Open Access Article
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One-pot facile simultaneous in situ synthesis of conductive Ag–polyaniline composites using Keggin and Preyssler-type phosphotungstates

Abbas Amini *ab, Marjan Rahimi c, Marziyeh Nazari d, Chun Cheng e and Bijan Samali a
aCentre for Infrastructure Engineering, Western Sydney University, Kingswood Campus, Bld Z, Locked Bag 1797, Penrith, NSW 2751, Australia. E-mail: a.amini@westernsydney.edu.au; a.amini@ack.edu.kw
bDepartment of Mechanical Engineering, Australian College of Kuwait, Mishref 13015, Kuwait
cDepartment of Chemistry, Mashhad Branch, Islamic Azad University, Mashhad, Iran
dMathematics Department, Australian College of Kuwait, Mishref, Kuwait
eDepartment of Materials Science and Engineering, South University of Science and Technology, Shenzhen, China

Received 31st October 2018 , Accepted 22nd December 2018

First published on 21st January 2019


Abstract

Two heteropolytungstate structures, Keggin (H3PW12O40) and Preyssler (H14[NaP5W30O110]), were used to synthesize conductive silver nanoparticle–polyaniline–heteropolytungstate (AgNPs–PAni–HPW) nanocomposites. During the oxidative polymerization of aniline, heteropolyblue was generated and served as the reducing agent to stabilize and distribute AgNPs within “PAni–Keggin” and “PAni–Preyssler” matrixes as well as on their surfaces. The prepared nanocomposites and AgNPs were characterized using UV-visible (UV-Vis) and Fourier-transform infrared spectroscopy (FT-IR), X-ray diffraction (XRD), pore size distribution BET, scanning electron microscopy (SEM), and transmission electron microscopy (TEM). UV-Vis results showed different stages of the formation of metal NPs embedded in the polymer–HPW composites, and FT-IR spectra presented characteristic bands of PAni, Keggin and Preyssler anions in the composites confirming no changes in their structures. The presence of AgNPs and an intensely crystalline matrix were confirmed by the XRD pattern. The BET surface areas were found to be 38.426 m2 g−1 for “AgNPs–PAni–Keggin” and 29.977 m2 g−1 for “AgNPs–PAni–Preyssler” nanocomposites with broad distributions of meso-porous structure for both nanocomposites. TEM and SEM images confirmed that the type of heteropolyacids affected the size of AgNPs. This is the first report that uses Keggin and Preyssler-type heteropolytungstate to synthesize “AgNPs–PAni–HPW” nanocomposites in an ambient condition through a low-cost, facile, one-pot, environmentally friendly and simultaneous in situ oxidative polymerization protocol.


1. Introduction

Conductive polymers (CPs) are highly conjugated pi-bonded polymers with unique conductivity as a result of their delocalization of electrons.1–3 The extended π-conjugated electron block, existing in CP molecules, originates their low energy optical transitions and high values of electrical conductivity, mechanical flexibility and surface areas. Significant electron affinity and porous structure of CPs extend their applications to useful substances for the incorporation of nanoparticles (NPs) in polymers. Incorporating metal NPs (MNPs) in organic–inorganic hybrid materials enhances their conductivity4 and active surface area, due to the facilitation of charge transfer between the substrate and dispersed NPs in the matrix of hybrid composites.5 Conductive polymeric metal NPs (CP-MNPs) composites have shown significant electric, electronic and optical properties, as well as high mechanical flexibility and porosity.6 These characteristics have directed CP-MNPs composites to various applications in organic light emission diode (OLED), photovoltaics (PV), and electrochromic devices (ECD).7,8

Many textures have been used for CPs, including: polyaniline (PAni), polyacetylene (PA), polythiophene (PTh), polypyrrole (PPy), polyphenylenevinylene (PPV), polyN-vinylcarbazole (PNVC), polyfluorene, polyindole, and their substituted derivatives. These compounds have extended inspiring applications of CPs to rechargeable batteries, microelectronics, sensors and electrochromic displays.9–11 Among these textures, PAni has desirable surface area, mesoporous nature, simple preparation, low cost, high catalytic property, high redox and ion-exchange properties, as well as tunable electrical conductivity property (resulted from the flexible –NH group in its backbone), and good chemical and environmental stability in both air and solutions.11 Aniline has three idealized oxidation states: fully reduced state (leucoemeraldine, colorless), fully oxidized state (pernigraniline, purple), and partially oxidized state (emeraldine base, blue color, and emeraldine salt, green color). In fact, the conductivity of common semiconductors (10−4 to 102 S cm−1), exceeding from the conductivity of common polymers (<10−12 S cm−1), is originated from the conductivity of emeraldine salt (unsoluble).12 The desired properties of electrical conductivity and morphology of PAni nanostructures (different for nanofibers, nanorods, nanotubes, nanowires and nanospheres) can be simply tuned depending on the type of dopant, the type and ratio of oxidant to monomer concentration, the temperature, the acidity of reaction, and the applied polymerization instructions.13 PAni has been used both as a filler14 and matrix15–18 material to achieve the desired properties of hybrid materials. The processability of PAni makes it suitable for the fabrication of polymer matrix of composites by incorporating conducting materials such as CNTs13 and various MNPs as fillers. As a result of these unique properties, PAni can be one of the best platforms for synthesizing nanocomposites through doping with various metallic nanostructures.19 Thus, PAni can be one of the most promising active materials suitable for pseudo-capacitor electrodes and super-capacitors,19,20 corrosion inhibitors, electrochromic display structures, electro-optic and smart windows for energy storage in secondary batteries, and a membrane for OLED devices.21 Due to its biocompatibility, PAni has been also used in biosensors, cell simulators, bio-actuators and drug delivery systems.22–24

CP-NPs composites are synthesized through: electrochemical deposition,9,15,24–26 solution or drop casting,27,28 layer-by-layer self-assembly,29,30 and entrapment into sol–gel matrices.16,31–34 Most of these conventional methods and materials have limitations and disadvantages including: process complexity, toxicity, high cost, environmental problems, time-consuming, high energy loss, low efficiency and low doping.6,24 Hence, producing modern CP-NPs composites with favorable properties and their corresponding synthesized methods have faced the following challenges. First, the agglomeration of NPs in the polymer matrix that should be avoided by using a suitable solvent. Second, the polymerization, formation and concurrent incorporation of MNPs into a CP matrix that should be spontaneous under ideal conditions (e.g., typical ambient temperature). When the number of steps in sequential reactions is reduced, the fabrication of composite occurs under a higher efficient process. It also receives the same benefits when the reaction is concluded in one container-solution-reagent. Third, the reductive agent for immobilization and stability of NPs that should be non-toxic and environmentally friendly.

To overcome these challenges and provide ideal conditions for simultaneous reactions for polymerization, formation, and homogeneous distribution of metallic NPs, we used heteropolyacids (HPAs) to incorporate into the PAni matrix as dopant anions which not only has strong acidic properties for providing an ideal environment for the polymerization of monomers such as aniline, but it also has high oxidizing potential for readily acquiring and releasing several electrons per molecule.

