Open Access Article
Ian Zammit
a,
Vincenzo Vaianob,
Giuseppina Iervolinob and
Luigi Rizzo
*a
aDepartment of Civil Engineering, University of Salerno, Via Giovanni Paolo II 132, 84084 Fisciano, SA, Italy. E-mail: l.rizzo@unisa.it; Fax: +39089969620; Tel: +39089969334
bDepartment of Industrial Engineering, University of Salerno, Via Giovanni Paolo II 132, 84084 Fisciano, SA, Italy
First published on 20th July 2018
Heterogeneous photocatalysis (HPC) is a subset of Advanced Oxidation Processes (AOPs) with potential future applications in water disinfection. Herein, a zinc oxide photocatalyst was doped with cerium at various atomic ratios ranging from 0 to 0.1 Ce
:
Zn. Keeping in mind that the application of HPC is often limited by its cost of use, a simple and easy to upscale method, that is the hydroxide induced hydrolysis of zinc nitrate in the presence of Ce3+ followed by calcination at 300 °C, was used to synthesise the catalysts. The catalysts have been characterized by different techniques such as X-ray diffraction (XRD), UV-vis diffuse reflectance (UV-vis DRS) and Raman spectroscopy. XRD results showed that Ce3+ ions were successfully incorporated into the ZnO lattice. UV-vis DRS spectra evidenced that Ce–ZnO samples present band-gap values of about 2.97 eV, lower than those of undoped ZnO (3.21 eV). These various photocatalysts, at 0.1 g L−1 in saline 0.85%, were used to inactivate Escherichia coli previously isolated from an urban wastewater treatment plant. Higher atomic ratios of Ce in the ZnO lattice, as confirmed by XRD and Raman spectroscopy, showed significant improvements to the inactivation rate; the resulting recommended optimum cerium loading of 0.04
:
1 Ce
:
Zn gave multiple orders of magnitude higher rate of inactivation after 60 min of treatment when compared to un-doped ZnO. This optimum loading of cerium was faster than the de facto literature standard TiO2-P25 tested under identical conditions.
In HPC, ROS are generated by the light induced generation of electron–hole pairs within the photocatalyst in the presence of water. Electron–hole pairs are only generated when the energy of the electromagnetic radiation absorbed by the semiconductor is of higher or equal energy than its band gap – the gap between the valence and conduction bands. Titanium dioxide is the most investigated photocatalyst partially due to its commercial availability and abundance but recently zinc oxide (ZnO) has gained traction over titanium dioxide due to the fact that it has the same advantages but is cheaper.20–25
Metal doping of semiconductors is a technique employed to change the photocatalytic properties of the material, such as the band gap, the recombination rate of electron–hole pairs and adsorption properties of the material, these in turn affect the generation of ROS and reaction kinetics.26,27
Doping of ZnO with cerium has been previously investigated in the development of sensors28–30 and coating fibers.31 More relevantly to the work herein, Ce doped ZnO was also investigated in the removal of chemical pollutants,32–36 showing promising results, at times better than titanium dioxide. However, to the best of our knowledge Ce doped ZnO has not been used for the inactivation of bacteria so far, and the promising results on chemical pollutants warrant research on bacterial inactivation. Additionally we test a wider range of cerium atom ratios in doping to evaluate possible improvements over the optimum of 0.01 previously tested against chemical compounds.37 Herein photocatalytic inactivation of an indigenous E. coli strain selected from the secondary effluent of an UWTP was investigated using Ce doped ZnO as the photocatalyst. The loading of cerium within ZnO was optimised with respect to its activity in inactivating the selected E. coli strain with the aim of improving the activity of the photocatalyst while maintaining low costs of production and a simple and easy to upscale method of synthesis. This work is part of an effort to develop a reactor using an easy to upscale optimised photocatalyst for the disinfection of wastewater allowing safe and economically feasible agricultural reuse.
