Hasan B. Balkhoyora,
Mohammed M. Rahman*ab and
Abdullah M. Asiriab
aChemistry Department, King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia. E-mail: mmrahman@kau.edu.sa; mmrahmanh@gmail.com; Fax: +966-02-6952292; Tel: +966-59-6421830
bCenter of Excellence for Advanced Materials Research (CEAMR), King Abdulaziz University, P.O. Box 80203, Jeddah 21589, Saudi Arabia
First published on 6th June 2016
Various Ce-doped ZnO nanostructures (Ce/ZnO NSs) were prepared by a facile wet chemical method using reducing agents in alkaline medium. The Ce/ZnO NSs were characterized by UV/vis, FT-IR, field emission scanning electron microscopy (FESEM), energy-dispersive X-ray spectroscopy (XEDS), X-ray photoelectron spectroscopy (XPS), and X-ray powder diffraction (XRD). The Ce/ZnO NSs were deposited onto flat glassy carbon electrode (GCE) with conducting Nafion binders to produce a sensor that has a fast response towards selective 3-methoxyphenol (3MP). Characteristics including higher sensitivity, lower detection limit, better reliability, good reproducibility, ease of integration, long-term stability, high selectivity, and enhanced electrochemical performance were investigated in detail at room conditions. The calibration plot is linear (r2 = 0.9879) over a large concentration range (0.9 nM to 0.9 mM). The sensitivity and detection limit was calculated as ∼94.937 μA cm−2 μM−1 and 11.5 ± 0.2 pM (at a signal-to-noise-ratio [SNR] of 3), respectively. Finally, the efficiency of the proposed chemisensor can be applied and effectively utilized for the detection of various toxic chemical compounds in the environment with acceptable and reasonable results.
Metal oxide nanomaterials have attracted much attention because of their exceptional properties and potential applications in every area of science and technology.9 The easy synthetic route of doped material is probably self-aggregation, in which ordered aggregates are formed by a spontaneous chemical process in the presence of reactive reactant precursors.10 However, it is still a big challenge to develop a simple and reliable method for a low-dimensional doped metal oxide with designed chemical components and controlled morphology using inorganic transition doping materials, which strongly affect the properties of the host nanomaterials.11 Recently, nano-sized nanostructures of paramagnetic iron oxides coupled with various materials have been investigated extensively due to their wide applications in nano-fields such as ferro-fluids,12 magneto-caloric refrigeration,13 biotechnology and biomedical field,14 in controlled drug delivery systems, as contrast agent of magnetic resonance imaging, and in tissue repair and the detoxification of biological fluids.15 It also has been extensively studied in diverse fields including catalysis,7 environmental protection,16 magnetic storage devices,17 clinical diagnosis, and treatment.18 Nanomaterials may also be utilized in different technological fields, refrigeration systems, medical imaging, drug targeting, biological applications, and electrocatalysis.19 Since the reduction–oxidation reactions are activated by the active surface area, reducing the crystal dimension and enhancing the surface area of the sensing materials provide optional approaches to improving the responses of nanoparticles.20 ZnO is a multifunctional nanomaterial because of its unique physical and chemical properties that reflect its numerous chemical and physical applications. Industries such as rubber, pharmaceutics, cosmetics, textile, electronic, and electro-technology use ZnO in many of their products, beside its use in electrocatalysis and photocatalysis.21 ZnO doped with different metals and nonmetals show enhanced photocatalytic activity; the band-gap energy of ZnO nanostructure is ∼3.37 eV, which can be lowered by maximizing the valence band, minimizing the conduction band, or introducing mid-band-gap energy levels.22 Besides that, doping also results in high surface-to-volume ratio, crystal defects, and the initiation of charge carrier traps.23 CeO2 nanoparticles with high ionic conductivity, negligible cytotoxicity, and good redox activity extend ZnO's application in many ways.24
