One-pot synthesis of graphene- cobalt hydroxide composite nanosheets (Co/G NSs) for electrocatalytic water oxidation

We report a one-pot method for the preparation of graphene-cobalt hydroxide nanosheets (Co/G NSs) and their use as an effective elelctrocatalyst for water oxidation. Mechanical exfoliation of graphite via sonication produced graphene sheets, which were stabilized by the surface adsorption of a cationic surfactant (CTAB). In a subsequent step, varying amount of a cobalt complex [sodium hexanitrocobaltate(III)] was added which selectively bound with the positively charged head of surfactant. In the last step, cobalt complex was reduced with sodium borohydride to obtain Co/G NSs catalyst. The catalyst showed lower overpotential (280 mV) as compared to benchmark catalysts and decent stability and turnover frequency (TOF: 0.089 s−1) for oxygen evolution reaction (OER).


Results and Discussion
We used cationic surfactant, cetyltrimethyl ammonium bromide (CTAB), to produce graphene flakes in water by mechanical exfoliation of graphite via ultrasonication (Fig. 1) 65 . The surfactant gets adsorbed on the surface of so produced graphene via Van der Wall's interactions and stabilizes the 2-dimensional material (I in Fig. 1). In the following step, a cobalt complex (Na 3 [Co(NO 2 ) 6 ]: CoL) was added whose anion ([Co(NO 2 ) 6 ] 3-) electrostatically binds with the the positive head of the surfactant (II in Fig. 1). In third step, cobalt complex was reduced to produce Co/G NSs (III in Fig. 1). In past, stable graphene dispersions with an optimum yield have been achieved with a maximum surfactant concentration of 0.1 mg/ml 70 . Any higher concentration of surfactant leads to the agglomerations of graphene flakes due to the disruption of electric double layer by counter ions 71 .
UV-vis absorption spectrum of graphene dispersion was found featureless and flat (Fig. 2a) at and above 400 nm where absorption by surfactant molecules was negligible. Absorption at 660 nm could therefore be attributed to suspended graphene and was used to find the concentration using Beer-Lambert law (A = αCl) 71 . For the  calculation of extinction coefficient (α), a graphene dispersion (500 ml) was prepared using graphite (3 mg/mL) and CTAB (0.1 mg/mL). After centrifugation and decantation, absorption spectrum was taken at 660 nm. 60 mL of this dispersion was filtered through pre-weighted filter units, dried and weighed to find the graphene concentration. The value of absorptivity constant was found to be 1256 mL/mg/l which is close to the reported value of 1390 mL/mg/l 65 .
Next, various parameters for instance, sonication time, surfactant and graphite concentration were optimized to improve graphene yield. It was found that graphene yield increases almost linearly with sonication time as presented in Fig. 2b. The yield (8 μg/mL) obtained after ten hours of sonication was used as the optimum value for the rest of the experiments. In the same way concentration of graphite (C G ) and CTAB (C CTAB ) were also optimized and optimum yield of graphene was found with C G = 3 mg/mL and C CTAB = 0.1 mg/mL [see Fig. S1 in supporting information (SI)]. Under optimized conditions, 500 mL of graphene dispersion was centrifuged (@15000 rpm for 1 hour) followed by vacuum filtration to remove undissolved graphite. Afterwards graphene concentration in the dispersion was calculated using uv-visible spectrophotometry 65 .
Raman spectroscopy 66,72 was used to get further structural information about graphite, graphene and Co/G NSs materials. All the spectra as presented in Fig. 2c contain D (~1352 cm −1 ), G (~1587 cm −1 ) and 2D (~2710 cm −1 ) bands 65 . The D band corresponds to the breathing modes of sp 2 atoms in rings 73 while G band attributes to in-plane vibrational modes of sp 2 -bonded carbon atoms 74 . 2D band which is the second order of D band appeared at ~2710 cm −1 in all the spectra. Intensity ratio of G and 2D bands (I G /I 2D ) can be used to differentiate graphite from graphene and is probably the best way to decide layer-thickness 75 . I G /I 2D ratio in our case decreased from 1.42 in graphite to 1.2 in graphene and to 1.0 in Co/G NSs material. The latter corresponds roughly to a thickness of 5-layers 76 . Raman spectrum of Co/G NSs showed an additional intense band at ~520 cm −1 which was assigned to A 2u lattice mode of cobalt(II) hydroxide [77][78][79] .