| Zn(NO3)2·6H2O(aq.) + 2OH(aq.)− → Zn(OH)2(s) + 2NO3− | (1) |
| Zn(OH)2(s) + heat → ZnO(s) | (2) |
Seven doping levels of cerium in ZnO were also prepared using the same method. The only difference being that cerium(III) nitrate hexahydrate was dissolved and well homogenised with the zinc salt prior to co-precipitation on the addition of the base. The amount of cerium(III) nitrate hexahydrate used in the synthesis was in the range of 0.042 millimoles to 1.681 millimoles obtaining samples at different Ce
:
Zn molar ratio. In particular, the seven molar ratios of Ce
:
Zn prepared are 0.0025
:
1, 0.0050
:
1, 0.0100
:
1, 0.0150
:
1, 0.0400
:
1, 0.0700
:
1, 0.1000
:
1. Thus the range of Ce to Zn atom ratio ranged from nil, in the undoped, to 10%.
305
700°, 014.8
448
900°). Blue colonies were isolated on selective chromogenic agar (TBX). X-Gluc in TBX agar identifies β-glucuronidase activity in E. coli and results in blue coloured colonies. One of these colonies was isolated, cultivated in LB broth and a mother stock preserved in glycerol. The strain was also tested on a second chromogenic agar, the expected dark blue colouration was also observed here. The strain is hence presumed to be E. coli.
The selected E. coli strain was grown overnight in LB broth, centrifuged at 3000 rpm for 10 min and a suitable volume to reach 106 CFU mL−1 was suspended in 250 mL of sterile isotonic water. Separately 0.05 g of photocatalyst was sonicated for 15 min in 250 mL of isotonic water. The volumes were mixed under stirring and the initial bacterial density sampled. The stirred mixture was left for 60 min in the dark to establish an equilibrium of adsorption between bacteria and the catalyst. After 60 min of dark phase the reactor was exposed to the UVA radiation from the 125 W lamp pre-warmed for 20 min. The stirred mixture was then sampled after 15 min, 30 min, 60 min, 120 min, and 135 min. Additionally two control measurements were also carried out, these being bacterial inactivation due to UVA radiation damage only, labelled as UVA control and the inactivation of bacteria with the optimum catalyst loading in the dark, labelled as Dark Ce-400.
XRD spectra of the samples were analysed more accurately in the range 31–33° (Fig. 2). It is possible to observe that the position of the diffraction pattern associated to (1 0 0) plane shifted towards lower angle with increasing the Ce content, indicating that the lattice parameters of ZnO increased.41 This result can be explained considering that the radius of Ce3+ ion is much larger than that of Zn2+ (0.074 nm), so inducing a shift of diffraction peak and indicating that the Ce ions have been successfully incorporated into the ZnO lattice and substituted the Zn2+ sites.42
The successful doping with Ce and the formation of CeO2 was further confirmed by Raman spectroscopy (Fig. 3).
In particular, for the undoped ZnO and Ce-25, Ce-50, Ce-100 and Ce-150, it is possible to note the presence of the signals located at about 332, 379, and 437 cm−1 assigned to vibration modes of wurtzite phase of ZnO.43 Compared to undoped ZnO, the main Raman signal of the ZnO structure for Ce-400, Ce-700 and Ce-1000 samples was shifted from 437 to about 433 cm−1. This shift is due to stress phenomena induced by the lattice distortion of ZnO crystalline structure, in agreement with literature concerning Ce-doped ZnO.44,45 Moreover, in the Raman spectra of the same samples (Ce-400, Ce-700 and Ce-1000), the signal observed at about 456 cm−1 is originated from the Raman active mode characteristic of CeO2 fluorite-structured materials corresponding to the ceria Ce–O8 vibrational unit.46
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| Fig. 4 Control tests and E. coli photocatalytic inactivation for all the synthesised photocatalysts. | ||
UV-vis DRS spectra of undoped ZnO and Ce doped ZnO samples were used to calculate the energy band gap (Ebg) of the samples and the obtained values are reported in Table 1.