Different types of nanoparticles and metallic colloids have been used to improve patient acquiescence and therapeutic efficacy of applicable medicines in the medical field. Ferro-fluids are stable dispersions of magnetic iron-oxide nanoparticles in water and have been studied in biomedical sciences as efficient devices for in vitro diagnosis, cell separation, immunoassays, and nucleic acid concentration.25 In chemistry, iron oxide nanoparticles have been used in NO reduction,26 as adsorbents for heavy metals,27 as pigments in cosmetic powders,28 as anodes in lithium-ion batteries,29 in the detection of hydrogen peroxide,30 in the polymer coating of supra-magnetic nanoparticles,31 in magnetic resonance imaging,32 in biomedical applications,33 as imaging agents,34 in photocatalysis,35 for removing inorganic and organic pollutants,36 in glycerol hydrogenolysis,37 in the hydrogenation of nitrobenzene,38 in high-performance supercapacitors,39 in catalytic oxidation,40 in water treatment,41 in the separation of acid dye,42 in antibody functionalization,43 in biosensor applications,44 in the hybridization of nanotube,45 in oil spill removal,46 in bio-distribution studies,47 etc. Substituted and unsubstituted phenols are common byproducts of the industrial process and are highly toxic. They are frequent contaminants in food and in freshwater and wastewater48 environments. 3MP is toxic chemical that greatly effects the environment and health. Due to the many demerits of phenols, it is very urgent to develop an appropriate analytical method that is reliable, robust, cheap, and effective for the accurate quantification and sensitive detection of 3MP. Various sensing techniques have been already introduced and published in the scientific reports to detect phenolic compounds by electrochemical methods, HPLC, and spectrometry. Among several detection methods, the electrochemical current vs. voltage (I–V) technique is cheap, portable, fast, robust, and easy to handle. Therefore, numerous chemically modified electrodes based on different nanostructured materials, semiconductor-doped nanomaterials, transition metal oxides, and electrocatalytic moieties (electron-mediator species) have been developed for the detection of 3MP.49
In this study, Ce/ZnO nanostructures were synthesized by a wet chemical process using different ratios by volume, which yielded a various structures and morphologies of the doped transition metal. The Ce/ZnO NSs allow very sensitive recognition and transduction during the chemical interaction, thus changing the electrochemical properties. Finally, Ce/ZnO NSs were fabricated at a suitable volume-to-volume ratio and applied onto polished GCE surface to make a simple, reliable, and efficient chemical sensor for 3MP at room conditions. To the best of our knowledge, this is the first report of the highly sensitive detection of 3MP with Ce/ZnO NSs using the simple and reliable I–V method with a short response time.
NaOH(s) → Na(aq)+ + OH(aq)− | (i) |
Ce2(SO4)3(s) → 2Ce(aq)3+ + 3SO4(aq)2− | (ii) |
ZnCl2(s) → Zn(aq)2+ + 2Cl(aq)− | (iii) |
8OH(aq)− + 2Ce(aq)3+ + Zn(aq)2+ → Zn(OH)2(aq)↓ + 2Ce(OH)3(aq)↓ | (iv) |
Zn(OH)2(aq) + Ce(OH)3(aq) → Ce/ZnO(s)↓ + H2O(l) | (v) |
In Ce/ZnO NSs growth method, initial ZnO and CeO2 nucleus growth takes place by self- and mutual-aggregation when two individual reactant precursors [Ce2(SO4)3 and ZnCl2] are mixed by vigorous magnetic stirring at lower temperature. Then, nanocrystals of reactant precursors [Zn(OH)2 and Ce(OH)3] reaggregated and formed aggregated ZnO and CeO2 nanocrystals by releasing water molecules into the reaction medium via the Ostwald ripening method at a higher temperature. Nanocrystals are crystallized and re-aggregated (ZnO and CeO2), with each counter-heterogeneous part in the presence of disperse reactant precursors through van der Waals forces. Finally, Ce/ZnO nanostructure morphology is re-formed at the calcination temperature, as presented in Scheme 1.
