rGO Sheets / ZnFe 2 O 4 Nanocomposities as an E � cient Electro Catalyst Material for I 3-/ I-Reaction for High Performance DSSCs

Anto feradrick Samson V (  antofradrick@gmail.com ) Department of Physics, Loyola College https://orcid.org/0000-0002-5124-9645 Bharathi Bernadsha S Department of Physics, Loyola College Albin John P Paul Winston Department of Physics, Loyola College Divya D Department of Physics, Loyola College James Abraham Department of Physics, Loyola College Victor Antony Raj M Department of Physics, Loyola College Madhavan J Department of Physics, Loyola College


Introduction
In recent years, fossil fuels becoming increasingly scarce and global warming gained momentum from rising carbon dioxide emission that imply the need to go for alternates which can replace the fossil fuel and mitigate the pace of global warming. Natural resources such as solar energy, wind energy, hydroelectric energy, geothermal and thermal energy can be harnessed as alternate energy reserves [1,2].
The incident radiation or light energy of the sun is converted to electrical energy or electricity. The Photo Voltaic systems are employed for this conversion process. Dye Sensitized Solar Cells (DSSC) are identi ed as signi cant options due to low manufacturing cost, environmental friendly, non-pollution and high energy conversion under low light conditions [3,4]. The major components of DSSC are photo anode, dye, electrolyte and catalytic Counter Electrode (CE). CE is an indispensable key component in the working of a DSSC to improve conversion e ciency, act as a catalyst for the tri-iodide reduction and also collects the electron from the external circuit and injecting it to the electrolyte. Traditionally Platinum (Pt) is widely used as standard CE material for the DSSC due to its good conductivity, catalytic capacity, low charge transfer resistance and higher activity in visible and infrared regions. However Pt it's costlier, possesses highly corrosive nature in the liquid electrolyte which may lead to serious drawbacks in the large scale production [5]. Therefore, developing materials which reduce the use of Pt in DSSC is the need of the hour. So far, other alternative materials like carbon allotropes (activated carbon, CNTs and graphene), conducting polymers (CP) and transition metals have also been introduced to substitute Pt CEs. However the conversion e ciency of those electrodes is still low compared to Pt as a result of low electron conductivity and poor catalytic activity. Recently, it's reported that graphene-based nanocomposites designed to own high chemical stability, signi cant electro catalytic activity towards iodine triiodide electrolyte, large surface area and more activated electrochemical functionalized sites.
Also, there are reports on spinel type rGO based hybrid materials (MFe 2 O 4 and MCo 2 O 4 (M=Ni, Co, Zn, Mg)) examined as a CE material for DSSCs owing to their chemical properties, low cost, high stability against corrosion, interactions between metal ions via chemical bonds and multi metal composition provide more active sites improving the electrochemical activity [6,7].In this case, a novel spinel type (MFe 2 O 4 ) nanocomposites consisting of reduced graphene oxide (rGO) are suitable with excellent electro catalytic activity [8,9]. Moreover, graphene possesses π-π conjugation structure, which endowed them with excellent electrical property and superior chemical stability in electrochemical environment. properties. In this favor, we have prepared rGO/ZnFe 2 O 4 nanocomposites by facile one-pot hydrothermal method with a different weight ratio of GO sheets. The in uence of structural and electrochemical performances of the nanocomposites is investigated. Finally, Dye Synthesized Solar Cells are made employing as synthesized CEs and the results are compared to that of the cells fabricated with Pt CE.

synthesis of rZnF nanocomposites
The Preparation of graphene and reduced graphene oxide (rGO) procedure were followed as reported by Then 5M of NaOH solution added until the pH value exceeds above 10. The above solution mixture was slowly added to as previously prepare GO suspension. Then the solution was taken in autoclave and heated at 180°C for 12 Hrs. After that the precipitate was collected by centrifuge several times and dried at 80°C for 12 Hrs. The obtained sample named as rZnF-25. For rZnF-50 prepare by adapting the same procedure additionally double amount of adding GO. For comparison pure ZnFe 2 O 4 (ZnF) also prepared by without adding GO.

Fabrication of DSSCs
The CEs paste is prepared by 100mg as prepared sample was ground well in mortar, then adding (N, Ndimethyformamidel solution) NMP and PVDF to form a slurry sticky paste, Then the slurry was coated in FTO subtract by using doctor blade method with a contact area of 1.5 cm 2 and sintered 500°C for 30 minutes. The Pt CE was prepared by drop coating method using H 2 PtCl 6 solution with a contact area of 1.5 cm 2 and sintered 500°C for 30 minutes. After natural cooling to room temperature all prepared CE was ready for both electrochemical and photovoltaic studies. simultaneously, the same procedure followed by the preparation of photo anode using commercially available TiO 2 paste. Then the prepared photo anode