Generally, HPAs are categorized under anionic metal-oxide clusters of d-block transition metals with high oxidation states (WVI, MoV,VI, VIV,V) and various size, structure, composition and functions.35 Due to their inherent ability (vacant d molecular orbitals), HPAs can undergo fast, reversible, stepwise redox reactions under mild conditions while retaining their intact structures.36 Highly negatively charged nature of HPAs is desirable for the molecular dispersion of HPAs on the positively charged backbone of a polymer. This alleviates the aggregation of AgNPs while silver ions are electronically embedded into the PAni matrix.37 So, during the oxidative polymerization of aniline, Keggin and/or Preyssler heteropolyanions can transfer electron from aniline to silver ions and, thus, serve as the protonating, reducing and stabilizing agents for the reduction and stabilization of silver ions in the CP framework. The role of HPAs in the synthesis and stabilization of NPs is reviewed in the light of many recent developments of these hybrid materials by various synthesis techniques. Table 1 presents the recent studies on CP-NPs composites using different NPs, CPs and HPAs.

Table 1 Recent advances in using HPAs for synthesizing nanoparticles-based conductive polymer composites
Nanoparticle Conductive polymer Method Advantages; disadvantages Heteropolyacid Ref.
a POM has the same meaning as heteropolyacid. b Poly.: polymerization.
MoO2 [Cu2(BTC)4/3(H2O)2]6[POM]·(C4H12N)2·xH2O (BTC = 1,3,5-benzenetricarboxylate) (POMa–MOF) Thermolysis in N2, calcination at 600 °C Well-defined polyhedral POM–MOF single crystals; high temperature, ex situ poly.,b time-consuming, multi-stage Keggin-type, H3PMo12O40 8
Au Polypyrrole (PPy) Electrodeposition and cyclic voltammetry technique High sensitivity; time-consuming, preparation of electrode prior to coating needs professional operators, multi-stage K7PMO2W9O39·H2O, (α-POM) 9
Poly(3,4-ethylenedioxythiophene) (PEDOT) Electrodeposition (LBL) self-assembly High sensitivity; time-consuming, preparation of electrode prior to coating, multi-stage Keggin-type H6[PMo9V3O40] 24
Poly(diallyldimethyl-ammonium chloride) functionalized reduced graphene oxide (PDDA-RGO) Electrodeposition (LBL) self-assembly Thickness controllability; multi-stage, complex, time-consuming, ex situ poly., using H2SO4 and HCl Dawson-type K8P2W16V2O62 26
CNT Layer-by-layer (LBL) self-assembly Simple, versatile and wide range of materials can be used for film assembly, reversible; using many chemicals plus HCl, complex Dawson-type K6P2W18O62 or [P2W18O62]6− or (P2W18) 30
Reduced graphene oxide (RGO) Chemically reduced with NaBH4/PMo12 solution Well-dispersed NPs, low tendency to agglomeration; using many chemicals, multi-stage Keggin-type, H3PMo12O40 38
Polyaniline (PAni) In situ oxidative poly. One-pot, in situ, room temperature, aqueous solution; uncontrollable because of very fast reaction 18
Poly(3,4-ethylenedioxythiophene) (PEDOT) Reduction Aqueous solution; using several expensive electrodes, multi-stage, time-consuming, complex Keggin-type, H3PMo12O40 39
SiO2 MPTMS as precursors, glutaraldehyde (GA, as cross linker), polyvinylpyrrolidone (PVP) Sol–gel and solution casting Well-dispersed NPs, controlled thickness; needs stepwise and slow different heating stages, time-consuming, multi-stage Keggin-type, H4SiW12O40 32
Sulfonated polysulfone (sPSU) Solution casting Uniform and homogeneous NPs dispersion; agglomeration for high NPs concentrations, difficult for electrode fabrication due to insolubility Keggin-type, H3PMo12O40 27
Polyimide (PI) In situ sol–gel Homogeneous dispersion of NPs; high temperature, stepwise H3PMo12O40 (Dawson and Keggin-type) 33
Nafion Multiphase self-assembly Uniform nano-arrays of hexagonal cylinder along the channels direction with long-range order; using and removing surfactant at the end, time-consuming, multi-stage Keggin-type, H3PW12O40 40
Ru4POM PPy, PAni, PEDOT Electrodeposition Room temperature; using several expensive electrodes and requires special instruments, multi-stage, [Ru4O4(OH)2(H2O)4(γ-SiW10O36)2]10− (Ru4POM) 15
Pt– Cs2.5H0.5PW12O40 Sulfonated poly ether ether ketone (SPEEK) In situ electrochemical Moderate temperature; expensive, time-consuming, ex situ poly. Pt–Cs2.5H0.5PW12O40 41
Pt Poly(diallyldimethylammonium chloride)functionalized reduced graphene oxide (PDDA-RGO), (PDDA-CNT) Electrodeposition Non agglomerate NPs; multi-stages, expensive [PW11NiO39]5− 25
PWA–silica–NH2 Sulfonated poly arylene ether sulfone (SPAES) Sol–gel and solution casting Controllable; ex situ poly., multi-stage, time-consuming, Keggin-type, H3PW12O40 31
Au–Pd Quartz, silicon, ITO Layer-by-layer (LBL) self-assembly Simple, versatile and wide range of materials can be used for film assembly, eco-friendly; costly, multi-stage, ex situ, reversible Dawson-type K8P2W16V2O6218H2O (P2W16V2) 29
Titanium(IV) molybdophosphate (TMP) Poly(3-methylthiophene) (P3MTh) In situ oxidative poly. Dense and globular TMP in matrix, in situ poly.; agglomeration, using H2SO4 and HCl, multi-stage Ti4PMo12O40 42
Pd/Ni RGO Wet-chemical Facile chemical method, aqueous solution; high temperature, costly, multi-stage Keggin-type, H3PW12O40 36
Molybdenum phosphide (MoP) Carbon quantum dots (ECQDs) Charge-directed self-assembly, phosphatizing at 700 °C High efficient, using no noble metals; high temperature, ex situ poly., time-consuming, multi-stage, using HCl Keggin-type, H3PMo12O40 37
Tungsto-molybdate (TM) Poly(aniline-co-o-toluidine), PAni-Co-OT Sol–gel Reproducible; needs controlling temperature and pH, using HCl Tungsto-molybdate (TM) 17
CsPW (Cs2.5H0.5PW12O40) and the PWS (H3PW12O40/SiO2) End-group cross-linkable, sulfonated fluorinated biphenol (ESF-BP), poly(arylene ether) Aromatic nucleophilic substitution polycondensation Enhanced physico-chemical properties, thickness controllability; high temperature, ex situ poly., time-consuming, multi-stage CsPW (Cs2.5H0.5PW12O40) and the PWS (H3PW12O40/SiO2) 43
PAni–HPMo Polyethersulfone (PES) Phase inversion Controlled dispersion of NPs; needs very low temperature and excess solvent for neutralizing, wide range of NPs size:120–700 nm Keggin-type, H3PMo12O40 14
Pd Graphene In situ self-assembly Mild, facile, economical, surfactant-free; expensive novel metal 44
Pt–Ru Graphene Modified hummers method, (microwave heating) Uniformly dispersed NPs.; expensive, time-consuming, using special instruments 45
Keggin-type, H3PW12O40 (HPW) Ordered SiO2 matrix on spherical monodispersed PS as template Evaporation-induced self-assembly (EISA) Well-ordered macro-porous and 2D hexagonal meso-structures, single step; using nonionic surfactant Keggin-type, H3PW12O40 46
Ordered TiO2 matrix on spherical monodispersed PS as template Solution, calcination at 400 °C Ordered frameworks with hierarchical architectures and 2D hexagonal meso-structures; high temperature, ex situ poly., time-consuming, multi-stage 47
CeO2/Pt RGO Solution casting Uniformly loaded spherical NPs into the matrix; high temperature, costly, multi-stage, ex situ poly., using HCl H3PMo6W6O40 (PMo6W6) 28
Poly(vinylimidazolium) cation [PVIM+]/Na12Co5POM Nitrogen-doped CNT (NCNTs) Ion-exchange method Formation of fairly homogeneous layer around the NCNTs, enhancing the electron transport, removing interferences; multi-stage, time-consuming, using HNO3 Sandwich-type Na12[WCo3(H2O)2(CoW9O34)2] 48