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Scheme 1 Schematic representation of the growth mechanism of Ce/ZnO nanostructures by a wet chemical process. |
In UV/visible principle, the outer electrons of the atom absorb radiant energy and then shift to the higher energy levels. The spectrum including the band-gap energy of the metal oxide is achieved due to optical absorption. The UV/vis spectra of the Ce/ZnO NSs was recorded in the visible range. Absorption spectrum in the visible range between 300.0 and 800.0 nm for Ce/ZnO NSs is presented in Fig. 2a, which shows a broad absorption band at 375.0 nm for the selective Ce/ZnO (2:
1) ratio. This absorption coefficient value is related to the optical band-gap energy in accordance with the expression α = (hν − Eg)1/2, where h is Planck's constant and ν is the frequency of incident photons. The intercept on the energy axis is obtained by extrapolating the linear portion of Tauc's plot (αhν)2 vs. hν, as shown in Fig. 2b. The band-gap energy (Eg) of the doped Ce/ZnO (2 : 1 ) is ∼2.85 eV. The band-gap energy is calculated at a lower magnitude for Ce/ZnO NSs compared to only zinc oxide or cerium oxide.51
XPS is a quantitative spectroscopic technique used to indicate the chemical nature of the elements existing in a particular material. XPS spectra are recorded by irradiating the doped nanomaterial with an X-ray beam, and kinetic energy, including the electron number of the doped sample might be determined consecutively. Here, the XPS spectra for the binding energy of Ce/ZnO NSs are confirmed in the presence of CeO2, as presented in Fig. 3a. The blank ZnO and CeO2 peaks appear at 882.4 eV for Ce3d [Fig. 3b], 1022.6 eV for Zn2p [Fig. 3c], and 532 eV and 537 eV for O1s peaks in the two undoped samples [Fig. 3d]. The shifting of binding energy could be a result of the Ce doping at different ratios, where the values are obtained in good agreement with the literature.52,53 Table 1 summarizes the binding energy and band-gap energy values for various compositions of Ce/ZnO, ZnO, and CeO2.
Sample | Binding energy (eV) | Ebg (eV) | |||
---|---|---|---|---|---|
Zn2p | O1s | Ce3d | |||
ZnO | 1022.6 | 532 | — | 3.25 | |
Ce![]() ![]() |
1![]() ![]() |
1022.3 | 532 | 883.7 | 3.0 |
2![]() ![]() |
1022.2 | 533.2 | 882.8 | 2.85 | |
3![]() ![]() |
1022.0 | 531 | 883.2 | 2.96 | |
4![]() ![]() |
1022.2 | 532 | 883.6 | 2.96 | |
CeO2 | — | 537 | 882.4 | 3.1 |
X-ray powder diffraction was employed to measure the Ce/ZnO nanomaterial phases by comparing with the standard value of lattice parameters, crystal structures, and crystallinity in the Joint Committee on Powder Diffraction Standards (JCPDS) of ZnO and CeO2. XRD spectra in Fig. 4 reveal that all of the blank ZnO peaks (*) match the Bragg reflections of the standard hexagonal phase structure of space group P63mc (186), a = b = 3.249 Å, c = 5.207 Å, (wurtzite, JCSPD 36-1451), for the diffraction planes at (100), (002), (101), (102), (110), (103), (200), (112), (201), (004), and (202). The blank cerium oxide match CeO2 peaks (#) for [JCPDS No. 65-5923] face-centered cubic structure at reflections planes of (111), (200), (220), (311), (222), (400), (331), and (422). In comparison of the two blank pattern with the Ce/ZnO spectra, it shows the peaks (+) which indicate Ce-doping with ZnO and change of intensities in some peaks. Although the XRD profile of the doping samples specially (2:
1, 3
:
1, 4
:
1) resemble the CeO2 which gives indication that the Zn doped in CeO2 structure, this might be because of large ionic radii of Ce and difference of oxidation numbers.51,54,55
FESEM is one of the prominent methods for studying the nanostructure morphology of nanomaterials. The morphology of the prepared Ce/ZnO NSs were measured using FESEM-coupled XEDS. Fig. 5a and b shows typical shapes of Ce/ZnO nanostructures for 2:
1 ratio sample at low and high magnification.
Energy-dispersive X-ray spectroscopy (EDS) gives the quantitative presence of all elements in the prepared doped Ce/ZnO nanomaterial samples. Fig. 6a and b for Ce/ZnO indicates the presence of oxygen (31.21% wt), zinc (9.58% wt), and cerium (59.21% wt).