Stability of graphene dispersions was tested by zeta potential analysis ( Fig. 2d) as these colloids were expected to be stabilized by electrostatic repulsion between the surfactant-coated graphene sheets. Hydrophobic tail of CTAB gets adsorbed on graphene sheets due to Van der Waal forces and impart positive charge due to the positively charged head of surfactant 80 . The formation of so-called electric double layer will avoid possible agglomeration of graphene sheets 81 . It is reported that colloidal particles will be electrostatically stabilized if the zeta potential values fall between −15 mV and 15 mV 82 . Our graphene dispersion showed a zeta potential value of 47 mV which indicated stability of the system 83 .
The morphology of Co/G NSs was analysed by TEM. Figure 3a presents an overview image of the Co/G NSs material showing a sheet-like morphology. At a higher resolution (Fig. 3b) folded nanosheets (NSs) with a thickness of ~3.8 nm (inset) were observed. A SEM image of the material is presented in Fig. 3c where again folded NSs can be clearly seen. EDX maps of the selected region suggest the presence of Co, O and C with an atomic ratio of 52, 25 and 9 atomic percent. Therefore we conclude that NSs are made up of either oxides or hydroxides of Co. EDX spectrum of another region is presented in S2 (SI) provides further confirmation about the chemical nature of NSs.
Co/G NSs material was further confirmed by X-ray photoelectron spectroscopy (XPS). In survey spectrum of the material presented in Fig. 4a, peaks at 284.0, 531.0 and 779 eV were indexed to C(1s), O(1s) and Co(2p) respectively. Magnified view of C(1s) spectrum is provided in Fig. 4b where a main peak at 284.0 was assigned to sp 2 carbon and a small peak at higher binding energy (286.0 eV) to O-C-O and C-OH groups 84 . The oxygen (1 s) core spectrum (Fig. 4c) was deconvoluted into two peaks at 530.2 and 530.6 eV and were assigned to O(1 s) in cobalt hydroxide Ca(OH) 2 85 .
High resolution XPS spectrum of Co 2p (Fig. 4d) showed a spin-orbit splitting into 2p 3/2 and 2p 1/2 with an energy difference of ~16 eV typically known for cobalt(II) hydroxide 86,87 . 2p 3/2 peak was deconvoluted into two peaks centering at 782.6 and 787.6 eV and were assigned to Co(OH) 2 , the latter being the shake-up satellite of 2p 3/2 88 . The peak at higher binding energy was broken down into two Gaussian peaks at 798.6 and 804.5 eV and were attributed to 2p 1/2 and its shake-up satellite for cobalt hydroxide respectively. Although Co 2p 3/2 peak of Co 3 O 4 also occurs in the same region (~779 eV), its presence in the sample was ruled out because of the fact that Co 3 O 4 does not show any satellite peak 89 . Co/G NSs composite for oxygen evolution reaction (OER) was tested in 0.1 M KOH using a three-electrode system details of which are given in experimental part. Linear sweep voltammetry (LSV) of the material revealed an efficient OER catalytic activity (onset 1.51 V) with a low over potential of 280 mV to achieve 10 mA/cm 2 current density (Fig. 5a). This OER activity (280 mV) of Co/G NSs is even better than the benchmark IrO 2 catalyst (297 mV) under the same experimental conditions 90 and other cobalt-based catalysts reported to date (see Table S1).
