b) revealed the presence of carbon and

Titanium, corresponding to the major elements present in pomegranate dye and TiO2, respectively. The carbon content of pomegranate dye/TiO2 in comparison with the bare TiO2 was also

investigated with EDS. The relatively intense carbon peak in the spectra of the dye-sensitized TiO2 film (Fig. 6d) compared to the negligible carbon peak in spectra of the bare TiO2 film

(Fig. 6c) is indicative of a thorough adsorption of pomegranate dye onto the TiO2 film. Although carbon and oxygen are the structural elements of the pigments present in the pomegranate dye,

the peaks for oxygen are relatively the same in both EDS spectra (Fig. 6c and d) due to the oxygen component of TiO2. The Fig. 6e shows a cross sectional view of the Dye/TiO2 sample

exhibiting distinct layers of TiO2, FTO and the glass substrate. The elemental composition of the layers was confirmed by the EDS analysis and is displayed in Supplementary Fig. 7. The

thickness of FTO on the glass was found to be about 500 nm (nominated size: 400 nm) and Dye/TiO2 film was found to be approximately 7 μm. As compared to the TiO2 thin films prepared with

other techniques such as the electrophoretic deposition method and the chemical reduction method, the TiO2 film prepared by the spin coating method tend to possess a high void content, ample

surface irregularities and a high degree of roughness, consistent with the findings of this imaging studies29,30. Thus, the porous surface of the TiO2 photo-anode suggests an enhancement in

the adsorption of pomegranate dye into TiO2 structure. TRANSMISSION ELECTRON MICROSCOPY IMAGING The Transmission electron microscopy (TEM) images of the bare TiO2 nanoparticles and the

pomegranate dye sensitized TiO2 nanoparticles are displayed in Fig. 7. A monodispersed layer of spherical TiO2 nanoparticles with particle size in the range of 20–25 nm was observed (Fig. 7a

and b). The Fig. 7c and d clearly show the presence small spherical nanoparticles, likely dye particles, with size in the range of 1–3 nm well distributed and decorated on the surface of

the TiO2 particles with a lattice fringe. These spherical nanoparticles were not observed on the bare TiO2 nanoparticles as seen in the Fig. 7a and b which leads us to speculate that they

are indeed dye particles. The interaction between the pomegranate dye and the TiO2 nanoparticles results from the deprotonation of hydroxyl groups from the anthocyanin pigment. The selected

area electron diffraction (SAED) pattern of the dye/TiO2 film as displayed in Fig. 7(e) shows the crystalline nature of the TiO2 nanoparticles. The four bright concentric diffraction rings

in the SAED can be indexed as the (101), (004), and (200) planes of the anatase TiO2, and (220) plane of the rutile TiO2. The HRTEM image of the TiO2/dye (Fig. 7d), displays the lattice

fringe with an interlayer spacing of 0.3487 corresponding to the d-spacing of (101) planes in anatase TiO2 as shown in the Fig. 7f. SOLAR CONVERSION EFFICIENCY MEASUREMENT The solar cell’s

photovoltic performance in terms of efficiency, voltage, and current was tested with a standard illumination of air-mass 1.5 global (AM 1.5G) having an irradiance of 100 mW/cm2. After

optimization of the photoanode and counter electrode, a photoelectric conversion efficiency (_η_) of 2%, an open-circuit voltage (_Voc_) of 0.39 mV, and a short-circuit current density

(_Isc_) of 12.2 mA/cm2 were obtained. The enhanced cell efficiency is attributed to the robust dye purification procedures adopted, treatment of anode with TiCl4 and the use of graphite

counter electrode. A further treatment of TiO2 coated FTO glass with TiCl4 has been shown to provide more sites for dye adsorption leading to high dye concentration that ensure the

absorption of a greater amount of sunlight. The earlier fabrication carried out with just amorphous carbon and colloidal graphite (Fig. 8a) yielded 1.16% and 1.41% efficiencies,

respectively. The improved efficiency obtained is also higher than a 1.5% efficiency of a pomegranate sensitized solar cell previously published by Bazargan _et al_.22. This efficiency is

