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Template free-synthesis of cobalt–iron chalcogenides [Co0.8Fe0.2L2, L = S, Se] and their robust bifunctional electrocatalysis for the water splitting reaction and Cr(VI) reduction

Manzoor Ahmad Pandita, Dasari Sai Hemanth Kumara, Manigandan Ramadossab, Yuanfu Chenb and Krishnamurthi Muralidharan*a
aSchool of Chemistry, University of Hyderabad, Hyderabad, India. E-mail: murali@uohyd.ac.in
bSchool of Electronic Science and Engineering, University of Electronic Science and Technology of China, Chengdu 610054, PR China

Received 21st January 2022 , Accepted 22nd January 2022

First published on 9th March 2022


Abstract

The ease of production of materials and showing multiple applications are appealing in this modern era of advanced technology. This paper reports the synthesis of a pair of novel cobalt–iron chalcogenides [Co0.8Fe0.2S2 and Co0.8Fe0.2Se2] with enhanced electro catalytic activities. These ternary metal chalcogenides were synthesized by a one-step template-free approach via a hexamethyldisilazane (HMDS)-assisted synthetic method. Transient photocurrent (TPC) studies and electrochemical impedance spectra (EIS) of these materials showed free electron mobility. Their bifunctional activities were verified in both the electrochemical oxygen evolution reaction (OER) and in the electrochemical reduction of toxic inorganic heavy metal ions [Cr(VI)] in polluted water. The materials showed robust catalytic ability in the oxygen evolution reaction with minimum possible over potential (345 and 350 mV @ η10) as determined by linear sweep voltammetry and the lower Tafel values (52.4 and 84.5 mV dec−1) for Co0.8Fe0.2Se2 and Co0.8Fe0.2S2 respectively. Surprisingly, both the materials also showed an excellent activity towards electrochemical Cr(VI) reduction to Cr(III). Besides the maximum current achieved for Co0.8Fe0.2S2, a minimum value for the Limit of detection (LOD) was obtained for Co0.8Fe0.2S2 (0.159 μg L−1) compared to Co0.8Fe0.2Se2 (0.196 μg L−1). We tested the durability of catalysts, the critical factor for the prolonged use of catalysts, through the recyclability measurements of these materials as catalysts. Both the catalysts presented outstanding durability and balanced electro catalytic activities for up to 1500 CV cycles, and chronoamperometry studies also confirmed exceptional stability. The enhanced catalytic activities of these materials are ascribed to the free electron movement, evidenced by the increased TPC measured and EIS. Therefore, the template-free synthesis of these electro catalysts containing non-noble metal illustrates the practical approach to develop such types of catalysts for multiple functions.


1. Introduction

Energy conversion through photo- or electro catalytic water splitting is a promising method to supplement depleting energy sources. In this water splitting, the half-reactions involved are hydrogen evolution (HER) and oxygen evolution (OER) reactions. The catalysts based on noble metals like Pt, RuO2, or IrO2 perform well in electrocatalytic water splitting.1,2 However, the high cost and low abundance in Earth's crust prevents their large-scale utility.3,4 Over the years, scientists have been engrossed in developing an efficient catalyst for the OER from water as it is the most favourable for green and cheap energy production.5–8 Therefore, the focus is on readily available transition metals, which are cheap and less toxic, and their efficiency should match that of Pt or other noble metal catalysts.9–11 Various transition metal compounds are active for electro catalytic OER performance.12–17 The materials such as alloys, phosphides, carbides, selenides, borates, nitrides, carbon-based materials, and hydroxides are also used effectively as the OER catalysts.18–25

There are continuous investigations on the use of active transition elements like Ni, Co, Fe, Cu, and Mo and their combinations with sulphur as electro catalysts. Some varieties include Co–Ni–S,26–29 Cu–Co–S, and Cu–Mo–S,30–32 Co–Fe–S,33–37 Co–Mo–S,38 and Zn–Co–S.39 The ternary chalcogenides have shown superior properties like high electrical conductance than monometallic due to the low activation energy for electron transfer between cations.3 Apart from the stoichiometric combinations, distinct features such as the crystalline phase, morphology, and particle size influence the electro catalytic activity of transition metal sulfides.16,17,40–42 Shen et al. reported a composite formation between cobalt–iron sulphide and nitrogen-doped mesoporous graphitic carbon (Co0.5Fe0.5S@N-MC) employing a simple soft template scheme. The covalently bonded nanostructures on a mesoporous graphitic layer in this material played the catalytic role in water oxidation reactions.43 Consecutively, the transition metal chalcogenides have emerged as elegant OER electro catalysts.

