Abstract
In the last couple decades, several viral outbreaks resulting in epidemics and pandemics with thousands of human causalities have been witnessed. The current Covid‐19 outbreak represents an unprecedented crisis. In stopping the virus’ spread, it is fundamental to have personal protective equipment and disinfected surfaces. Here, the development of a TiO2 nanowires (TiO2NWs) based filter is reported, which it is believed will work extremely well for personal protective equipment (PPE), as well as for a new generation of air conditioners and air purifiers. Its efficiency relies on the photocatalytic generation of high levels of reactive oxygen species (ROS) upon UV illumination, and on a particularly high dielectric constant of TiO2, which is of paramount importance for enhanced wettability by the water droplets carrying the germs. The filter pore sizes can be tuned by processing TiO2NWs into filter paper. The kilogram‐scale production capability of TiO2NWs gives credibility to its massive application potentials.
Keywords: E. coli, electron spin resonance, filter, nanowires, photocatalysis, reactive oxygen species, TiO2
In TiO2 nanowire‐based filters, the high dielectric constant of TiO2 enhances the wettability by the water droplets carrying the bacteria or viruses. Upon UV illumination, reactive oxygen species (e.g., OH., O2 −., H2O2) are created, which destroy the germs. Such a filter is suitable for reusable personal protective mask, for a new generation of air conditioners and air purifiers.
1. Introduction
The threats coming from microorganisms, viruses and bacteria are getting more frequent and more devastating lately, primarily due to the highly increased mobility of people and goods, which enhances the spread of infections. One may have in mind the outbreak of SARS‐CoV in 2004[ 1 , 2 , 3 , 4 , 5 , 6 ] of H1N1 in 2009,[ 7 , 8 , 9 ] and the Ebola virus in 2018.[ 10 , 11 , 12 ] In the case of bacteria, the O104:H4 strain of Escherichia coli [ 13 , 14 , 15 , 16 ] caused causalities, but the danger is also coming from antibiotics resistant species like Legionella bacteria,[ 17 , 18 , 19 ] Klebsiella pneumoniae,[ 20 , 21 , 22 , 23 ] and Staphylococcus aureus.[ 24 , 25 , 26 , 27 ]
The most sinister actuality is the pandemic outbreak of Covid‐19, caused by the highly contagious coronavirus SARS‐CoV‐2. It has rapidly spread worldwide, leading to infections on a millions‐scale, along with hundreds of thousands of human losses.[ 28 ]
As if today, the world is far behind in finding an efficient fight against this disease. Our society needs to employ all possible means in reducing the number of infections and mortalities.
In this struggle, one possibility is to create specialized surfaces, which by photophysical effects could damage and disable airborne pathogens such as bacteria and viruses,[ 29 ] as well as SARS‐CoV‐2. The bactericidal‐virucidal surfaces suggested herein have potential applications in air filtering systems such as air conditioners, and most importantly in the fabrication of personal protective masks. Filters made of photocatalytic materials that generate high levels of reactive oxygen species (ROS) upon UV light illumination, could not only efficiently inactivate airborne pathogens, but would also offer the benefits of reusability.
From this perspective, TiO2‐based photocatalytic materials represent a very promising solution for the above‐mentioned field of applications.[ 30 , 31 , 32 , 33 , 34 , 35 , 36 ] Most explicitly, enhanced photocatalytic properties are expected from nanoparticular forms of TiO2, such as TiO2 nanoparticles (TiO2NPs) and 1D TiO2 nanostructures, like nanowires (TiO2NWs) or nanotubes (TiO2NTs), which offer a much larger specific surface area than bulk and polycrystalline counterparts.[ 37 , 38 ] It has been demonstrated that the high surface‐to‐volume ratio of 1D TiO2 nanostructures leads to a marked decrease in the hole–electron recombination rate, as well as to a faster interfacial charge carrier transfer rate. Both of these factors are favorable for enhancing the photocatalytic activity of 1D nanoparticular forms of TiO2.[ 39 ]
It is also worth mentioning that, due to free electrons’ high mobility in the air, both virus‐laden water microdroplets and single airborne microorganisms often accumulate a noticeable negative charge. Therefore, the high dielectric constant of TiO2—with its concomitant large charge‐storage capacity—contributes to the enhanced electrostatic precipitation of the droplets on the nonwoven network of TiO2NWs. Moreover, the presence of numerous Ti3+ sites on the surface or TiO2NWs, previously reported by us,[ 40 ] is highly favorable for water adsorption, leading to super‐hydrophilicity at the macroscale.[ 41 ] Therefore, the super‐hydrophilicty of TiO2NWs‐based filtering materials causes water droplets to adhere and spread on the TiO2 surface, aiding in filtration.