also higher than most natural dye sensitized solars as revealed in a review by Hug _et al_.11 and other reviews in which percent efficiency of solar cell made from natural dyes were mostly

less than one. The performance of the pomegranate dye as a potent sensitizer assessed in comparison with other dyes via the current, voltage, fill factor and conversion efficiency

measurement are displayed in Table 1. The data shows that pomegranate sensitizer efficiency is far greater than that of berry fruit dyes employed in the study. The natural dyes studied

included Blackberry, Cranberry and Blueberry dyes. Blackberry dye sensitized solar cell had the second highest efficiency (1.4%) followed by Cranberry sensitized solar cell (1.2%) and

Blueberry dye sensitized solar cell (0.40%). ELECTROCHEMICAL IMPEDANCE ANALYSIS The electrochemical impedance spectroscopy (EIS) has often been used to probe the kinetics and energetics of

charge transport and recombination in dye sensitized solar cells. The EIS were recorded in the frequency range between 1 Hz and 100 KHz. Figure 8c shows the Nyquist plot of the various dye

sensitized solar cells. Well-defined semicircles related to the charge transfer resistance between the counter electrode and redox (I−/I3−) electrolyte are shown in the high frequency

regions. In the EIS analysis, the pomegranate dye solar cell shows the smallest charge transfer resistance, 17.45 (Ω) compared to other dye cells: 85.38 Ω for blueberry, 68.94 Ω for

cranberry, and 33.50 Ω for blackberry respectively. All natural dyes have anthocyanin a pigment responsible for the harvesting of radiant energy. Pomegranate having a large percentage of

delphinidin possesses the ability to absorb more light than the other berries under consideration. This greater ability to absorb sunlight results in fast electron (hole) generation and

transport, hence a lower hole-electron recombination in the cell. The light absorption is not as good in the berry fruit dye extract resulting in poor electron generation leading to

relatively high resistance to the flow of electron at the TiO2/dye/electrolyte interphase. Despite, the observed equivalence between the resistance for all the cell series, they do possess

almost similar values. As shown in the I-V curve in the Fig. 8b, the pomegranate dye cell showed the highest efficiency because the low charge transfer resistance acted as the dominant

factor affecting the performance of the natural dye sensitized solar cells. Figure 8d shows the Bode phase plot for the NDSSC. The blackberry dye showed a big phase shift in the high

frequency region (the maximum frequency: 506 Hz) due to relatively small capacitance (52.8 μF) compared to that of the other dyes. Overall the performance of the pomegranate DSSC is better

than blackberry DSSC due to the electron transfer resistance of blackberry dye which is far higher than that of Pomegranate dye. WORKING PRINCIPLE OF DYE SENSITIZED CELL (DSSC) Upon

illumination, dye molecules (S) adsorbed on the TiO2 film absorb photon and are excited from the highest occupied molecular orbitals (HOMO) to the lowest unoccupied molecular orbital (LUMO)

state as shown in Fig. 9(a). The photo-excited dye species (S*) injects an electron into the conduction band of TiO2 electrode and becomes oxidized (S+). The oxidized dye species

subsequently accept an electron from the electrolyte (I−) and the ground state of the dye (S) is restored. The injected electron percolates through the mesoporous TiO2 film to the FTO layer

and is transported through an external circuit to a load where the work done is delivered as electrical energy. The electron from the external load diffuses to the cathode where it gets

transferred to the electrolyte, (I3−) so the electrolyte system is regenerated. Density Functional Theory (DFT) calculations were used to optimize the geometry of delphinidin molecule using

the software Spartan’ 14 from Wavefunction, Inc. Irvine, CA, USA. These calculations were used to determine the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular

orbital (LUMO) energies of delphinidin dye. The anthocyanidin, delphinidin, was chosen for the calculations because it has been shown that it’s derivative, delphinidin -3, 5-diglucoside is

the predominant anthocyanin present in pomegranate dye extract. The calculations gave a result for the HOMO of −8.71 eV and the result for the LUMO of −6.27 eV. The difference in the HOMO