Metal selenides are better than sulphides in many aspects as they possess more metallic character than sulphides and outstanding electrochemical properties.44–47 Many transition metal selenides of the type MSe2 (here M = Fe, Co, Mo, Ni, Cu, and Mn) were used as an electrode in energy conversion or storage devices such as solar cells, battery, super capacitor, fuel cells, sensors, and in water-splitting reactions (HER and OER).48–53 Xiao et al. succeeded in depositing lamellar structured nanosheets of CoSe2 on the Ti plate (CoSe2NS@Ti) by an in situ method, and they used it directly as a cathode for superior hydrogen evolution activity.54 An active strategy of attaining advanced properties in the nanoscale regime is doping CoSe2 crystal structure with another element with the same electronic configuration and atomic radius. This phenomenon will supplement defects/vacancies on an atomic scale by regulating the electrocatalytic active sites. Ramadoss et al. reported porous nanoarchitecture constructed by ultrathin CoSe2 embedded Fe–CoO nanosheets acted as an excellent electrocatalyst material for water oxidation.55 Zhao et al. reported synthesizing ultra-small FeSe2 nanoparticles by a high-temperature solution-based method that acted as an excellent material for sodium-ion storage.56 Sakthivel et al. claimed hydrothermal synthesis of CoFeSe2/f-CNF and its use to detect caffeic acid electrochemically.57 Yiqing et al. reported sulfidation and selenation of cobalt–iron by the hydrothermal method as the precursors to produce the Prussian-blue-analog (PBA) nanocubes and used them as excellent electrodes for dye-sensitized solar cells.58

On the other side, the continuous elimination of toxic and harmful chemicals from industrial effluents is detrimental to the environment. Many poisonous and carcinogenic chemicals released into the atmosphere significantly affect both aquatic as well as terrestrial life. The water bodies contaminated with such carcinogenic and toxic chemicals, including organic dyes [e.g., rhodamine B, methylene blue dyes, nitro compounds]59–62 and toxic inorganic chemicals [e.g., Cr(VI)]63 are unfit for drinking and other purposes. Therefore, the challenge is to develop such catalysts that are easily accessible, cheap, and their precursors must be abundant. Thus, the need is to develop highly efficient and stable catalysts to perform multirole in water splitting and detoxify toxic organic/inorganic chemicals.

Since electro catalysis depends on the unrestricted mobility of electrons, the environment around the nanocatalyst should promote electron movement rather than behaving as an insulator.64 Moreover, chemical reactions occur on the catalyst's surface. To use metal chalcogenides as catalysts in any reaction, their active centres at the surface should be free from any hindrance and exposed to the interaction with the substrate. Although many reports documented sulphides and selenides as catalysts, the effect of clean surfactant-free surfaces on ternary chalcogenide systems without insulating effect and their bifunctional role in catalysis is not being probed. Besides the template free approach, the morphology and size of the catalyst are also the deciding parameters for superior catalysis. Primarily, morphological nanostructures having open access to their active sites are remarkably the most suitable bifunctional catalysts for sensors, OER and reduction of toxic chemicals.65 Thus, a facile technique to develop and produce bifunctional ternary metal chalcogenides is highly imperative.

Inspired by the literature mentioned above and the results obtained herein, we report a study on transition metal chalcogenides (Co0.8Fe0.2S2 and Co0.8Fe0.2Se2) as bifunctional electro catalysts. The materials had no residual organic moieties resulting from the synthetic process. The materials were produced via hexamethyldisilazane (HMDS) – assisted self-template synthesis and characterized using various analytical and spectroscopic techniques.66,67 The outstanding catalytic activities of the materials (Co0.8Fe0.2S2 and Co0.8Fe0.2Se2) were delineated from the electrochemical oxygen evolution reaction (OER). Besides the above catalytic pathways, electrochemical Cr(VI) reduction using Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials is ample proof of their dual catalytic behaviour. There are no reports yet published about such types of bifunctional catalytic activities involving this material. Therefore, the present work establishes an attractive approach in developing non-noble metal and template free catalysts with multiple roles.

2. Experimental section

2.1. Materials

Cobalt chloride (CoCl2 anhydrous), ferric chloride (FeCl3 anhydrous), thiourea [H2NC(S)NH2], selenium powder, hexamethyldisilazane [(Me3Si)2NH] (HMDS), K2Cr2O7, ethanol and Nafion were purchased from Sigma Aldrich. Distilled water was used for both the electrocatalytic pathways. The above-enlisted chemicals were of analytical grade and used as such.