Keggin-type heteropolytungstic acid (H3PW12O40, HPW, phosphotungstic acid) belongs to the HPAs group with a central PO4 tetrahedron surrounded by twelve WO6 octahedrons with Td symmetry (Fig. 1a). It is the most widely used acid and oxidation catalyst for many reactions in industrial processes, such as electrophilic catalyses and oxidation reactions.46 Mono-Na+-encapsulated Preyssler-type phosphotungstic acid with the formula of H14[NaP5W30O110] consists of a cyclic arrangement of five PO4 tetrahedrons surrounded by thirty WO6 octahedrons (Fig. 1b). They are connected to each other from the edge and corner-sharing oxygen atoms assembled with D5h symmetry where the central cavity is occupied by one sodium ion.49,50


image file: c8ra09029g-f1.tif
Fig. 1 (a) Keggin-type structure, (b) Preyssler-type structure.

Preyssler polyanion possesses distinct properties that make it a unique heteropolyanion in comparison to the rest of HPAs family. These properties are as follow: (1) strong Brønsted acidity due to the presence of 14 acidic protons, which make it as an efficient solid “super acid”, (2) high thermal and hydrolytic stability (in pH 0–12 environment), compared to Keggin and Dawson structures, (3) insensitivity to water, (4) recyclability (being green), (5) high oxidation potential, (6) high surface area (Preyssler is the largest polyanion among HPAs), (7) reversible transformation, and (8) solubility in polar and non-polar solvents. Thus, while the pH (acidity) of the reaction mixture has an intense effect on the successful control of PAni synthesis,51 the Preyssler heteropolyanions can be excellent and more effective acidic catalysts than Keggin group to replace the conventional acids, such as H2SO4, HCl, HNO3 and HF, by creating an eco-friendly acidic environment for synthesizing and polymerization of PAni. There is only one report on synthesizing Ag–PAni nanocomposites using Keggin-type phosphomolybdic acid (HPMo) in an aqueous solution by in situ oxidative polymerization method.18 In addition, AgNPs–PAni composites were synthesized using Keggin-type phpsphotungstic acid (HPW) through a sol–gel method.16 Nevertheless, there is yet no report on utilizing the Preyssler-type for synthesizing CP-NPs composites.

In the present study, we focus on the synthesis of silver-incorporated PAni–HPW nanocomposites using Keggin (H3PW12O40) and mono-Na+-encapsulated Preyssler-type (H14[NaP5W30O110]) phpsphotungstic acids, along with their characterizations and comparisons. This report introduces a facile one-pot simultaneous in situ oxidative polymerization synthesis protocol to fabricate “AgNPs–PAni–Keggin” and “AgNPs–PAni–Preyssler” nanocomposites, by significantly lessening the common agglomeration issue in AgNPs.52,53 The two green materials, Keggin and Preyssler structures, can serve as: (1) green acid protonating species for oxidative polymerization of aniline monomers by replacing common hazardous liquid acids; (2) dopant anions or stabilizing agents to facilitate the stabilization and distribution of AgNPs in the matrix of PAni nanostructures; and, (3) reducing agents for the reduction of silver ions to stabilize AgNPs decorated in the polymer–HPW matrix. Both synthesized three-component nanocomposites exhibited dispersed and stable spherical silver NPs doped in the polymer (Table 2).

Table 2 Recent methodologies for synthesizing “AgNPs–CP–HPA” composites
Conducting polymer Method Advantages; disadvantages Heteropolyacid Ref.
Polyaniline (PAni) Sol–gel Polydispersed NPs; two irregular morphology of NPs sizes, excess washing for removing acid H3PW12O40 (Keggin-type) 16
In situ oxidative polymerization One-pot, in situ, room temperature, aqueous solution; uncontrollable because of very fast reaction H3PMo12O40 (Keggin-type) 18
Polyvinyl alcohol (PVA) Electrospinning and photo-reduction Uniform dispersion of AgNPs, moderate temperature; ex situ, multi-stage Keggin-type, H4SiW12O40 54
Poly-o-anisidine Sol–gel Polydispersed NPs, enhanced thermal stability up to 600 °C; irregular morphology of NPs sizes, ex situ, left-over acid and oxidant in samples because of very fast reactionary acid and oxidant in samples H3PMo12O40 (Keggin-type) 34
Polybenzidine (PBz) Ultrasound-assisted Simple, room temperature; not very exact method, broadening XRD peak 55
Polyaniline (PAni) In situ oxidative polymerization Room temperature, facile, one-pot, reproducible, eco-friendly, simultaneous, stable AgNPs; low amount of chlorine in the medium H3PW12O40 (Keggin-type), H14NaP5W30O110 (Preyssler-type) This study


2. Material and methods

2.1. Reagents

Most of the chemicals were obtained from MERCK, Germany, and used as received without further purifications. Acetonitrile was purchased from SAMCHUN Pure Chemical Co., South Korea, and Cation Exchange Resin, Dowex-50W-x8, was obtained from Sigma Aldrich, USA. The Preyssler-type HPA was prepared in our laboratory. Aqueous solutions were prepared from double distilled deionized water. All the chemical reactions were carried out at room temperature.

2.2. Synthesis of “AgNPs–PAni–Keggin” composite

The “AgNPs–PAni–Keggin” nanocomposite was synthesized via a one-step reaction: 0.30 mL (3.33 mmol) of freshly doubled distilled aniline and 3.48 g (1.05 mmol) of Keggin-type phosphotungstic acid (H3PW12O40) were dissolved in 20 mL acetonitrile; a light orange complex was immediately formed. Then, 1 mL (2 M) of freshly prepared ammonium persulfate (APS) was added to the mixture drop-wise. Due to the formation of heteropolyblue, the color was changed to an intense blue color which indicated an electron transfer from aniline to Keggin (producing reduced Keggin). To this solution, 7.5 mL AgNO3 (0.01 M) aqueous solution was added and ultrasonicated for 5 minutes using a TOSHCON sonicator, 40 KHz 100 W, Germany. The reaction was stirred for 20 hours at room temperature. The mixture was poured onto 100 mL methanol; an immediate precipitation of the product occurred. The precipitate was centrifuged at 6000 rpm for 5 minutes and repeatedly washed with methanol until the filtrate turned colorless. The precipitate was washed with double distilled demineralized/deionized water three times to remove excessive oligomer. Unreacted heteropoly and oxidant were washed using acetone. The black solid sample (AgNPs–PAni–Keggin) was air dried and placed in a vacuum oven under 80 °C and stored in a desiccator for further characterizations.