and LUMO, which is the energy band gap, was found to be 2.44 eV. The HOMO and LUMO surfaces and orbital energy diagrams are shown in Fig. 9(b and c) respectively. In Fig. 9(b and c), the

blue and red regions represent positive and negative values of the orbitals, respectively. CONCLUSION Dye extract from pomegranate fruit was utilized as the light-harvesting analog in the

fabrication of a low cost, eco-friendly dye-sensitized solar cell. The chemical, structural, morphology and optical properties of the pomegranate/TiO2 coated FTO glass were investigated via

atomic force microscopy, field emission scanning electron microscopy, energy-dispersive x-ray spectroscopy, uv-vis and fluorescence spectroscopy. The fabricated DSSC showed an enhanced

solar-to-electrical energy conversion. Theoretical calculation on delphinidin, an anthocyanin derivative found in pomegranate resulted in a HOMO of −8.71 eV and LUMO of −6.27 which makes it

possible for effective electron transfer of charge from the LUMO of the pomegranate into the conduction band of TiO2. The regeneration of the dye by the redox electrolyte (I−/I3−) coupling

increases the lifetime of the dye. Also the narrower band gap of delphinidin (2.44 eV) increases the intramolecular electronic transition probabilities. The efficiency of the prepared

pomegranate sensitized solar cell was _η_ = 2.0%, and fill factor FF = 0.41 with the short circuit current (I_SC_) and open circuit voltage (V_OC_) being 12.2 mA/cm2 and 0.39 V respectively.

The excellent photovoltaics performance of the solar cell could be attributed to the high concentration of anthocyanins present in pomegranate dye used in the sensitization of the

nanocrystalline TiO2. The use of graphite as the counter electrode and TiCl4 treatment of the photo-anode improved the solar cell efficiency by more than one percent. EXPERIMENTAL METHODS

MATERIALS Titanium dioxide powder (Degussa P-25) was purchased from the institute of chemical education, university of Wisconsin-Madison, department of chemistry, Madison, WI, USA. Fluorine

tin oxide (FTO) conducting glass slides were purchased from Harford glass company, Hartford City, Indiana, USA. Sodium Hydroxide (NaOH), acetone (C3H6O), ethanol (C2H5OH) and acetic acid

(CH3CO2H) were purchased from Sigma-Aldrich (St. Louis, MS, USA) and were used without further purification. CHARACTERIZATION TECHNIQUES The morphology of each film was analyzed using field

emission scanning electron microscopy (Model FESEM: JSM-7100FA JEOL USA, Inc.). The surface morphological characteristics of the nanocrystalline TiO2 were experimentally evaluated using

Atomic Force Microscopy (AFM) manufactured by NT-MDT (Model: Solver next, NT-MDT). Absorption spectroscopy was carried out with UV-3600 Plus from Shimadzu, MD, USA. Emission spectroscopy was

measured with RF-5301PC from Shimadzu, MD, USA. (Raman Studies was carried A model DXR smart Raman spectrometer (Thermo Fisher Scientific Co., Ltd., USA). ATR spectra were obtained with a

Thermo Nicolet iS50 FTIR.) Transmission Electron Microscopy (TEM) images were acquired on JEM-1400 PLUS (JEOL USA, Peabody, Massachusetts, USA). The images were viewed using Digital

Micrograph software from GATAN (GATAN Inc., Pleasanton, CA, USA). TiO2 paste was printed on FTO glass using WS-650 Series Spin Processor from Laurell Technologies Corporation, PA, USA.

Carbon paint used in making cathode slides was purchased from TED PELLA, INC, USA. The cell performance was measured using 150 W fully reflective solar simulator with a standard illumination

of air-mass 1.5 global (AM 1.5 G) having an irridance of 100 mW/cm2 (Sciencetech Inc.), London, Ontario, Canada. Reference 600 Potentiostat/Galvanostat/ZRA from GAMRY Instruments

(Warminster, PA). HOMO and LUMO calculations were carried out using Spartan’14 software from Wavefunction, Inc. Irvine, CA, USA. NATURAL DYE EXTRACTION A fresh pomegranate and berry fruits

were peeled and the juice extracted from the pulp coats using a commercial fruit juice extractor. The extraction was followed by a sequence of filtration, centrifugation, and decantation to

remove any precipitate present in the crude extract. FABRICATION OF NDSSC The electrodes were prepared according to a previously published procedure with some modification31. The