2.2. Instrumentation

The synthesized materials were subjected to various analytical techniques for their characterization. The crystal structure and phase purity were confirmed using PXRD patterns obtained from Bruker D8 (CuKα, λ = 1.54056 Å, 2θ = 20° to 70°) spectrometer. The morphology and elemental distribution of synthesized materials were performed by FESEM (Ultra 55 Carl Zeiss microscopy with operating voltage = 10 kV), TEM (FEI Technai G2 F20 STEM with a 200 kV) and EDAS studies. Optical properties were performed using the JASCO-V770 UV/Vis spectrophotometer. The nitrogen adsorption–desorption isotherms and the pore distribution of materials were estimated by the Brunauer–Emmett–Teller instrument (BET) (Nova 2000e, Quantachrome Instruments Limited, USA using liquid nitrogen (77 K)). The oxidation states of elements and the chemical composition were determined by X-ray photoelectron spectroscopy (XPS) (Thermo scientific Escalab 250Xi spectrometer with Al-Kα radiation). Electrochemical studies were carried using Ametek PARSTAT electrochemical workstation in a conventional three-electrode system. Transient-photocurrent (TPS) studies and electrochemical impedance spectra (EIS) were performed by Zahner-Zennium electrochemical work station using a three-electrode system.

2.3. Synthesis of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 chalcogenides

The wet chemical synthesis of Co0.8Fe0.2S2 nanoparticles was achieved by hexamethyldisilazane (HMDS) – assisted method with slight modification. In a typical reaction, 1.54 mmol of CoCl2 and 0.31 mmol of FeCl3 were added one by one into a two-neck RB connected to Schlenk lines and purged with N2 gas. Then HMDS (6 mL) was injected using a syringe under the continuous nitrogen gas supply to maintain the inert condition. The reaction mixture was stirred for 30 minutes to dissolve precursor salts in the medium at 40 °C; after 30 minutes, 3.08 mmol of thiourea was added. The reaction was set to reflux at 160 °C for 3 hours with continuous stirring. After completing the reaction, the precipitate was separated by centrifugation (set) at 2500 rpm, washed by deionized water and ethanol every 3–4 times to get the desired product. The material collected was subjected to a high vacuum at 70 °C overnight to remove any residual solvents. A similar procedure was applied to the synthesis of Co0.8Fe0.2Se2. The same precursors of cobalt and iron were used while thiourea was exchanged for selenium powder (3.08 mmol) to produce ternary metal selenide.

2.4. Transient photocurrent (TPC) and electrochemical impedance spectra (EIS)

The three-electrode system used for TPC and EIS consists of an FTO plate loaded with the synthesized materials as a working electrode, Pt as a counter electrode, and Ag/AgCl electrode as a reference. The working electrode was prepared by mixing 5 mg of synthesized materials (Co0.8Fe0.2S2 or Co0.8Fe0.2Se2) and 40 μl of Nafion (binder) in an 8[thin space (1/6-em)]:[thin space (1/6-em)]2 ratio water:ethanol solution. This mixture was sonicated to form a homogenous mixture and then drop-cast on an FTO glass plate to form a square-like thin film. The other portion of FTO was covered with Teflon tape and allowed to dry in an oven at 60 °C until the solvent was evaporated. The sodium sulphate solution 0.1 M was used as an electrolyte. For transient photocurrent studies, the plot of photocurrent against time during light on/off cycles with the time interval of 20 s was recorded. A similar FTO loaded glass plate was used for carrying EIS studies. The EIS measurements were taken in a frequency range of 100 mHz to 100 kHz at open circuit potential with the amplitude of sinusoidal voltage equal to 10 mV.

2.5. Preparation of electro catalyst as working electrodes for OER and electrochemical measurements

Electrochemical OER performances were monitored using the electrochemical workstation (CHI 660D) at room temperature (298 K). A home-made setup with a three-electrode system was used consisting of a glassy carbon (Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 modified and bare-GCE) as working electrode, Pt ring as the counter electrode, and a silver electrode as a reference electrode in 1 M KOH. Electro catalyst on GCE was loaded (∼0.3 mg cm−2) with Nafion binder via the drop-cast method with the micropipette assistance and then dried at the oven. All the electrochemical measurements were repeated many times to ensure consistency and reproductive performance. For the electrochemical performance evaluation, potentials of linear sweep voltammetry (LSV) and cyclic voltammogram (CV) were calibrated vs. reversible electrode (RHE as follows, ERHE = Eobt + EAg/AgCl + 0.059 × pH V). LSV measurements (0.005 V s−1, 1 to 1.8 V potential windows) were done to calculate onset over potential at current densities (j10, 10 mA cm−2) and Tafel plots (log(j) vs. VRHE). Double-layer capacitance (Cdl) measurements were done using CV measurements between the Vdl windows 1.203 V to 1.302 V.