Fig. 8a displays the current responses for bare GCE and for that with Ce/ZnO NS coating on the working electrode surface. The current response of the bare GCE was greater than that of the one coated with doped nanomaterials. The response of the resultant cell current (Fig. 8b) is shown for the Ce/ZnO (1:
1) NSs implemented for the detection of a group of various analytes to study the selectivity in the presence of different analytes. This study shows the suitability of using Ce/ZnO (1
:
1) NSs as a good selective sensor towards 3MP compared to all other chemicals, even phenolic derivatives.
A set of Ce/ZnO nanostructure samples was prepared with different ratios by volume as 1:
1, 2
:
1, 3
:
1, 4
:
1. The electrodes fabricated with these sample were tested with 3MP to study the effect of doping ratios, where the highest current response for 3MP was found to be Ce/ZnO with 2
:
1 ratio (Fig. 9a). Then, the fabricated electrode was used for concentration and repeatability studies for measuring and calculating the other sensor parameters. The concentration of 3MP was varied from 0.09 mM to 0.09 nM by adding deionized water at various proportions. A significant increase in the current value with applied potential was clearly demonstrated for the fabrication of thin NS film on flat GCE, as shown in Fig. 9c. It is observed that the current of NSs/GCE as a function of 3MP concentration at room conditions gradually increases from a low to high value of current with the increasing concentration of the target analyte. Fig. 9d shows the repeatability (R1 to R7) testing at 9.0 μM with a good consistent profile for the total run-set. A calibration curve is plotted (at +1.2 V) from the electrochemical responses in various 3MP concentrations and presented in Fig. 9e. The sensitivity and detection limit was calculated from the calibration curve based on the active surface area of fabricated GCE electrodes. The calibration plot is linear (r2 = 0.9879) over the 0.09 nM to 0.09 mM 3MP concentration range. The sensitivity and detection limit is found as 94.937 μA cm−2 μM−2 and ∼11.5 ± 0.2 pM (based on signal-to-noise-ratio of 3), respectively. The fabricated 3MP sensor also exhibits good sensitivity, a good detection range of 0.9 nM to 9.0 mM, and long-term stability as well as enhanced electrochemical response towards the target analyte. The response time was approximately 10.0 s for the Ce/ZnO NSs-coated GCE to achieve saturated steady-state current. The prominent sensitivity of the 3MP sensor could be attributed to good absorption (porous surfaces fabricated with conducting binders), adsorption ability (large surface area), and high catalytic activity. The sensitivity of Ce/ZnO NSs affords good electron communication features, which enhances the direct electron transfer between the active sites of NSs and sensor electrode surfaces. The modified thin NSs/GCE has a better reliability as well as stability compared to those reported in literature.58–60
3MP is mostly converted to benzoquinone (BQ) and methanol in the presence of doped semiconductor nanomaterials. Here, oxygen (dissolved) is chemisorbed onto the Ce/ZnO/GCE NSs surfaces, while the NS-coated film electrode is immersed into the PBS system. During chemisorption, the dissolved oxygen is converted to ionic species (such as O2− and O−) by gaining electrons from the conduction band of aggregated Ce/ZnO NSs, which improve and enhance the current responses against potential during the I–V measurement at room conditions61,62 (eqn (6) & (7)). The aqueous 3MP sensing mechanism of Ce/ZnO/GCE NS sensors is presented here based on the semiconductor oxides, due to oxidation or reduction of the semiconductor oxide itself, according to the dissolved O2 in bulk solution, the surface/air interface, and the surrounding atmosphere.
e−(Ce/ZnO/GCE) + O2 → O2− | (6) |
e−(Ce/ZnO/GCE) + O2− → 2O− | (7) |
These reactions take place in the bulk solution, air/liquid interface, or surrounding air due to the low carrier concentration, which increases the resistance. 3MP sensitivity toward Ce/ZnO/GCE NSs (MOx) could be attributed to the high oxygen deficiency and defect density, leads to increased oxygen adsorption. The larger the amount of oxygen adsorbed on the surface, the larger the oxidizing capability and the faster the oxidation of 3MP would be. The reactivity of 3MP would have been very large as compared to other chemicals with the surface under the same condition. 3MP reacts with the adsorbed O2 on the doped surface of the film, liberating free electrons in the conduction band as could be expressed through the following reactions:
MOx + 3MP + O2− → M(3MP(OX)) + H+ + 2e− | (8) |
M(3MP(OX)) + H2O → BQ + CH3OH + H+ | (9) |
These reactions correspond to oxidation of the reducing carriers. These processes are increased with the carrier concentration of analyte and consequently reduce the resistance on contact with reducing liquids. At room conditions, the contact of Ce/ZnO NS surface with reducing liquid/analytes results in a surface-mediated chemical process. The elimination of ionosorbed oxygen enhances the electron density as well as the surface conductance of the Ce/ZnO NSs/GCE film. The reducing analyte 3MP donates electrons to Ce/ZnO NSs/GCE surface. Therefore, resistance decreases and hence, conductance increases. This causes the 3MP analyte response (current response) to increase with increasing potential (increasing the respective current), as proposed in Fig. 10. Thus, the produced electrons cause rapid enhancement in conductance of the large surface area of Ce/ZnO NSs. The Ce/ZnO NS eccentric regions dispersed on the surface would enhance the ability of the material to absorb more oxygen species, giving high resistance in ambient air.