Supplementary Fig. S1 shows a schematic of the stages involved in the fabrication of the pomegranate dye sensitized solar cell. The working electrode was prepared by depositing a thin film

of TiO2 on the conductive side of a fluorine doped tin oxide (FTO) glass using a spin coater and annealing the film at 380 °C for 2 hours. The TiO2 coated FTO glass was subsequently dipped

in TiCl4 solution for an hour and annealed again for 30 minutes. The substrate was then immersed in a freshly squeezed pomegranate juice for dye sensitization. To concentrate the sample,

pomegranate juice was lyophilized and dissolved in a minimum amount of water before dye sensitization. The counter electrode (cathode) was prepared by either depositing carbon soot on FTO

glass slide or painting this glass slide with colloidal graphite. The pomegranate dye sensitized and the carbon electrodes were assembled to form a solar cell by sandwiching a redox (I−/I3−)

electrolyte solution as displayed in Supplementary Fig. S1. ADDITIONAL INFORMATION HOW TO CITE THIS ARTICLE: Ghann, W. _et al_. Fabrication, Optimization and Characterization of Natural Dye

Sensitized Solar Cell. _Sci. Rep._ 7, 41470; doi: 10.1038/srep41470 (2017). PUBLISHER'S NOTE: Springer Nature remains neutral with regard to jurisdictional claims in published maps and

institutional affiliations. REFERENCES * Singh, G. K. Solar power generation by PV (photovoltaic) technology: A review. _Energy_ 53, 1–13 (2013). Article  Google Scholar  * Chen, W. et al.

Efficient and stable large-area perovskite solar cells with inorganic charge extraction layers. _Science_ 350, 944–948 (2015). Article  CAS  Google Scholar  * Yoo, K. et al. Completely

Transparent Conducting Oxide-Free and Flexible Dye-Sensitized Solar Cells Fabricated on Plastic Substrates. _ACS Nano_ 9, 3760–3771 (2015). Article  CAS  Google Scholar  * O’Regan, B. &

Gratzel, M. A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO2 films. _Nature_ 353, 737–740 (1991). Article  ADS  Google Scholar  * Narayan, M. R. Review: Dye

sensitized solar cells based on natural photosensitizers. _Renew Sust Energ Rev_ 16, 208–215 (2012). CAS  Google Scholar  * Hao, S., Wu, J., Huang, Y. & Lin, J. Natural dyes as

photosensitizers for dye-sensitized solar cell. _Sol. Energ_ 80, 209–214 (2006). Article  ADS  CAS  Google Scholar  * Shalini, S., Balasundara prabhu, R., Prasanna, S., Mallick, T. K. &

Senthilarasu, S. Review on natural dye sensitized solar cells: Operation, materials and methods. _Renew Sust Energ Rev_ 51, 1306–1325 (2015). Article  CAS  Google Scholar  * Sugathan, V.,

John, E. & Sudhakar, K. Recent improvements in dye sensitized solar cells: A review. _Renew Sust Energ Rev_ 52, 54–64 (2015). Article  CAS  Google Scholar  * Bahadur, K. I., Jyoti, N.

J., Kumar, M. P. & Suman, C. Dye-Sensitized Solar cell using extract of Punica Granatum L. Pomegranate (Bedana) as a Natural Sensitizer. _Research of J. Chem. Sci._ 2, 81–83 (2012).