2.6. Electrochemical Cr(VI) reduction

Electrochemical reduction of Cr(VI) was carried using a conventional three-electrode system. Glassy carbon electrode (GCE), Ag/AgCl (3 M KCl), and Pt were used as working, reference and counter electrodes respectively. The potentials used in the experiments were from −0.2 V to 1 V. The electrochemical Cr(VI) reduction was initially performed with different acidic media solutions to check which one will produce maximum current. The electrolyte, which gives the highest current, was used for further experiments. Apart from this, different concentrations of Cr(VI) (0.01 μM to 50 μM) were also prepared for the other experiments. The limit of detection was calculated from the calibrated plot by using the formula shown in eqn (1) below.
 
Limit of detection (LOD) = 3 × (s/m) (1)
where s is the standard deviation of the calibrated plot and m is the slope of the regression equation.

3. Results and discussion

3.1. Synthesis and characterization

The hexamethyldisilazane (HMDS)-assisted synthesis has emerged as a robust method to produce binary metal chalcogenide nanoparticles without surfactant molecules.66 In this work, the ternary materials, Co0.8Fe0.2S2 and Co0.8Fe0.2Se2, were synthesized utilizing the HMDS-assisted method with some modifications (Scheme 1). In this reaction, FeCl3 and CoCl2 were used as metal sources and thiourea or selenium powder as chalcogens to produce the desired sulphide and selenide materials. In both the reactions, HMDS acted as the solvent, reducing agent and surfactant molecule.67 The entire process was accomplished using the Schlenk line through which nitrogen gas was purged continuously to maintain the inert atmosphere.
image file: d2ra00447j-s1.tif
Scheme 1 Illustration of the reaction scheme carried for the synthesis of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 desired materials.

The crystal structure determination, together with phase purity, begins with powder X-ray difraction studies. Fig. 1 shows the well-established crystal structural information of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 chalcogenide materials. As shown in Fig. 1a, all the peaks correspond to the hexagonal structure of Co0.8Fe0.2S2 (JCPDS. No. 75-0607). The peaks at 2θ of 30.80°, 33.21°, 35.38°, 46.72°, and 54.64° can be indexed to planes of (100), (022), (101), (102) and (110) respectively. Likewise, Fig. 1b representing the diffraction spectra of Co0.8Fe0.2Se2 has various intense peaks at 2θ values of 23.4°, 29.67°, 35.77°, 41.28°, 43.72°, 45.25° and 52.3° designated to crystal planes of (110), (011), (111), (210), (102), (221) and (311) respectively.57 Besides this, the high-intensity peaks show the high crystalline nature of Co0.8Fe0.2Se2. No other characteristic peaks are indexable to either pure CoS2, CoSe2, FeS2 phases or any other stoichiometry of this trio in the PXRD spectra. Thus, confirming the single-phase and high purity of the material.


image file: d2ra00447j-f1.tif
Fig. 1 PXRD of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials.

The X-ray photoelectron (XPS) spectrum (Fig. 2) of Co0.8Fe0.2Se2 revealed its chemical composition and the valence oxidation states of elements in it. The survey spectrum (Fig. 2a) confirms the presence of Co, Fe, and Se in the material, besides the presence of C and O is indicative. As seen in Fig. 2b, the peaks related to Co 2p1/2 were appearing at 798.12 eV and 802.79 eV and the two other peaks at 782.90 eV and 786.31 eV. These peaks are the characteristics of Co3+ and Co2+.58 The XPS spectrum of Fe (Fig. 2c) shows peaks at 711.96 eV and 714.56 eV which are delineated with Fe2+ 2p3/2 and Fe3+ 2p3/2 respectively. In addition to these two peaks, another peak observed at 726.10 eV was characteristic of Fe 2p1/2.57 The two satellite peaks obtained at the binding energies of 719.08 eV and 732.12 eV is an excellent proof for the existence of bivalence for Fe in Co0.8Fe0.2Se2. The XPS spectrum of selenide (Fig. 2d) had two peaks at 52.06 eV for 3d5/2 and 57.30 eV for 3d3/2, respectively, indicating the existence of the metal–selenium bond.


image file: d2ra00447j-f2.tif
Fig. 2 The XPS spectrum of Co0.8Fe0.2Se2. (a) Survey spectrum showing the presence of requisite elements. (b–d) The binding energy values for Co 2p, Fe 2p and Se 3d energy levels.