For electrocatalytic performance, Tafel slope can be used for the kinetics study to determine the rate and rate determining step during OER reaction. We calculated a value of 79.2 mV/dec for Co/G NSs material (see Fig. 5b) which is though high as compared to other first-row transition metals, nevertheless provides valuable information about the kinetic parameters. Value of Tafel slope suggests that the formation of MO (where M denotes a free metal site) from the adsorbed OH − ions is the rate determining step 91 . The mass activity (583.3Ag −1 ) and TOF (0.089 s −1 ) of Co/G NSs catalyst were also found to be high (Table S2) at low mass loading (17 µg/cm 2 ).
Stability of the catalysts was evaluated by controlled current electrolysis (CCE) experiment performed in 0.1 M KOH (pH = 13). Chronoamperometry was conducted at 1.65 V (vs RHE) while maintaining current density of 5.65 mA/cm 2 for 3600 sec under steady state condition. From the stability plot (Fig. 5c), the tolerance of this electrocatalyst against intermediate species may be attributed the strong interaction of Co with graphene. Fig. S3 displays a plot under constant current density of 10 mA/cm 2 between applied potential (E/V vs RHE) and time (t) and it shows that this catalyst is stable up to 1100 sec vs applied current density.
Electrochemical impedance spectroscopy (EIS) measurement was also carried out to investigate OER activity of Co/G NSs. Figure 5d shows the Nyquist plot at applied potential of 1.51 V (vs RHE) in the frequency range of 1 Hz to 100 kHz to determine the conductivity and resistivity of the catalysts. The semicircular portion of the plot provided solution resistance (Rs), charge transfer resistance (R ct ), and double layer capacitance (C dl ). R ct value (408.7Ω) was rather high for our catalyst system and could be attributed to the presence of surfactant. Solution resistance (R s ) was calculated to be 72.8Ω (Table S3).
Using C dl value we calculated electrochemically active surface area of Co/G NSs to be 27 cm 2 which can be correlated to the presence of more active sites at electrolyte/analyte interface, and hence higher electrocatalytic activity 92 of our electrocatalyst as compared to other electrocatalysts (Table S2). There can be error in the reported value of specific capacitance of metal electrodes as large as 7% in acidic and basic media 11 .
The above results revealed an accessible and simple way to obtain stable dispersions of graphene in surfactant (CTAB)/water systems followed by the generation of Co(OH) 2 NSs to fabricate a Co/G nanocomposite. The dispersion and concentration of graphene increased linearly with CTAB concentration and sonication time. Presence of graphene increased the electrical conductivity of Co(OH) 2 and hence OER activity of the composite material. Current density of 63 mA/cm 2 was achieved at low overpotential (280 mV) in basic medium. Electrocatalytic activity of Co/G NSs was found better as compared to the state-of-the-art catalysts based on the oxides of Ir and Ru. Overpotential value, ECSA, mass activity and TOF of the catalyst was also found superior than other cobalt-based catalysts reported so far.

Methods
Graphite obtained from used zinc-carbon batteries was soaked and washed with hydrochloric acid to leach metal impurities. Cetyl trimethylammonium bromide (CTAB), Sodium borohydride (NaBH 4 ), Sodium hexanitrocobaltate(III) (Na 3 [Co(NO 2 ) 6 ] was purchased from Sigma Aldrich. All the solutions were prepared in deionized water (DI) and methanol.
Uv-visible spectra were obtained on UV-1800 SHIMADZU Spectrophotometer while zeta potential was measured on Malvern ZETA SIZER NANO. Energy dispersive X-ray spectroscopy (EDX) and surface morphology were examined by using FEI NOVA nano SEM 450 equipped with Oxford EDX detector. Raman spectra were taken using Raman Microscope Renishaw, UK. Surface analysis of the catalysts was conducted using X-ray photoelectron spectrometer (ESCALAB 250Xi, Thermo Scientific, UK). Charging of the spectra was corrected against the graphitic-like C 1 s peak (from the instrument itself) taken at 284 eV and used as a reference. CASAXPS software (version 2.3.16) was used for peak fitting.