Google Scholar  * Meyer, G. J. The 2010 Millennium Technology Grand Prize: Dye-Sensitized Solar Cells. _ACS Nano._ 4, 4337–4343 (2010). Article  CAS  Google Scholar  * Hug, H., Bader, M.,

Mair, P. & Glatzel, T. Biophotovoltaics: Natural pigments in dye-sensitized solar cells Appl. _Energy_ 115, 216–225 (2014). CAS  Google Scholar  * Ludin, N. A. et al. Review on the

development of natural dye photosensitizer for dye-sensitized solar cells. _Renew Sust Energ. Rev._ 31, 386–396 (2014). Article  CAS  Google Scholar  * Mathew, S. et al. Dye-sensitized solar

cells with 13% efficiency achieved through the molecular engineering of porphyrin sensitizers. _Nat. Chem_. 6, 242–247 (2014). Article  CAS  Google Scholar  * Karki, I. B., Nakarmi, J. J.,

Mandal, P. K. & Chatterjee, S. Absorption Spectra of Natural Dyes and Their Effect on Efficiency of ZnO Based Dye-Sensitized Solar Cells. _NJST_ 13, 179–185 (2013). Google Scholar  *

Duffy, N. W., Peter, L. M., Rajapakse, R. M. G. & Wijayantha, K. G. U. Investigation of the Kinetics of the Back Reaction of Electrons with Tri-Iodide in Dye-Sensitized Nanocrystalline

Photovoltaic Cells. _The J. Phys. Chem B._ 104, 8916–8919 (2000). Article  CAS  Google Scholar  * Hosseinnezhad, M., Moradian, S. & Gharanjig, K. Fruit extract dyes as photosensitizers

in solar cells. _Curr. Sci_. 109, 953–956 (2015). Article  CAS  Google Scholar  * Dai, Q. & Rabani, J. Photosensitization of nanocrystalline TiO2 films by anthocyanin dyes. _J. of

Photochem. Photobiol_. 148, 17–24 (2002). Article  CAS  Google Scholar  * Dai, Q. & Rabani, J. Photosensitization of nanocrystalline TiO2 films by pomegranate pigments with unusually

high efficiency in aqueous medium. _Chem Commun._ 20, 2142–2143 (2001). Article  Google Scholar  * Noda, Y., Kaneyuki, T., Mori, A. & Packer, L. Antioxidant activities of pomegranate

fruit extract and its anthocyanidins: delphinidin, cyanidin, and pelargonidin. _J Agric Food Chem_. 50, 166–171 (2002). Article  CAS  Google Scholar  * Hou, D.-X., Fujii, M., Terahara, N.

& Yoshimoto, M. Molecular Mechanisms Behind the Chemopreventive Effects of Anthocyanidins. _J Biomed Biotechnol_. 2004, 321–325 (2004). Article  Google Scholar  * Cherepy, N. J.,

Smestad, G. P., Grätzel, M. & Zhang, J. Z. Ultrafast Electron Injection: Implications for a Photoelectrochemical Cell Utilizing an Anthocyanin Dye-Sensitized TiO2 Nanocrystalline

Electrode. _J. Phys. Chem B_. 101, 9342–9351 (1997). Article  CAS  Google Scholar  * Bazargan, M. H., Byranvand, M., Kharat, N. & Fatholahi, L. _Optoelectron Adv Mat_. 5, 360–362 (2011).

CAS  Google Scholar  * Li, N., Pan, N., Danhong, Li & Lin, S. Natural Dye-Sensitized Solar Cells Based on Highly Ordered TiO2 Nanotube Arrays. _Int. J. Photoenergy._ 598753, 1–5 (2013).

Google Scholar  * Sivaranjani, K. & Gopinath, C. S. Porosity driven photocatalytic activity of wormhole mesoporous TiO2-xNx in direct sunlight. _J. Mater. Chem_. 21, 2639–2647, (2011).

Article  CAS  Google Scholar  * Kumar, P. M., Badrinarayanan, S. & Sastry, M. Nanocrystalline TiO2 studied by optical, FTIR and X-ray photoelectron spectroscopy: correlation to presence

of surface states. _Thin Solid Films_ 358, 122–130 (2000). Article  ADS  CAS  Google Scholar  * Zhang, J.-Y. et al. Nanocrystalline TiO2 films studied by optical, XRD and FTIR spectroscopy.

_J. Non-Cryst. S_ 303, 134–138 (2002). Article  ADS  CAS  Google Scholar  * Kudin, K. N. et al. Raman Spectra of Graphite Oxide and Functionalized Graphene Sheets. _Nano Let_. 8, 36–41

(2008). Article  ADS  CAS  Google Scholar  * Maiaugree, W. et al. A dye sensitized solar cell using natural counter electrode and natural dye derived from mangosteen peel waste. _Sci Rep_.