3.2. Morphology and surface area

The FESEM and TEM images (Fig. 3 and 4) were investigated to ascertain the morphological metaphors of synthesized materials, while EDAS (Fig. S1) was used to chalk out elemental analysis. Fig. 3a and b show that Co0.8Fe0.2S2 particles acquired spherical morphology. The spheres outer surface looks like a loose texture type, probably because of the absence of an external surfactant in the synthesis process. As observed in both low and high magnification FESEM images, the spheres are fused. The average particle size determined for Co0.8Fe0.2S2 was ∼112 nm.
image file: d2ra00447j-f3.tif
Fig. 3 The morphological analysis of chalcogenide materials. (a and b) Low and high magnification FESEM images of Co0.8Fe0.2S2 showing sphere type morphology (c and d) low and high magnification FESEM images of Co0.8Fe0.2Se2 showing flower type morphology.

image file: d2ra00447j-f4.tif
Fig. 4 The TEM images of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 (a and b) and HRTEM images (c and d).

The Fig. 3c and d show flowers with flakes type morphology for Co0.8Fe0.2Se2. Both low and high magnification FESEM reveal flower-like morphology delineated with thin flakes for Co0.8Fe0.2Se2. Many spaces and porous surfaces are visible from the flowers showing that they can be promising materials for electrochemical processes. The elemental composition determined from EDAS (Fig. S1) for both the materials exposed the good dispersal of elements Co, Fe, S, and Se. The TEM images (Fig. 4a and b) indicate that the materials show similar morphologies as in FESEM. The HRTEM images (Fig. 4c and d) show that the lattice fringes with d-spacing of 0.28 nm and 0.24 nm corresponding to (100) and (101) planes of Co0.8Fe0.2S2, whereas the lattice fringes with d-spacing value 0.39 nm corresponds to (110) plane of Co0.8Fe0.2Se2 respectively. The results obtained from HRTEM are therefore in good agreement with PXRD results of both Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 respectively.

The present study aims to develop surfactant-free materials to exhibit excellent catalytic properties. The surface area of any material is the most crucial factor in explaining its catalytic activities. The specific surface area and pore size distribution were determined by studying BET isotherms. The Fig. 5a and b depict the N2 adsorption–desorption isotherm of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials representing the specific surface area. The calculated surface area for Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 was 10.69 and 21.41 m2 g−1. Besides the surface area, the pore size distribution, as determined by BJH plots (Fig. 4c and d), was 18.753 Å and 17.147 Å for Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials confirming the mesoporous nature of synthesized materials. The large surface area of Co0.8Fe0.2Se2 materials shows that more active sites will be available, and hence more diffusion of electrolytic solution into pores will take place, thereby showing better catalytic performance.


image file: d2ra00447j-f5.tif
Fig. 5 Surface area analysis of (a) Co0.8Fe0.2S2 and (b) Co0.8Fe0.2Se2 materials. The pore radius of (c) Co0.8Fe0.2S2 and (d) Co0.8Fe0.2Se2.

3.3. Optical properties

The UV-Visible DRS spectra of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 revealed their optical properties (Fig. S2). The absorption spectrum shows the materials absorbing mainly in the visible region with onset absorption at 260 nm. The broadband absorption was extending from 400 to 700 nm with maximum absorption at 650 nm. The broad absorption peak might be because of the morphological differences as we experience an inherent property shown by all the nanomaterials based on their size and shape. The energy bandgap (Eg) can be estimated from (αhν)2 vs. hν plot by projecting the straight line to hν axis were the point of intersection confirms the band value as shown in equation (2).68
 
αhγ = A(Eg)2 (2)

In this equation, α represents optical adsorption constant, h is the Planck constant; ν is the frequency of light; Eg is the band edge value. From the DRS spectrum of these materials, the bandgap calculated were 1.52 eV for Co0.8Fe0.2S2 and 1.57 eV for Co0.8Fe0.2Se2. The low bandgap of spheres is because of quantum confinement, which results in a blue shift.