2.3. Preparation of Preyssler-type sodium 30-tungstopentaphosphate (H14[NaP5W30O110])

In a 100 mL beaker, 40 mL distilled water was heated to 40–45 °C; then, 33 g (100 mmol) sodium tungstate dihydrate (Na2WO4·2H2O) was gradually added while stirring to dissolve thoroughly. The mixture was consolidated with ortho-phosphoric acid (25 mL, H3PO4, 85%), and transferred to a 100 mL flask where it was refluxed for 5 hours. After cooling down to ambient temperature, the content of flask was transferred to a beaker where pulverized potassium chloride (10 g KCl) was gradually added to the mixture and stirred for 30 minutes. The resultant light greenish precipitate was filtered and recrystallized in distilled water. After cooling, the needlelike white crystals, which contained Preyssler salt (Na1.5K12.5[NaP5W30O110]), were separated from the mixture by using a Büchner funnel and dried. In the next stage, to prepare Preyssler acid, the needlelike heteropoly crystals were dissolved in distilled water, and passed through a column (50 × 1 cm) of Dowex-50W-x8 (cation exchange resin). After evaporating the solvent at 70 °C, the Preyssler acid, H14[NaP5W30O110], was obtained as an off-green solid; it was characterized by IR test (Fig. 2c).
image file: c8ra09029g-f2.tif
Fig. 2 FT-IR spectra of: (a) pure Keggin-type structure, (b) “AgNPs–PAni–Keggin” nanocomposite, (c) pure Preyssler-type structure, and (d) “AgNPs–PAni–Preyssler” nanocomposite.

2.4. Synthesis of “AgNps–PAni–Preyssler” composite

The “AgNPs–PAni–Preyssler” nanocomposite was synthesized in a one-step reaction: 0.65 mL (7.15 mmol) of freshly doubled distilled aniline and 3.69 g (0.50 mmol) of Preyssler acid were dissolved in 30 mL acetonitrile; white precipitate was immediately formed. Then, 1.3 mL of freshly prepared APS (2 M) was added to the mixture drop-wise, where, owing to the formation of heteropolyblue, the color was changed to an intense blue color indicating an electron transfer from aniline to Preyssler (producing reduced Preyssler). To this solution, 12 mL AgNO3 (0.01 M) aqueous solution was added and ultrasonicated for 5 minutes in the sonicator. The reaction was stirred for 20 hours at room temperature. The mixture was poured onto 100 mL methanol, an immediate precipitation of product occurred. The precipitate was centrifuged at 6000 rpm for 5 minutes and repeatedly washed with methanol until the filtrate turned colorless. After that, it was washed three times with double distilled demineralized/deionized water to remove excessive oligomer. Unreacted heteropoly and oxidant were washed using acetone. The black solid sample (AgNPs–PAni–Preyssler) was air dried, placed in a vacuum oven at 80 °C, and stored in a desiccator for further characterizations.

2.5. Characterization of AgNPs embedded polyaniline–heteropolytungstate composites

A UV-Vis spectrophotometer (CARY50, VARIAN Spectrometer, Australia) was utilized to record different stages of the formation of “AgNPs–PAni–HPW” nanocomposite within the wavelength range 200–800 nm. Fourier transform infrared spectra (FT-IR) were recorded by a Nicolet (Thermo) Avatar 370 FTIR Spectrometer, USA, using the KBr pellet mode in the region of 4000–400 cm−1. A Transmission Electron Microscope (TEM, PHILIPS, model CM120, Netherland) was utilized at 120 K accelerating voltage. The Scanning Electron Microscopy (SEM) was carried out by Philips XL30 ESEM, at 20 KV voltage. The X-Ray Diffraction (XRD) patterns were recorded by a diffractometer, Explorer θθ, GNR, Italy, equipped with a dectris (fast strip) detector and fitted at 0.25 mm radiation entrance slit, using Ni-filtered Cu Kα radiation (k = 1.5418 Å at 0.01° scan rate in 2θ). The Brunauer–Emmett–Teller (BET) specific surface area of the samples was examined using PHS-1020 (PHSCHINA), China. The pore size distributions were calculated through the Barrett–Joyner–Halenda (BJH) method.

3. Results and discussion

In the present protocol, PAni-supported AgNPs, containing Keggin and Preyssler-type phosphotungstic acids, were prepared in a one-step reaction through simultaneous in situ oxidative polymerization of aniline in the presence of APS as the co-oxidant at room temperature. The experimental evidence, which proves the stability and existence of Keggin and Preyssler heteropolyanions incorporated to the PAni matrix, comes from the FT-IR spectra (Fig. 2a–d). In Fig. 2a, the FT-IR spectra of fingerprint bands of bulk HPW Keggin anion, [PW12O40]3−, are seen at 1080, 982, 891, 797 and 594 cm−1 which were slightly shifted to the bands at 1080, 978, 894, 805 and 595 cm−1 in correspondence to the FT-IR spectra of “AgNPs–PAni–Keggin” nanocomposite in Fig. 2b, which indicated that HPW retained its Keggin structure. Band shifts are identified as the reflection of strengthening and shortening of Keggin units upon doping in the PAni backbone (Table 3).46,56 In addition, Fig. 2b corresponds to FT-IR spectra of “AgNPs–PAni–Keggin” nanocomposite. This represents the characteristic bands of Keggin in the nanocomposite: the peaks of PAni at 1578 cm−1 and 1486 cm−1 (the deformation modes of benzene rings, benzoid and quinoid rings), 1304 cm−1 (C–N bending, vibration of aromatic amine), 1245 cm−1 (C–N+˙ stretching vibrations in the polaron structure representing the existence of conducting protonated PAni), and, 1148 cm−1 (stretching mode of protonated PAni).46,57,58
Table 3 FTIR peak assignment of Keggin structure (bolded) and “AgNPs–PAni–Keggin” nanocomposite
Wavenumber [cm−1] Peak assignment
3382 cm −1 O–H stretching
>3227 cm−1 N–H stretching of PAni
1578 cm−1 and 1486 cm−1 Stretching modes of deformed benzene rings, benzoid and quinoid rings of PAni
1304 cm−1 C–N bending (vibration of aromatic amine)
1245 cm−1 C–N+˙ stretching vibrations in the polaron structure representing the existence of conducting protonated PAni
1148 cm−1 C[double bond, length as m-dash]N stretching mode of protonated PAni
1080 cm −1 P–O stretching mode of central PO 4 tetrahedron
1080 cm−1 P–O stretching shift of Keggin dopped in “AgNPs–PAni–Keggin” nanocomposite
982 cm −1 W[double bond, length as m-dash]O stretching mode of exterior WO 6 octahedron of pure Keggin
978 cm−1 W[double bond, length as m-dash]O stretching shift of Keggin dopped in “AgNPs–PAni–Keggin” nanocomposite
891 and 797 cm −1 W–O–W stretching mode of corner and edge shared octahedron of pure Keggin
894 and 805 cm−1 W–O–W stretching shift of Keggin dopped in “AgNPs–PAni–Keggin” nanocomposite
594 cm −1 P–O bending of pure Keggin
595 cm−1 P–O bending shift of Keggin dopped in “AgNPs–PAni–Keggin” nanocomposite