5, 15230, (2015). Article  ADS  CAS  Google Scholar  * Voïtchovsky, K. et al. _In Situ_ Mapping of the Molecular Arrangement of Amphiphilic Dye Molecules at the TiO2 Surface of

Dye-Sensitized Solar Cells. _ACS Appl. Mater. Interfaces_ 7, 10834–10842 (2015). Article  Google Scholar  * Lim, S. P., Pandikumar, A., Lim, H. N., Ramaraj, R. & Huang, N. M. Boosting

Photovoltaic Performance of Dye-Sensitized Solar Cells Using Silver Nanoparticle-Decorated N, S-Co-Doped-TiO2 Photoanode. _Sci Rep_. 5, 11922 (2015). Article  ADS  Google Scholar  * Amadi,

L. et al. Creation of Natural Dye Sensitized Solar Cell by Using Nanostructured Titanium Oxide. _Nanosci. Nanoeng_. 3, 25–35 (2015). Article  CAS  Google Scholar  Download references

ACKNOWLEDGEMENTS This work was financially supported by the University of Maryland System (Wilson E. Elkins Professorship), Constellation, an Exelon Company (E2- Energy to Educate grant

program) and the United States Department of Education (USDE-SAFRA Title III Grant). The authors are also grateful to the Institution of Advancement, Coppin State University, for

administrative help. The content is exclusively the responsibility of the authors and does not necessarily represent the offical views of the funding agencies. AUTHOR INFORMATION AUTHORS AND

AFFILIATIONS * Department of Natural Sciences, Center for Nanotechnology, Coppin State University, 2500 W. North Ave, Baltimore, MD, USA William Ghann, Hyeonggon Kang, Tajbik Sheikh, Sunil

Yadav, Tulio Chavez-Gil, Fred Nesbitt & Jamal Uddin Authors * William Ghann View author publications You can also search for this author inPubMed Google Scholar * Hyeonggon Kang View

author publications You can also search for this author inPubMed Google Scholar * Tajbik Sheikh View author publications You can also search for this author inPubMed Google Scholar * Sunil

Yadav View author publications You can also search for this author inPubMed Google Scholar * Tulio Chavez-Gil View author publications You can also search for this author inPubMed Google

Scholar * Fred Nesbitt View author publications You can also search for this author inPubMed Google Scholar * Jamal Uddin View author publications You can also search for this author

inPubMed Google Scholar CONTRIBUTIONS J.U. conceived the idea and reviewed the final manuscript. W.G., T.S., H.K. designed the experiments. W.G., T.S. and S.Y. performed the experiments.

W.G. and H.K. wrote the manuscript with the assistance of J.U. T.C.h.-G. performed Raman and FT-IR experiments and analysis., F.N. performed HOMO-LUMO theoretical calculation-analysis. All

authors participated in the discussion and commented on the paper. CORRESPONDING AUTHOR Correspondence to Jamal Uddin. ETHICS DECLARATIONS COMPETING INTERESTS The authors declare no

competing financial interests. SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION (PDF 1794 KB) RIGHTS AND PERMISSIONS This work is licensed under a Creative Commons Attribution 4.0

International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the

material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit

http://creativecommons.org/licenses/by/4.0/ Reprints and permissions ABOUT THIS ARTICLE CITE THIS ARTICLE Ghann, W., Kang, H., Sheikh, T. _et al._ Fabrication, Optimization and

Characterization of Natural Dye Sensitized Solar Cell. _Sci Rep_ 7, 41470 (2017). https://doi.org/10.1038/srep41470 Download citation * Received: 27 June 2016 * Accepted: 20 December 2016 *

Published: 27 January 2017 * DOI: https://doi.org/10.1038/srep41470 SHARE THIS ARTICLE Anyone you share the following link with will be able to read this content: Get shareable link Sorry, a

shareable link is not currently available for this article. Copy to clipboard Provided by the Springer Nature SharedIt content-sharing initiative