3.4. Transient photocurrent (TPC) and electrochemical impedance spectroscopy (EIS) studies

The TPC and EIS studies were carried on Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials to understand the effect of clean and template free surfaces on electro catalytic properties. A three-electrode system, consisting of a conductive FTO glass plate on which the catalytic materials (Co0.8Fe0.2S2 and Co0.8Fe0.2Se2) were drop-cast to form a thin film acting as a working electrode, Pt as a counter electrode, and Ag/AgCl as a reference electrode, was set up to study the TPC properties. The materials remain attached to FTO using Nafion as a binder, and the LED light (200 W) of wavelength 456 nm served as the source for visible light radiations. The 0.1 M sodium sulfate (pH 7) solution was used as the electrolyte solution.

When the Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials were used in the dark, no photocurrent response was observed (Fig. 6a). A similar phenomenon was observed for blank FTO, but when loaded FTO was used, an appreciable photo response was observed when exposed to the visible light source. As shown in Fig. 6a with alternate on–off cycles, the spikes of transient photocurrent responses were observed for Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials loaded on FTO. The photocurrent responses achieved were stable and with high intensity. The uniform and high transient photocurrent values indicate an efficient separation of photo excited charge carriers on the FTO glass loaded with Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials.


image file: d2ra00447j-f6.tif
Fig. 6 (a and b) Transient photocurrent and impedance measurements (c and d) CVs obtained for 0.1 mM Cr(VI) in different acid electrolytes (H2SO4, HNO3, HCl all 0.1 M) using GCE/Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 at a scan rate of 10 mV s−1 (e and f) CVs of different Cr(VI) concentrations using GCE/Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 at a scan rate of 10 mV s−1 in 0.1 M HCl.

The resistance to the flow of charge carriers and the recombination rate were investigated further by recording EIS. The EIS spectra were obtained at a frequency of 100 kHz and alternating current (AC) voltage amplitude of 10 mV with an open circuit potential of 1 V. The EIS results are represented by the Nyquist plot (Z imaginary vs. Z real) in Fig. 6b. From the Nyquist plots, it is observed that the smaller arc radius is obtained for Co0.8Fe0.2S2 compared to Co0.8Fe0.2Se2, showing that the interfacial charge transfer process is smooth and the resistance offered to the flow of charge carriers is less for Co0.8Fe0.2S2 than Co0.8Fe0.2Se2. The small size of arc radius of Co0.8Fe0.2S2 indicates superior catalytic performance than Co0.8Fe0.2Se2.

3.5. Electrocatalytic water splitting using Co0.8Fe0.2S2 and Co0.8Fe0.2Se2

The capabilities of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 materials as the catalysts in OER are evaluated by the LSV (Fig. 7a) and CV (Fig. 7c–f) measurements using a typical homemade three-electrode system. Highly reactive electro active sites were created on GCE by modifying it with Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 to achieve an excellent oxygen evolution reaction (OER). The achieved over potential during LSV measurements was calculated as E(RHE) −1.23 V. As shown in Fig. 6a, Co0.8Fe0.2Se2 (345 mV η @ 10 mA cm−2 and 425 mV η @ 50 mA cm−2) resulted in relatively less over potential than Co0.8Fe0.2S2 (350 mV η @ 10 mA cm−2 and 475 mV η @ 50 mA cm−2). Whereas GCE results in negligible OER current indicating Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 have strong OER catalytic ability. The low over potential resulting from the electrode modification demonstrated Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 as unique types of electro catalysts.
image file: d2ra00447j-f7.tif
Fig. 7 (a) LSV curves, (b) Tafel plots, (c and d) Cdl measurements, (e) ECSA measurements, (f) stability of electro catalysts and (g) chronoamperometric (JV) measurements in 1 M KOH of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2.

Furthermore, Co0.8Fe0.2Se2 precatalysts OER kinetics (Tafel plots) is also favourable towards OER and consistent with reports. It was derived from the Tafel equation as follows, η = a + b[thin space (1/6-em)]log[thin space (1/6-em)]|J| by fitting the linear portion of LSV curves.35 Tafel plots (Fig. 7b) of Co0.8Fe0.2Se2 (52.4 mV dec−1) and Co0.8Fe0.2S2 (84.5 mV dec−1) are very smaller than bare GCE (130.1 mV dec−1). The observed values of over potential and Tafel slopes obtained for our materials (Co0.8Fe0.2Se2 and Co0.8Fe0.2S2) are superior to the reported ones as shown in Table 1. In general, this robust OER could have resulted from unique surface behaviours, multicomponent synergistic environments and unique morphology of electro active sites, which leads to improved electron transport and enhanced current densities.16,17,34,40–42