The characteristic peaks of pure Preyssler unit, [NaP5W30O110]14−, are exhibited at 1164 and 1085, 939, 914, 768 and 534 cm−1 (Fig. 2c). In the IR spectra of synthesized “AgNPs–PAni–Preyssler” nanocomposite, peaks are located at 1151 and 1082, 984, 910, 782 and 510 cm−1 (Fig. 2d and Table 4). From the FTIR analysis, slight shifts confirm the existence of strong peaks of pure Preyssler and PAni. A strong electrostatic interaction between Preyssler and PAni matrix exists while the molecular structure of Preyssler anions is preserved during the incorporation with the nanocomposite (despite the larger size of Preyssler structure compared to Keggin). As there are strong covalent bonds in the defined structure of Preyssler molecule between oxygen and tungsten atoms, its structure is maintained after doping, although some deviations occur in its spatial form; this phenomenon is reflected in the slight shifts in IR spectra. Proper distribution of molecular active particles of Keggin and Preyssler heteropoly anions in the PAni nanostructures introduces them as excellent candidates for heterogeneous catalysis applications with enhanced performances.38

Table 4 FTIR peak assignment of Preyssler structure (bolded) and “AgNPs–PAni–Preyssler” nanocomposite
Wavenumber [cm−1] Peak assignment
3401 cm −1 O–H stretching
3423 cm−1 N–H stretching of PAni
1568, 1488 cm−1 Stretching modes of deformed benzene rings, benzoid and quinoid rings of PAni
1302 cm−1 C–N bending (vibration of aromatic amine)
1243 cm−1 C–N+˙ stretching vibrations in the polaron structure representing the existence of conducting protonated PAni
1164 and 1085 cm −1 P–O stretching modes of pure Preyssler
1151 and 1082 cm−1 P–O stretching shift of Preyssler dopped in “AgNPs–PAni–Preyssler” nanocomposite
768 cm −1 W[double bond, length as m-dash]O stretching mode of pure Preyssler
782 cm−1 W[double bond, length as m-dash]O stretching shift of Preyssler dopped in “AgNPs–PAni–Preyssler” nanocomposite
939 and 914 cm −1 W–O–W stretching mode of pure Preyssler
984 and 910 cm−1 W–O–W stretching shift of Preyssler dopped in “AgNPs–PAn–Preyssler” nanocomposite
534 cm −1 P–O bending of pure Preyssler
510 cm−1 P–O bending shift of Preyssler dopped in “AgNPs–PAni–Preyssler” nanocomposite


The optical properties of “AgNPs–PAni–Keggin” (Fig. 3a) and “AgNPs–PAni–Preyssler” nanocomposites (Fig. 3b) were analyzed using the UV-Vis spectrophotometry method at room temperature. Curve (I) in Fig. 3a illustrates the UV-Vis spectrum of Keggin-type solution with no obvious absorbance in the range of 400–800 nm. Curve (II) corresponds to the UV-Vis absorption of blue-colored solution (heteropolyblue) which contains reduced Keggin solution and oxidized aniline after adding APS.


image file: c8ra09029g-f3.tif
Fig. 3 UV-Vis spectra of (a) “AgNPs–PAni–Keggin” nanocomposite: (I) 10 mmol Keggin-type solution, (II) blue-coloured solution containing Keggin anion and Aniline, (III) after addition of AgNO3 to blue-coloured solution (II); and (b) “AgNPs–PAni–Preyssler” nanocomposite: (I) 10 mmol Preyssler-type solution, (II) blue-coloured solution containing Preyssler anion and aniline, (III) after addition of AgNO3 to blue-coloured solution (II).

An absorption band at 415 nm shows the transfer of one electron from aniline to Keggin (due to the electron transition to d orbitals of W). The broad weak peak at 700 nm is ascribed to the overlap of characteristic absorption of [PW12O40]3− and PAni.18 Color intensity increased due to the electron transition in the examined substances. Curve (III) shows the spectra of PAni–Keggin mixture to which AgNO3 solution was added to reduce the silver ions to AgNPs. Strong absorption peaks were observed at ∼450 and ∼573 nm because of the excitation of surface plasmon resonance (SPR) of AgNPs in “AgNPs–PAni–Keggin” nanocomposite, along with the transferring electrons from the internal orbitals (d) of Keggin to Ag ions (Fig. 3a, curve (III)).18,59

In Fig. 3b, curves (I) and (II) correspond to the UV-Vis spectra of “AgNPs–PAni–Preyssler” nanocomposite which are nearly similar to the ones for Keggin-type, however, curve (III) differs by a strong absorption band at 415 nm and a weak band at ∼700 nm. Given that each heteropoly structure has a specific redox potential; these differences are important for the reduction of silver NPs where the redox potential should be large enough to reduce and stabilize AgNPs in the polymer matrix. In summary, Preyssler-type HPAs like Keggin could reduce and stabilize AgNPs in the nanocomposite in a one-pot process at the ambient temperature.

SEM method was employed to investigate the morphology and size of AgNPs dispersed in both synthesized “AgNPs–PAni–Keggin” (Fig. 4a) and “AgNPs–PAni–Preyssler” (Fig. 4b) nanocomposites. SEM results exhibited highly crystalline, porous and irregular structure intermingled with small islands due to some agglomeration of HPW-doped polymer while very small light spots of AgNPs dispersed in the matrix. The irregular morphology of PAni occurs due to the intermolecular hydrogen bonding as well as the existence of folded PAni chains during the polymerization process.57 This property indicates that only a part of Keggin molecules dispersed on the surface of polymer and the rest crystallized on the surface of support (polymer matrix).60


image file: c8ra09029g-f4.tif
Fig. 4 SEM images of (a) “AgNPs–PAni–Keggin” nanocomposite, and (b) “AgNPs–PAni–Preyssler” nanocomposite.