X-Ray Diffraction
XRD pattern of GO, rGO, ZnF, rZnF-25and rZnF-50 are Shown in Fig.1 (a,b). Graphene oxide characteristic peak at 9.8° following to the plane (001) indicates the successful preparation of graphene oxide from graphite power. For rGO, small broad peak observed at 24.4°corresponds to (002) plane has con rmed the conversion of rGO from GO. The peaks at 29.78°(220), 35.15°(311), 37.90°(222), 42.73°(400) 53.28°(422), 56.71°(511) and 62.36°(440) con rm the formation of high crystallinity cubic spinel structure of ZnF, which were very well synchronized with the JCPDS (card No.01-077-0011).For nanocomposites, there is no disordered graphene oxide peaks were seen, which is due to the considerable amount of adding graphene in the composites and also the diffraction of disordered graphene planes is weak as compare to ne crystalline ZnF planes [14]. This con rms the graphene oxide is successfully dispersed on the surface of ZnF nanoparticles and does not make any structural changes in the planes. The average particle size is calculated using Scherer's equations and the value is found to be 26.1, 17.8 and 15.3 nm for ZnF, rZnF-25 and rZnF-50 respectively. Also In this study, addition of graphene plays a key factor for adjusting the size of the particles. Lattice parameter of cubic crystal lattice (a=b=c) was calculated using the formula, the obtained lattice parameter is listed in Table 1.
a= d (h 2 +k 2 +l 2 ) Å…………… (1)  Fig 2 (a&b) shows the HR-TEM images of rGO and rZNF-50 samples respectively. The sheetlike rGO sheets are found to exhibit wrinkled morphology with high transparency representing single layer graphene. In Fig 2(b) it can be seen that the amorphous rGO sheets were smoothly distributed on the surface of ZnF nanostructure, which is expected to provide low charge transfer resistance and e cient channel path for conductivity of the material [13]. Fig. 2(c) shows the SAED pattern of rGO, which con rms the amorphous nature of the graphene sheets. In respectively. From HR-TEM analysis, the particle size is found to be 29.7, 20.2 and 18.8 nm for ZnF, rZnF-25 and rZnF-50 respectively. The decreasing in particle size bene tted the quick spread of electrolyte and fast charge transport. The obtained particle size from TEM results are in good agreement with XRD results.

FT-Raman
FT-Raman spectra of graphene oxide, rZnF-25 and rZnF-50 nanocomposites are shown in Fig 3. Generally, Ferrite cubic spinel structure which gives rise to 39 normal Raman modes in which 2A 1g , 1E g , 3F 2g are Raman active modes. The Raman spectra of rZnF-25 and rZnF-50 samples revels four Raman active modes. The band at 648, 371, 297 and 198 cm -1 were belonging to the vibration modes of A 1g , F 2g , E g and T 2g respectively. The vibration mode A 1g and F 2g represent Fe-O and M-O stretching at the tetrahedral sites, additionally E g and T 2g modes present corresponds to the asymmetric stretching of oxygen atoms with respect to the metal ion at the octahedral site respectively [15]. The corresponding graphene oxide peaks such as 1340 cm -1 and 1590 cm -1 were represents D-Band, breathing point of Phonon A 1g symmetry and G-band, E 2g Phonon of Sp 2 C-atoms respectively. Generally, the value of the intensity ratio of the D band to the G band (I D /I G ) is used to estimate the degree of disorder and the defects of carbon material. The obtained ratio is 0.98, 1.17 and 1.26 for rGO, rZnF-25 and rZnF-50 respectively. I D /I G values were higher than that rGO con rms a low graphitic degree, more defects or edges, and disordered structures were introduced in rZnF-25 and rZnF-50 samples which could be bene cial for triiodide reduction process [8].

Electrochemical Measurements
Cyclic Voltametry (CV) To evaluate the ion diffusivity and electro catalytic activity towards I 3 reduction were examined by CV measurements and (oxi/red) peaks of CE shown in Fig 3a. The pair of negative and positive peaks was observed in all the samples were determined the following redox reactions.
The highest cathodic reduction peak current density (J red ) and the smallest peak to peak (E pp ) separation . Where (R s ) is series resistance (R ct ) is charge transfer resistance (Z w ) is resistance of nernst diffusion [17]. Obtained values in the following sequence rZnF-50> Pt >rZnF-25>ZnF>rGO. rZnF-50 exhibits lower R s and R ct values than other electrodes due to addition of graphene sheets evenly covers ZnF nanoparticles which offer more channels for electron transfer and also improve electrode electrolyte interface area, as well as their bonding in the subtract bene ts fast charge transfer improves electrochemical activity.

Tafel Polarization
To further con rm the electrocatalytic activity abilities of different CEs, Tafel polarization measurements were performed on same potential window as performed in CV measurements (Fig 4d.). In the tafel studies exchange current density J o and limiting current density J lim were obtained from anodic and cathodic slopes which are directly related electro catalytic activity of CEs. J o and J lim are obtained from the following Equations: A Tafel polarization result con rms that rZnF-50 exhibit higher J o values than other electrodes and displays superior electrocatalytic performance of the CE material [10].This is mainly credited to adding graphene structure into ZnF which gives large number of tiny holes and pores for I 3 -/ Ielectrolyte to linkup inside the CE area and accelerates the reduction reaction.  Table 2. The photocurrent density (J) vs voltage (V) curves of DSSCs based on as prepared different CEs shown in Fig 5. The obtained photovoltaic parameters are summarized in table 3. Generally, High electrocatalytic ability of the CE material leads to fast reduction of I -3 and generation of Iions, which enables to achieve highest short current (Jsc) and photo conversion e ciency (PCE). The DSSC fabricated with rZnF-50 CE exhibits higher J sc of (17.98mA/cm 2 ), FF of 0.62 value and power conversion e ciency PCE of (8.71%) than the PCE of platinum (Pt) (8.53%) CE. The increase in J sc and FF is achieved by the intrinsic conductivity created by grafting graphene sheets on rZnF-50 CE which results enhanced electrochemical active sites for triiodide reduction I -3 and generation Ireactions. It also reduces the diffusion resistance between CE and electrolyte and smooth surface accelerates fast electron transmission pathways. At the same time ZnF and rGO exhibit lower value of Jsc and conversion e ciency mainly due to rough surface and low conductivity and electrochemical stability of the CEs.    FT-Raman spectra of rGO, rZnF-25 and rZnF-50nanocomposities  The photocurrent density (J) vs voltage (V) curves of GO, rGO, ZnF, rZnF-25 and rZnF-50 CEs