Table 1 Comparison of OER performance of cobalt–iron Chalcogenides prepared in present work with the OER performance of electrodes reported in the literature
Materials Material form Overpotential @ 10 mA cm−2 (mV) Tafel slope (mV dec−1) Electrolyte Ref.
CoFeP Powder 350 59 1 M KOH 69
CoS2 Film 361 64 1 M KOH 70
Co3S4 Powder 360 84.7 1 M KOH 71
Co-NP Powder 390   0.1 M KOH 72
Co1−XS–N and S codoped graphene Powder 371 63 0.1 M KOH 73
O doped CoS2 Film 370 67 1 M NaOH 74
CoS–Co(OH)2@aMoS2+x Film 380 68 1 M KOH 75
NiCoS/Ti3C2Tx Powder 365 58.2 1 M KOH 76
Co9S8@CNFs Powder 512 78 1 M KOH 77
Co0.8Fe0.2Se2 and Co0.8Fe0.2S2 Powder 345, 350 52.4, 84.5 1 M KOH This work


For superior electro catalysis, the materials should obtain higher current densities with lower over potential and Tafel values, which is observed here for Co0.8Fe0.2Se2, confirming it better electro catalyst than Co0.8Fe0.2S2 and bare GCE. Moreover, the insight into electrode kinetics of modified electrodes is evaluated using double-layer capacitance (Cdl) and electrochemical surface area (ECSA). Generally, ECSA is directly proportional to Cdl values. The Cdl measurements of Co0.8Fe0.2Se2 and Co0.8Fe0.2S2 (Fig. 7c and d) using cyclic voltammetry are carried with various scan rates from 0.02 to 0.002 V s−1 in 1 M KOH solution. Co0.8Fe0.2Se2 possesses an excellent Cdl value than Co0.8Fe0.2S2, hence higher value of ECSA of 0.853 mF cm−2 for Co0.8Fe0.2Se2 than 0.589 mF cm−2 for Co0.8Fe0.2S2 (Fig. 7e). Therefore, the higher Cdl value of Co0.8Fe0.2Se2 is evidence of having an enormous number of active catalytic sites and high surface area of Co0.8Fe0.2Se2 catalyst, resulting in enhanced electro catalytic performance.

In addition, the electro catalytic durability of both Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 hybrid electro catalysts are evaluated through continuous 1500 CV cycling measurements (Fig. 7f). These experiments showed Co0.8Fe0.2Se2 has negligible current density loss than Co0.8Fe0.2S2 after 1500 CV cycles measurements, which indicates the high electro catalytic stability of Co0.8Fe0.2Se2. To evaluate the electro catalytic stability of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2, we have conducted chronoamperometry (it) studies (Fig. 7g). The chronoamperometry (it) studies of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 shows that the materials are stable for more than 18 h of activity. The current density of the electro catalyst was identified to be almost equal for a long time. The small sudden change in the current density at 8–10 h was due to the bubble formation, which blocks the active site, and then it remained stable upto 18 hours.

Remarkably, these results emphasize that Co0.8Fe0.2Se2 and Co0.8Fe0.2S2 produced through our HMDS assisted one-pot approach can perform as a class of efficient catalysts in alkaline OER electro catalysis. Consequently, exceptionally high surface area and mesoporous behaviours resulting from our novel approach of producing Co0.8Fe0.2Se2 and Co0.8Fe0.2S2, have made them suitable candidates to achieve effective redox kinetics. Besides the above factors, the template free approach leads to the easy access of substrates towards the active sites on catalysts surface, resulting in enhanced performances.67 Thus, the decreased charge transport barriers led to good OER performance.

3.6. Electrochemical Cr(VI) reduction using Co0.8Fe0.2S2 and Co0.8Fe0.2Se2

For electrochemical Cr(VI) reduction, the nature of the electrolytic medium is an essential criterion. The acidic medium is suggested to be the best-suited media for carrying Cr(VI) reduction to Cr(III).78 Therefore, we have performed the electro catalytic reduction of Cr(VI) in different acidic media (H2SO4, HNO3 and HCl) having similar pH. The Fig. 6c and d represents the CV of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 electro catalysts in 0.1 mM Cr(VI) concentration loaded on GCE in different acidic media. A well-defined CV curve for Cr(VI) reduction is obtained in HCl medium for both the electro catalysts in the potential window of 0.0 V to −0.2 V compared to H2SO4 and HNO3 in similar conditions. Besides this, the maximum value of current is obtained for both the electrocatalysts in the HCl medium, indicating it as a suitable acidic medium to carry electrocatalytic Cr(VI) reduction.