In Fig. 5, a clear view of AgNPs dopped in PAni–HPW composites is seen through TEM images. Fig. 5(a and b) for “AgNPs–PAni–Keggin” nanocomposite and Fig. 5(c and d) for “AgNPs–PAni–Preyssler” nanocomposite, respectively, exhibit spherical AgNPs dispersed and stabilized in the “PAni–Keggin” and “PAni–Preyssler” nanocomposite matrixes. TEM micrographs clearly showed the matrix of ashy PAni background with individual intense grayish AgNPs with predominant spherical shape surrounded by polymer support, implying the successful synthesis of AgNPs embedded in PAni. Dispersed and stabilized spherical AgNPs are clearly seen in the TEM images of “PAni–Keggin” and “PAni–Preyssler” nanocomposite matrixes without the common agglomeration issue which unfavorably occurs in AgNPs products.18 From TEM results, the size range of NPs in “AgNPs–PAni–Preyssler” nanocomposite is estimated to be smaller than the size of NPs in “AgNPs–PAni–Keggin” nanocomposite. Thus, it can be concluded that the size of NPs was affected by the type of HPA because different HPAs had a specific redox potential and this controlled the size of NPs. As the Preyssler had the highest activity among HPAs (mentioned in Introduction), a faster reduction occurred, which resulted in smaller and more uniform NPs.61 The dark highlighted blue circles in Fig. 5 show the impurity contents of AgNO3 or tungsten oxides during the oxidative polymerization of aniline (appeared in XRD results among AgNPs signals).


image file: c8ra09029g-f5.tif
Fig. 5 TEM images of (a and b) “AgNPs–PAni–Keggin” nanocomposite, and (c and d) “AgNPs–PAni–Preyssler” nanocomposite.

Generally, AgNPs tend to agglomerate due to small gauges and high surface/volume ratio of NPs.62,63 Electrostatic repulsion between Keggin and/or Preyssler molecules arose from their highly negatively charged units which facilitated the dispersion of HPWs on the positively charged backbone of PAni. Indeed, HPWs structure served as an anchor for the dispersion or trapping AgNPs. So, this alleviated the aggregation of AgNPs while silver ions were electronically introduced into the PAni–HPW network and firmly attached to the framework. The strong grafting interaction between the HPW–PAni and AgNPs was found from the nearly thin and transparent PAni matrix doped by the silver NPs where only a few AgNPs were scattered in the PAni matrix.63 As a consequence, the attached AgNPs may have ignorable crumpling together in the PAni network.63

AgNPs were decorated on both surface as well as the matrix of PAni.35 This also indicated that a certain amount of embedded AgNPs could efficiently prevent PAni from stacking during the reduction.63 Generally, despite all the studies in the field of AgNPs, their dynamic and complex surface chemistry have not been fully understood. The relationships and interactions in HPA-stabilized NPs with polymer matrix (which are newly emerging hybrid materials), various morphology and different reaction conditions, and wide range of particle size, make it a potential topic for comprehensive studies in the future.64

The XRD analysis was served to confirm the presence of AgNPs in both synthesized “AgNPs–PAni–Keggin” (Fig. 6a) and “AgNPs–PAni–Preyssler” (Fig. 6b) nanocomposites. As shown, four peaks were presented at 38.1°, 44.3°, 64.2° and 77.4° which were indexed to Bragg's reflections at (111), (200), (220), and (311) crystalline planes of face-centered cubic (fcc) symmetry of silver metal.65 The XRD analysis confirmed that AgNPs were successfully decorated into the crystalline polymer hybrid matrix. Further analysis of the XRD patterns confirmed two peaks at around 30.8° and 36.5°, related to the characteristic diffraction peaks of Keggin-type HPW. It is concluded from this fact that only a part of Keggin molecules dispersed on the polymer surface and the rest were crystallized on the surface of support,66 as appeared in the form of irregular structure intermingled with small islands confirmed by SEM. The peaks at around 32.1°, 32.7°, 33° and 55° were related to impurities in AgNO3, such as Ag2O, Ag2W2O7 (silver tungsten oxide), Ag4P2O7 (silver phosphate) (Table 5). As per the small size, AgNPs can easily participate in the polymerization reactions.63 From XRD data, it was evident that the “AgNPs–PAni–Preyssler” nanocomposite exhibited broader peaks for NPs than “AgNPs–PAni–Keggin” nanocomposite; this verifies the small crystalline size of AgNPs. For AgNPs with smaller size, the concentration of oxides became larger due to larger surface–volume ratio.63 This finding is in-line with the results verified by TEM and BET data on the small-size NPs embedded in the matrix of nanocomposites. It is worthwhile to mention that the size of AgNPs can be estimated from the Debye–Scherrer formula.60,65


image file: c8ra09029g-f6.tif
Fig. 6 XRD patterns of (a) “AgNPs–PAni–Keggin” nanocomposite, and (b) “AgNPs–PAni–Preyssler” nanocomposite.
Table 5 XRD peak assignment of AgNPs in “AgNPs–PAni–Keggin” and “AgNPs–PAni–Preyssler” nanocomposites
Peak assignment (2 theta) XRD peaks of nanocomposites Ref.
AgNPs 38.1°, 44.3°, 64.2°, 77.4° 53
Keggin structure 30.8°, 36.5° 51
Preyssler structure 33.7° 54
Ag2O 32.1° 51
Ag2W2O7 32.7° 51
Ag4P2O7 33°, 55° 51


The nitrogen adsorption/desorption isotherms of “AgNPs–PAni–Keggin” and “AgNPs–PAni–Preyssler” nanocomposites are shown in Fig. 7a and b, respectively. As shown in both Fig. 7a and b, the N2 isotherm of the as-prepared nanocomposites showed type III adsorption isotherms. The hysteresis loop with a H3 type is observed for non-rigid aggregates of plate-like particles (slit-shaped pores);67,68 in agreement with the SEM data. Besides, there was an additional adsorption step inflection occurred (with slight slope) at relative pressure range (p/p0) of 0.4–0.6. The meso-pores and step inflection with sharp uptake is observed at relative pressure (p/p0) of 0.8–1 which was the indication of the presence of textural macro-pores in both samples,46 identical with the macro-porous structures observed in SEM. The meso-pore size distribution curves calculated by BJH method are shown in Fig. 7a and b (inset), respectively. Obviously, the samples displayed broad pore size distributions ranging from 1.26 to 18.96 nm for “AgNPs–PAni–Keggin” and 1.25 to 19.95 nm for “AgNPs–PAni–Preyssler” nanocomposites (Table 6). The results of physical characterizations showed that micro-porous, meso-porous and macro-pores coexisted in the samples. Micro-pores were more significant (BJH isotherm) as they had high surface area. Both composites exhibited a broad distribution of micro/meso-pores, 12–189 Å for “AgNPs–PAni–Keggin” nanocomposite (Fig. 7a) and 12–199 Å for “AgNPs–PAni–Preyssler” nanocomposite (Fig. 7b). Here, the average pore diameters were determined as ∼2.244 nm for “AgNPs–PAni–Keggin” nanocomposite and ∼2.235 nm for “AgNPs–PAni–Preyssler” nanocomposite, nearly similar average pore size. On the other hand, pores with similar diameters in both nanocomposites were mainly in the range of <10 nm. Furthermore, the Brunauer–Emmett–Teller (BET) surface areas were found as 38.426 m2 g−1 for the “AgNPs–PAni–Keggin” nanocomposite and 29.977 m2 g−1 for “AgNPs–PAni–Preyssler” nanocomposites (Table 6).