| Labelled as | Cerium content Ce : Zn at/at |
Cerium content as measured by XRF Ce : Zn at/at |
SSA (BET method), m2 g−1 | Ebg, eV |
|---|---|---|---|---|
| ZnO | No cerium | No cerium | 14 | 3.21 |
| Ce-25 | 0.0025 : 1 |
0.002 : 1 |
19 | 3.19 |
| Ce-50 | 0.0050 : 1 |
0.005 : 1 |
23 | 3.18 |
| Ce-100 | 0.0100 : 1 |
0.011 : 1 |
19 | 3.17 |
| Ce-150 | 0.0150 : 1 |
0.017 : 1 |
23 | 3.16 |
| Ce-400 | 0.0400 : 1 |
0.038 : 1 |
22 | 3.15 |
| Ce-700 | 0.0700 : 1 |
0.074 : 1 |
27 | 3.00 |
| Ce-1000 | 0.1000 : 1 |
0.140 : 1 |
28 | 2.97 |
| TiO2-P25 | N/A | N/A | 47 | 3.30 |
The decrease of Ebg from 3.21 eV of undoped ZnO to 2.97 eV of Ce-1000 sample can be ascribed to the formation of a shallow level inside the band gap, because of impurity atoms (Ce3+) introduced into the wurtzite ZnO crystalline structure.47 These results are in agreement with UV-vis absorption results previously described and with recent reports in literature.45
The specific surface areas (SSA) of all the investigated samples are also reported in Table 1. All the doped samples show a higher surface area than undoped ZnO (14 m2 g−1 cf. 28 m2 g−1 for ZnO and Ce-1000, respectively), in agreement with the scientific literature.41 The synthetic method used herein also produced higher SSA than that reported by Wang et al. using a similar method but involving temperature shifts.36 As for SSA with the Ce
:
Zn ratio, there is not a clear cut trend. The ZnO Ce-700 and ZnO Ce-1000 did produce a higher SSA but the lower atom ratios did not gradually give an increase. In all atom ratio doesn't seem to greatly impact the surface area.
The Ce
:
Zn molar ratio in the samples was determined by XRF analysis (Table 1). It is possible to observe that, in all cases, the measured Ce
:
Zn atomic ratio well fits the nominal values indicating a good yield of the doping process.
log10 decrease measured after 135 min. This excludes substantial bacterial cell inactivation due to any potential toxicity of the catalyst to the cells implying inactivation being due to photocatalytic oxidative damage. The reduction of culturable bacteria in the dark is attributed to interactions between the cells and the powdered photocatalyst and not photocatalysis (i.e. the action of ROS).49 For this reason, 60 min of dark phase are included prior to each photocatalytic experiment to specifically measure the rate of removal due to photocatalysis.
The optimisation of cerium load in zinc oxide yielded drastic improvements in inactivation efficiencies when compared to the undoped ZnO. This is most noticeable after 60 min of treatment, the removal efficiency of all the doped ZnO is 1 to 3 orders of magnitude higher then ZnO undoped (Fig. 5). A gradual increase in efficiency was observed with cerium load. E. coli inactivation was higher than 99.995% for Ce-400, Ce-700, Ce-1000 within 60 min treatment time. It is worthy to mention that they even performed better than the standard TiO2 Degussa P25. By the end of the treatment time the percentage of inactivation reach comparable levels for all catalysts tested. Calza et al. obtained similar results with 1% cerium doped ZnO,32 however the fastest of the doped catalysts therein was in the same range of TiO2 under UVA light, and only under UV-visible light did the cerium doped ZnO overtake TiO2. This is expected since the doped catalyst has a lower band gap energy and thus can harness a larger part of the visible light spectrum.
There seems to be a positive correlation between cerium load and efficiency of inactivation up to a peak at ZnO–Ce400 (i.e. 0.038
:
1 Ce
:
Zn as measured by XRF). The two higher doping levels of cerium doped catalysis (namely Ce-700 and Ce-1000) did not produce further improvement but maintained a high level of efficiency. The optimised quantity of cerium for bacterial inactivation is thus determined to be 0.04 atoms of cerium per atom of zinc.
To the best of our knowledge, cerium doped ZnO has not been used for photocatalytic bacterial inactivation, it has however been used in photocatalytic reactions. Paganini et al. investigated the doping of ZnO with 1% of cerium.37 Their results show a decisive improvement in the removal of phenol (>95% degraded for the doped ZnO vs. 50% for undoped ZnO) and up to four times faster for the three contrast dyes investigated using Ce doped ZnO over TiO2 P-25 and undoped ZnO for the same duration. Jiang et al. showed optimum performance of cerium doped ZnO against methyl orange at 0.3% Ce loading and slower removal rates at the two other Ce loadings of 0.1% and 0.5%.33 Calza et al. observed higher efficiencies in removal of acesulfame K at 1% Ce loading over 0.5%,32 The differences between optimums for different substrates indicates that the optimisation should be targeted towards the substrate of interest. Since there is a clear correlation between ˙OH radical generation and bacterial inactivation50 and since the removal of organic compounds by photocatalysis is based on the same radical chemistry, there might be room for additional improvement in the removal of chemicals by further increasing the cerium load to the optimum of 4% identified herein. However, the efficiency of removal of both chemical compounds and biological matter does not exclusively depend on quantity of ROS generation. Physicochemical conditions such as adsorption are affected by doping.26,27 This in turn affects reaction rates since a better adsorbed species is in closer proximity to the site of generation of the very short-lived radicals increasing the probability that the radicals take part in a reaction with the compound of interest.