The effect of different concentrations of Cr(VI) was studied to comprehend further understanding. The Fig. 6e and f show a substantial increase in current for Cr(VI) reduction when the Cr(VI) concentrations increase from 0.01 μM to 50 μM. The very characteristic current peak value shows a direct proportional relationship with Cr(VI) concentration at the potential window of 0.0 V to −0.2 V, indicating the reduction of Cr(VI) to Cr(III) increases. When the peak current is calibrated against the Cr(VI) concentration of 0.01 μM to 50 μM, a linear relation is observed with a correlation coefficient of 0.956 and 0.934 for Co0.8Fe0.2S2 and Co0.8Fe0.2Se2, respectively (Fig. S3a and b). The limit of detection (LOD) of Cr(VI) based on the signal-to-noise ratio 3.3 was calculated as 0.159 μg L−1 and 0.196 μg L−1 for Co0.8Fe0.2S2 and Co0.8Fe0.2Se2, and observed that these limits are similar to the reported observation.78 Furthermore, CVs with different scan rates for 10 μM Cr(VI) concentration were reported from the potential range of 20 mV s−1 to 200 mV s−1 in 0.1 M HCl using modified GCE electrode loaded with Co0.8Fe0.2S2 and Co0.8Fe0.2Se2 (Fig. S3c and d). A slight negative shift is observed with the increase in scan rates, showing the Cr(VI) reduction reaction's irreversible nature.79,80

As described above, the electrochemical Cr(VI) reduction is best carried under an acidic medium, where it shows that the more is H+ ions available, the more the chances of reduction. According to the reported literature explaining the mechanism for Cr(VI) reduction, it is found that Cr(VI) reduction involves one electron and one proton transfer at a time, resulting in the disproportionation of Cr(VI) to Cr(IV) and Cr(VI) species. The Cr(IV) disproportionate further with Cr(V) to Cr(III) and Cr(VI), and it continues until complete reduction to Cr(III) takes place.78–80 The total number of electrons involved in the reduction process counts upto 3. Overall, in electrochemical Cr(VI) reduction to Cr(III), superior performance is observed for Co0.8Fe0.2S2 electro catalyst compared to Co0.8Fe0.2Se2. This might be probably due to the effect of morphology involving spherical materials as a best suited for Cr(VI) reduction where maximum of Cr(VI) ions get adsorbed on the surface than in case flower shaped selenium materials.

4. Conclusions

In this work, a pair of transition metal (Co, Fe) based metal chalcogenides (Co0.8Fe0.2S2 and Co0.8Fe0.2Se2) were synthesized using the newly developed HMDS-assisted one-pot synthesis method. The synthesized materials were characterized by a series of comprehensive physicochemical characterization tools. The electro catalytic water splitting for OER showed that the synthesized materials could serve as robust electro catalysts. The material Co0.8Fe0.2Se2 showed superior OER activity than Co0.8Fe0.2S2 as indicated by the low overpotential and Tofel values (345 and 350 mV η @ 10 ms A cm−2, 52.4 and 84.5 mV dec−1 for Co0.8Fe0.2Se2 and Co0.8Fe0.2S2, respectively). The electrochemical Cr(VI) reduction to Cr(III) further explains the bifunctional catalytic ability of Co0.8Fe0.2S2 and Co0.8Fe0.2Se2, where a maximum current and lower LOD is observed for Co0.8Fe0.2S2 as compared to Co0.8Fe0.2Se2. The materials showed potential to be excellent bifunctional electro catalysts for OER and Cr(VI) reduction.

Author contributions

Manzoor Ahmad Pandit, Dasari Sai Hemanth Kumar – data curation, formal analysis, investigation, methodology, writing – original draft. Krishnamurthi Muralidharan – conceptualization, supervision, funding acquisition, writing – review & editing. Manigandan Ramadoss, Yuanfu Chen – methodology, validation, visualization.

Conflicts of interest

The authors declare no conflicts of interest.

Acknowledgements

M. A. P thanks to UGC-BSR for fellowship. We thank to Centre for Nano Science and Technology (for TEM) and School of Physics (for PXRD) University of Hyderabad. Financial and infrastructure support from the University Grants Commission, New Delhi, India (through the UPE and CAS programs) and the Department of Science and Technology, New Delhi, India (through the PURSE and FIST programs) are gratefully acknowledged.

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Footnote

Electronic supplementary information (ESI) available: ESAS, UV-Vis DRS spectra, Data on controlled reactions and recyclability study and peak current study. See DOI: 10.1039/d2ra00447j

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