image file: c8ra09029g-f7.tif
Fig. 7 N2 adsorption/desorption isotherms of (a) “AgNPs–PAni–Keggin” nanocomposite, and (b) “AgNPs–PAni–Preyssler” nanocomposite, along with the inset figure of BJH pore size distribution.
Table 6 Parametric results from BET analysis for “AgNPs–PAni–Keggin” and “AgNPs–PAni–Preyssler” nanocomposites
N2 adsorption/desorption “AgNPs–PAni–Keggin” nanocomposite “AgNPs–PAni–Preyssler” nanocomposite
BET surface area 38.426 (m2 g−1) 29.977 (m2 g−1)
BJH pore size distribution 1.26–18.96 (nm) 1.25–19.95 (nm)
dBJH total pore volume 0.176 (cm3 g−1) 0.145 (cm3 g−1)
MP total hole volume 0.434 (cm3 g−1) 0.543 (cm3 g−1)
Average pore diameter 2.244 (nm) 2.235 (nm)


4. Conclusion

A new method was introduced for the synthesis of two novel “AgNPs–PAni–Keggin” and “AgNPs–PAni–Preyssler” conductive nanocomposites through a low-cost, facile, one-pot, environmentally friendly and simultaneous in situ oxidative polymerization protocol at room temperature by using green materials; Keggin and Preyssler-type phosphotungstate. This is the first report that introduces both heteropolytungstates (Keggin and Preyssler-type) as dopants for acid protonating species and oxidative polymerization of aniline monomers. High crystallinity of matrixes was confirmed by XRD and SEM characterizations while TEM analysis showed significantly avoiding the common agglomeration issue in AgNPs products. IR results confirmed the existence of HPW as dopant anions that facilitated the stabilization, reduction and distribution of spherical AgNPs in the PAni matrix. BET characterization exhibited highly porous structures for both nanocomposites with the broad distribution of meso-pores with average pore diameters of ∼2.244 nm for “AgNPs–PAni–Keggin” and ∼2.235 nm for “AgNPs–PAni–Preyssler” nanocomposites. The highly protonated degree of PAni with HPW dopants can result in elevated electrical conductivity and flexibility of PAni containing hybrid materials, which can be useful for hydrogen fuel cells, electrodes and catalyses applications.

Conflicts of interest

There are no conflicts of interest to declare.

Acknowledgements

The Australian College of Kuwait for funding no. IRC-2017-18-SOE-ME-PR01 and PR02 is acknowledged. Special thanks go to Mr Mohammad Akbar Rahimi for his great support for this project.