A number of novel photocatalysts that show higher bacterial inactivation activity than Degussa TiO2 P-25 are reported in literature. Zhu et al. synthesised a composite film of P/Ag/Ag2O/Ag3PO4/TiO2 catalyst reporting fast disinfection of E. coli under high intensity solar light (50 mW cm−2) in a tubular reactor.51 Karaolia et al. used reduced graphene oxide–TiO2 composites for the disinfection of bacteria and antibiotic resistant bacteria showing increased activity in some cases over commercial TiO2.15 Higher activity was observed in co-deposited TiO2 and WO3 on reduced graphene oxide to suppress electron hole-pair recombination.52 Regrettably, photocatalysts involving carbon materials such as graphene oxide, reduced graphene oxide and graphene have the disadvantage of involving high cost in the synthesis and usually employing the Hummer's method which leave much to desire in terms of green synthetic practices. Ibrahim and Asal, used a similarly facile method as the one used herein to dope ZnO with 3 lanthanides giving improvements in bacterial inactivation using UV-A lamps at 0.9 mW cm−2 over undoped ZnO but the results were not compared against TiO2 in the same conditions.53 The three lanthanides used gave very similar results at 0.025 mole ratio of the dopant. However, the highest activity in inactivation efficiency for all three cases was relatively low with only approximately 80% of the initial 2.3 × 104 CFU mL−1 inactivated within 120 min of treatment time. The authors attributed the higher activity of the lanthanide doped compared to un-doped ZnO to modified surface properties that led to higher adsorption and bacterial inactivation rates. Their results however show only marginally improved activity of the optimal doped catalyst over their un-doped ZnO. In contrast the cerium doped catalysts used herein showed up to log
3 higher efficiency of inactivation relative to un-doped ZnO after 60 min of treatment and at comparable UV irradiance of 1.26 mW cm−2. Li et al. synthesised ZnO/ZnFe2O4 coupled photocatalysts using high temperature treatment of sphalerite.54 At 1 g L−1 catalyst loading and 3.3 mW cm−2 of visible light with the UV region filtered out, the catalysts reported therein showed improvement over ZnO in terms of bacterial inactivation with the best performing catalyst achieving complete inactivation after 180 min of treatment while ZnO produced less than 1
log after 180 min and less than 2
log after 300 min. Dark controls for bacterial inactivation and activity relative to the established standard TiO2-P25 are not reported. The main limitation, together with long treatment times, is the high temperature (1200 °C) needed for the synthesis of the optimised catalysts. Kubacka et al. used zinc and silver modified titania at 0.6 g L−1 to improve the activity over unmodified titania against E. coli.55 However, the experimental setup reported therein (spectrophotometer used as light source) limits the comparability of results. Venieri et al. doped TiO2 using a similar method to the one used herein to produce photocatalysts with higher activity under simulated solar light at an intensity of 13.1 mW cm−2. Complete inactivation was recorded after 10–15 min for optimised catalysts and 30 min for TiO2-P25.56 Gupta et al. demonstrated an improvement in activity over unmodified ZnO by the interfacial coupling of copper and silver on iron doped ZnO. 6
log10 inactivation was recorded for 3 wt% Cu coupled iron doped ZnO under visible light (>400 nm 68 klx) and 0.25 g L−1 catalyst load. For chemical pollutant degradation an enhanced removal rate over unmodified ZnO was observed and this improvement was attributed to decreased electron hole-pair recombination.57 It is also worth noting that the improvement in the rate of disinfection demonstrated with ZnO–Ce400 is not due to a simple shift in the band gap resulting in a higher portion of the electromagnetic spectrum being utilised. This suggests that the higher activity is potentially due to modified surface activity resulting in higher affinity to the bacterial cells and/or reduced recombination rates of electron–hole pairs.
:
1 at/at Ce
:
Zn at 0.1 g L−1 concentration inactivated 99.995% of the initial bacteria after 60 min and below the limits of quantification after 135 min of treatment and 1.26 mW cm−2 at 365 nm. The results achieved are highly encouraging, even exceeding the efficiency of the standard TiO2 Degussa P25 in identical conditions.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra05020a |
| This journal is © The Royal Society of Chemistry 2018 |