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Fig. 10 Mechanism of Ce/ZnO/GCE NS chemical sensors at ambient conditions. (a) Before and (b and c) after injecting target 3MP analytes. |
The sensor response time was first set at 10 s for the Ce/ZnO/GCE NSs to reach saturated steady-state current. The higher sensitivity of the coated film could be attributed to the good absorption (porous surfaces fabricated with coating), adsorption ability, high catalytic activity, and good biocompatibility of the Ce/ZnO nanostructure materials. The estimated sensitivity of the fabricated sensor is relatively high for 3MP based on other composite or materials modified electrodes. Due to their large surface area, the nanomaterials provided a favorable nano-environment for the chemical detection with good quantity. The higher sensitivity of the Ce/ZnO/Nafion/GCE assembly provides better electron communication features, which improved the direct electron transfer between the active sites of Ce/ZnO NS materials and the GCE. The modified thin film has good stability due to high specific surface area, where the nanomaterials of Ce/ZnO NSs imparted a favorable environment for 3MP detection (by adsorption) with a large quantity. Ce/ZnO/GCE reveals several advantages for this approach in providing chemical-based sensors, encouraging the progress executed in this research. As for the doped nanomaterials, Ce/ZnO NS provides a path to a new generation of chemical sensors. Further research effort is required for the expansion of doped nanostructures in large-scale applications and to gain access to individual selective and sensitive chemical sensors. Reliable methods for fabricating, assembling and integrating the building blocks on sensitive chemical sensors need to be explored. Table 2 presents selected applications of nanocomposites or nanomaterials for sensing phenol compounds by electrochemical approaches.
Sensing layer | Analyte | Transduction | Performances | Ref. |
---|---|---|---|---|
MnO2/screen-printed sensor | Phenol | Voltammogram | Sensitivity: 0.123 mA μM−1 cm−2, DL: 0.64 μM, LDR: up to 716 μM | 63 |
SiO2/Nb2O5 sol–gel | Phenol | Potentiometry | Sensitivity: 3.2 nA dm3, DL: 0.5 μmol dm−3, LDR: 5–25 μmol dm−3 | 64 |
Ag2S QD/GC electrode | Phenol | Amperometry | Sensitivity: 0.0612 μA μM−1 cm−2, DL: 0.015 μM, LDR: 1 μM to 16 mM | 65 |
Graphene–polyaniline/GCE | Aminophenol | DPV | Sensitivity: 1.776042 μA μM−1 cm−2, DL: 0.065 μM, LDR: 0.2–20, 20–100 μM | 66 |
RGO/P-L-GSH/GCE | Aminophenol | Amperometry | Sensitivity: 0.0272 mA μM−1 cm−2, DL: 0.03 μM, LDR: 0.4–200 μM | 67 |
POAS–Ag/MWCNT/GCE | Methoxyphenol | I–V | Sensitivity: 3.829 μA μM−1 cm−2, DL: 0.36 nM, LDR: 0.4 nM to 40.0 mM | 49 |
Ce/ZnO NSs | 3-Methoxy phenol | I–V method | Sensitivity: 94.937 μA cm−2 μM−1, DL: 11.5 pM (at SNR of 3), LDR: 0.9 nM to 9.0 mM, linearity, r2 = 0.9879, response time: 10 s | This work |
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