References

  1. A. J. Heeger, Chem. Soc. Rev., 2010, 39, 2354–2371 RSC.
  2. A. J. Heeger, Angew. Chem., Int. Ed., 2001, 40, 2591–2611 CrossRef CAS PubMed.
  3. Y. Zhao, L. Cao, L. Li, W. Cheng, L. Xu, X. Ping, L. Pan and Y. Shi, Sensors, 2016, 16, 1787 CrossRef PubMed.
  4. R. Zhang, K.-s. Moon, W. Lin and C. Wong, J. Mater. Chem., 2010, 20, 2018–2023 RSC.
  5. M. Naseri, L. Fotouhi and A. Ehsani, The Chemical Record, 2018 Search PubMed.
  6. F. Xin and L. Li, Composites, Part A, 2011, 42, 961–967 CrossRef.
  7. C. Zhan, G. Yu, Y. Lu, L. Wang, E. Wujcik and S. Wei, J. Mater. Chem. C, 2017, 5, 1569–1585 RSC.
  8. Y. Zhang, B. Lin, Y. Sun, P. Han, J. Wang, X. Ding, X. Zhang and H. Yang, Electrochim. Acta, 2016, 188, 490–498 CrossRef CAS.
  9. A. Babakhanian, S. Kaki, M. Ahmadi, H. Ehzari and A. Pashabadi, Biosens. Bioelectron., 2014, 60, 185–190 CrossRef CAS PubMed.
  10. K. Dutta, S. Das, D. Rana and P. P. Kundu, Polym. Rev., 2015, 55, 1–56 CrossRef CAS.
  11. A. Muñoz-Bonilla, J. Sánchez-Marcos and P. Herrasti, in Conducting Polymer Hybrids, Springer, 2017, pp. 45–80 Search PubMed.
  12. A. Kumar, L. K. Jangir, Y. Kumari, M. Kumar, V. Kumar and K. Awasthi, J. Appl. Polym. Sci., 2016, 133, 44091 CrossRef.
  13. A. Kumar, V. Kumar and K. Awasthi, Polym.-Plast. Technol. Eng., 2018, 57, 70–97 CrossRef CAS.
  14. S. B. Teli, S. Molina, E. G. Calvo, A. E. Lozano and J. de Abajo, Desalination, 2012, 299, 113–122 CrossRef CAS.
  15. D. Jeon, N. Kim, S. Bae, Y. Han and J. Ryu, ACS Appl. Mater. Interfaces, 2018, 10, 8036–8044 CrossRef CAS PubMed.
  16. A. Khan, A. M. Asiri, M. A. Rub, N. Azum, A. A. P. Khan, S. B. Khan, M. M. Rahman and I. Khan, Composites Part B, 2013, 45, 1486–1492 CrossRef CAS.
  17. A. Khan, A. A. P. Khan, A. M. Asiri, V. Gupta and M. Rathore, J. Mol. Liq., 2016, 216, 646–653 CrossRef CAS.
  18. P. Kishore, B. Viswanathan and T. Varadarajan, Nanoscale Res. Lett., 2008, 3, 14 CrossRef CAS.
  19. Q. Meng, K. Cai, Y. Chen and L. Chen, Nano Energy, 2017, 36, 268–285 CrossRef CAS.
  20. R. Li, C. He, L. Cheng, G. Lin, G. Wang, D. Shi, R. K.-Y. Li and Y. Yang, Composites Part B, 2017, 121, 75–82 CrossRef CAS.
  21. S. Bhadra, D. Khastgir, N. K. Singha and J. H. Lee, Prog. Polym. Sci., 2009, 34, 783–810 CrossRef CAS.
  22. C. Dhand, M. Das, M. Datta and B. Malhotra, Biosens. Bioelectron., 2011, 26, 2811–2821 CrossRef CAS PubMed.
  23. H. Zhong, R. Yuan, Y. Chai, W. Li, X. Zhong and Y. Zhang, Talanta, 2011, 85, 104–111 CrossRef CAS PubMed.
  24. K.-H. Sun, Z. Liu, C. Liu, T. Yu, T. Shang, C. Huang, M. Zhou, C. Liu, F. Ran and Y. Li, Sci. Rep., 2016, 6, 23931 CrossRef CAS PubMed.
  25. A. A. Ensafi, E. Heydari-Soureshjani, M. Jafari-Asl and B. Rezaei, Carbon, 2016, 99, 398–406 CrossRef CAS.
  26. Z. Bai, C. Zhou, H. Xu, G. Wang, H. Pang and H. Ma, Sens. Actuators, B, 2017, 243, 361–371 CrossRef CAS.
  27. M. J. Martínez-Morlanes, A. Martos, A. Várez and B. Levenfeld, J. Membr. Sci., 2015, 492, 371–379 CrossRef.
  28. D. Zhu, H. Ma, H. Pang, L. Tan, J. Jiao and T. Chen, Electrochim. Acta, 2018, 266, 54–65 CrossRef CAS.
  29. C. Zhou, S. Li, W. Zhu, H. Pang and H. Ma, Electrochim. Acta, 2013, 113, 454–463 CrossRef CAS.
  30. S. Guo, L. Xu, B. Xu, Z. Sun and L. Wang, Analyst, 2015, 140, 820–826 RSC.
  31. D. J. Kim, B. M. Lee and S. Y. Nam, Thin Solid Films, 2013, 546, 431–435 CrossRef CAS.
  32. U. Thanganathan, J. Membr. Sci., 2016, 517, 100–110 CrossRef CAS.
  33. A. Kausar and M. Siddiq, Am. J. Polym. Sci. Eng., 2015, 3, 172–182 Search PubMed.
  34. A. Khan, A. A. P. Khan, A. M. Asiri and M. A. Rub, PLoS One, 2014, 9, e96897 CrossRef PubMed.
  35. J. Zuo, Z. Zhang, J. Jiao, H. Pang, D. Zhang and H. Ma, Sens. Actuators, B, 2016, 236, 418–424 CrossRef CAS.
  36. J. Hu, X. Wu, Q. Zhang, M. Gao, H. Qiu, K. Huang, S. Feng, T. Wang, Y. Yang and Z. Liu, Langmuir, 2018, 34, 2685–2691 CrossRef CAS PubMed.
  37. L. Zhang, Y. Yang, M. A. Ziaee, K. Lu and R. Wang, ACS Appl. Mater. Interfaces, 2018, 10, 9460–9467 CrossRef CAS PubMed.
  38. S. Zoladek, I. A. Rutkowska, M. Blicharska, K. Miecznikowski, W. Ozimek, J. Orlowska, E. Negro, V. Di Noto and P. J. Kulesza, Electrochim. Acta, 2017, 233, 113–122 CrossRef CAS.
  39. S. S. Hassan, Y. Liu, A. R. Solangi, A. M. Bond and J. Zhang, Anal. Chim. Acta, 2013, 803, 41–46 CrossRef CAS PubMed.
  40. C. Lin, T. Haolin and P. Mu, Int. J. Hydrogen Energy, 2012, 37, 4694–4698 CrossRef.
  41. P. Sayadi, S. Rowshanzamir and M. J. Parnian, Energy, 2016, 94, 292–303 CrossRef CAS.
  42. A. A. Khan and U. Baig, Sens. Actuators, B, 2013, 177, 1089–1097 CrossRef CAS.
  43. M. Amirinejad, S. S. Madaeni, K.-S. Lee, U. Ko, E. Rafiee and J.-S. Lee, Electrochim. Acta, 2012, 62, 227–233 CrossRef CAS.
  44. X. Fan, W. Yuan, D. H. Zhang and C. M. Li, ACS Appl. Energy Mater., 2018, 1, 411–420 CrossRef CAS.
  45. H. Li, X. Zhang, H. Pang, C. Huang and J. Chen, J. Solid State Electrochem., 2010, 14, 2267–2274 CrossRef CAS.
  46. Y. Du, P. Yang, S. Zhou, J. Li, X. Du and J. Lei, Mater. Res. Bull., 2018, 97, 42–48 CrossRef CAS.
  47. G. Li, X. Yan, P. Mei, Y. Jiang, Y. Zhang, F. Deng, Y. Xiong and H. Tang, J. Mater. Sci.: Mater. Electron., 2018, 1–7 Search PubMed.
  48. N. Thakur, S. Das Adhikary, M. Kumar, D. Mehta, A. K. Padhan, D. Mandal and T. C. Nagaiah, ACS Omega, 2018, 3, 2966–2973 CrossRef CAS PubMed.
  49. A. Hayashi, T. Haioka, K. Takahashi, B. S. Bassil, U. Kortz, T. Sano and M. Sadakane, Z. Anorg. Allg. Chem., 2015, 641, 2670–2676 CrossRef CAS.
  50. A. Hayashi, M. N. K. Wihadi, H. Ota, X. López, K. Ichihashi, S. Nishihara, K. Inoue, N. Tsunoji, T. Sano and M. Sadakane, ACS Omega, 2018, 3, 2363–2373 CrossRef CAS.
  51. I. Sapurina and J. Stejskal, Polym. Int., 2008, 57, 1295–1325 CrossRef CAS.
  52. J. Lu, K.-S. Moon, J. Xu and C. Wong, J. Mater. Chem., 2006, 16, 1543–1548 RSC.
  53. R. Pasricha, S. Gupta and A. K. Srivastava, Small, 2009, 5, 2253–2259 CrossRef CAS PubMed.
  54. C. Sui, C. Li, X. Guo, T. Cheng, Y. Gao, G. Zhou, J. Gong and J. Du, Appl. Surf. Sci., 2012, 258, 7105–7111 CrossRef CAS.
  55. A. Manivel, R. Sivakumar, S. Anandan and M. Ashokkumar, Electrocatalysis, 2012, 3, 22–29 CrossRef CAS.
  56. A. Proń, Synth. Met., 1992, 46, 277–283 CrossRef.
  57. A. Kumar, V. Kumar, M. Kumar and K. Awasthi, Polymer Composites, 2017 Search PubMed.
  58. A. Kumar, V. Kumar, P. Sain, M. Kumar and K. Awasthi, Int. J. Hydrogen Energy, 2018, 43, 21715–21723 CrossRef CAS.
  59. K. Awazu, M. Fujimaki, C. Rockstuhl, J. Tominaga, H. Murakami, Y. Ohki, N. Yoshida and T. Watanabe, J. Am. Chem. Soc., 2008, 130, 1676–1680 CrossRef CAS PubMed.
  60. G. Zhou, T. Cheng, W. Li, Y. Bi and K. Zhen, React. Kinet. Catal. Lett., 2003, 79, 295–302 CrossRef CAS.
  61. A. Ayati, A. Ahmadpour, F. F. Bamoharram and M. M. Heravi, Synth. React. Inorg., Met.-Org., Nano-Met. Chem., 2012, 42, 1309–1314 CrossRef CAS.
  62. S. Mohammadi, S. Pourseyedi and A. Amini, J. Environ. Chem. Eng., 2016, 4, 2023–2032 CrossRef CAS.
  63. J. Zeng, X. Tian, J. Song, Z. Wei, S. Harrington, Y. Yao, L. Ma and Y. Ma, J. Mater. Sci.: Mater. Electron., 2016, 27, 3540–3548 CrossRef CAS.
  64. D. K. Hazra and R. Chatterjee, J. Mol. Struct., 2013, 1045, 139–144 CrossRef CAS.
  65. T. Theivasanthi and M. Alagar, arXiv:1111.0260, 2011.
  66. D. M. Ruiz, G. P. Romanelli, P. G. Vázquez and J. C. Autino, Appl. Catal., A, 2010, 374, 110–119 CrossRef CAS.
  67. K. S. Sing, Pure Appl. Chem., 1985, 57, 603–619 CAS.
  68. U. Holzwarth and N. Gibson, Nat. Nanotechnol., 2011, 6, 534 CrossRef CAS PubMed.

Footnote

These authors had equal roles in this study.

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