Transmission electron microscopy (TEM) was carried out by using a Varian LEO 9220 (200 kV) and a JOEL JEM-2200FS instrument. The sample was suspended in chloroform and sonicated for 5 min. Subsequently a drop of the suspended sample was placed on a grid (Plano S 166-3) and allowed to dry.
Electrochemical analysis was executed by using Gamray Reference 600 Potentiostat/galavanostat/ZRA with three-electrode system. Catalyst synthesis. Graphene was prepared by a simple mechanical exfoliation method. Typically, graphite and CTAB were mixed in 3.3:1 mass ratio in DI water and the mixture was sonicated for 10 hr in ultrasonic bath (Elma X-tra 70 H) whose temperature was kept below 50 °C. CTAB-stabilized graphene suspension was centrifuged (Centrifuge -5810R) for one hour to remove undissolved graphite and unstable graphene. In the next step, Cobalt complex was added to graphene dispersion (Co to graphene mass ratio = 1:100) and sonicated for 30 min. Afterwards, freshly prepared solution of NaBH 4 was added and dispersion was stirred at room temperature for 2 hours.
For characterization, graphene dispersion was filtered through syringe filter (0.22 μm) and vacuum dried. For TEM and Raman analysis, dispersions were precipitated at 14000 rpm for 30 minutes. Electrochemical measurements. All the electrochemical experiments were performed at room temperature (25 °C) using standard three-electrode system. A glassy carbon (0.07 cm 2 ) electrode (GCE) was scrubbed with alumina powder (0.05 µm) before using as the working electrode. A silver/ silver chloride electrode (Ag/ AgCl) was used as reference electrode and platinum wire as counter electrode. All the potentials were converted into RHE by using following Nernst equation.
(RHE) ( Ag/AgCl) 5 µL of prepared catalyst without any binder, was deposited on GCE and air dried at room temperature. Then all OER tests were achieved in the 0.1 M KOH at the scan rate of 20 mV/sec with a scan limit of 0 to 1 V. For the evaluation of electrocatalytic activity, all the calculation were made from the iR corrected voltammogram (Fig. 5) Tafel slope was calculated by overpotential (η) and current density (j) by using Tafel equation.
where 'b' is the Tafel slope and 'a' is the constant.
Theoretically, mass activity was calculated by using the following equation. where 'j' is the current density (mA/cm 2 ) and 'm' is the loading mass of electrocatalyst (0.017 mg/cm 2 ). The turnover frequency (TOF) can also be theoretically calculated by considering that every metal atom is involved in catalysis. Electrochemically surface area (ECSA) for each system can be measured from double layer charging capacitance of electrocatalytic surface determined from non-faradic region of cyclic voltammetry at multiple scan rates from 10 mV/sec to 200 mV/sec of cyclic voltamogram [93][94][95][96] .
It is assumed that non-faradic current is due to double layer charging capacitance (Figs S4 and S5). A plot of scan rate and current was used for calculating double layer charging capacitance (C dl ) which yield a straight line equation with a slope which is equal to C dl according to following equation 97 (Fig. S6). = where i c is the double layer charging current, v is the scan rate and C dl is the double layer charging capacitance.
The value of C dl for electrodeposited Co/G NSs catalyst is 1.17 mF obtained from CV of different scan rates ( Fig S3). Then, ECSA can be calculated from following relationship. Here C s is the specific capacitance due to double layer of smooth surface of deposited sample on electrode. Values of C s for different metal electrodes have been reported in literature for acidic and alkaline solutions lies in the range of 0.022−0.130 mF cm −2 for KOH and NaOH. The reported value of specific capacitance for cobalt surface is 0.043 mF cm −2 in 0.1 M KOH and consider it as a 'typical' value for such materials. The calculated electrochemically active surface area of Co/G NSs is 16 cm 2 according to our calculations by using C dl value.