Thus, all things considered, the TiO2NWs are very suitable for preparing larger photocatalytic surfaces because they also have an ideal shape for assembly into nanoporous aerogel membranes.[ 42 ] We here report on the feasibility of producing a reusable photocatalytically active filter paper from TiO2NWs. We also provide a thorough characterization of this composite material in terms of its high propensity toward photogeneration of ROS, and the degradation of microbiological pathogens.
2. Results and Discussion
2.1. Synthesis
The herein presented elaboration of a practical and reliable large‐scale synthesis of TiO2NWs represents a breakthrough strategy toward the fabrication of photocatalytic materials suitable for preparing easily sterilizable air filters, including reusable protective masks.
Titanium oxide nanowires are normally attained via hydrothermal synthesis, where nanoparticles of TiO2 are treated in a closed vessel at high pressures of 140–200 °C during several days of reaction time (see Figure 1a).[ 43 , 44 , 45 , 46 ] Unfortunately, the yield of such synthesis is very low, several few gramms per run, which is a strong handicap for large scale applications.
Through an original synthesis method,[ 42 ] production has been greatly upscaled. In a base solution, Ti containing starting material is added, and the mixture is heated in a base resistive vessel to 70 °C. A shear mixing results the formation of a high fraction of mesoporous titanates, ans a lower fraction of macroporous material. The textural properties can be tuned by temperature, with and by the time of shear mixing. After the synthesis, the jelly titanium oxide composite (see Figure 1b) is transferred into a press or centrifuge to separate it from the residues of the reaction. In a single shot the quantity of titanate NWs is in the 0.3–1 kg range.
The NWs can be processed into films by doctor blading, screen printing, filtering, dip coating, and spin coating with a thickness less than 2 μm.[ 47 ] The film can be removed from the support if the support is a hydrophobic material. After air drying at 120 °C, calcination and phase transformation from titanate to anatase to rutile occur within a range of 400–1000 °C range.[ 48 ] It results in a freestanding, flexible film, which—depending on the thickness—could be even transparent.[ 49 ] Note that the calcination fuses the TiO2NWs together (see the inset to Figure 1c and the Supporting Information), thus resulting in a filter paper, which does not release nanostructures under normal flow conditions.[ 37 ]
This film of TiO2NWs filter paper is the starting structure for all water and air filters which, by UV illumination, could be disinfected from viruses, bacteria, and generally all organic species. Here below, the efficiency of TiO2NWs and the filter is demonstrated by the photocatalytic ROS generation, as well as the corresponding high potential for DNA degradation and annihilation of E. coli, the gold‐standard bacteria.
2.2. The Principle
The principle of the filter papers operation is illustrated in Figure 2 . The pore‐sizes of the filter can be tuned during its fabrication process by modifying both the thickness and density of the filter paper (See Figure S2 of Supporting Information). This can allow for the efficient trapping of pathogens of different sizes, including the smallest viruses (Figure 2a).
An important characteristic of the TiO2 is its high dielectric constant (ε) in the 70–80 range, which defines the polaronic nature of the electronic charges in the material.[ 50 ] A high ε value is important for the filtering material, since it facilitates wetting the filter's surface by droplets of water or saliva, which could carry the germs.
It is worth mentioning that the presence of moisture, even in the form of humidity traces, is essential for the photocatalytic and antimicrobial activities of the filter paper. It is therefore widely accepted that in an aqueous milieu and upon UV illumination, the TiO2—based photocatalytic materials efficiently generate the so‐called ROS—that is, hydroxyl radicals (OH ∙ ), hydroperoxyl radicals (HO2 ∙ ), hydrogen peroxide (H2O2), singlet oxygen (1O2), and superoxide radicals (O2 −∙ ).[ 51 ] In particular, the UV‐light excited TiO2 nanoparticles convert the incident photons into electron/hole pairs. These can either recombine, or migrate to the particle's surface, where they can generate ROS and/or activate redox processes.[ 52 ] The plausible mechanisms of photogeneration of various forms of ROS during the UV‐light induced stepwise oxidation of water (H2O), and stepwise reduction of oxygen (O2) taking place on the surface of the TiO2NWs, are schematically illustrated in Figure 2b.
In general, OH ∙ radicals are considered the most powerful oxidizing species.[ 53 , 54 ] They are also believed to be the first responsible for the photodegradation processes of organic micropollutants in aqueous solutions. Although concomitantly photogenerated superoxide radicals (O2 −∙ ) have less oxidizing properties, they still can lead to the formation of other active ROS, including singlet oxygen (1O2), which is also very potent.[ 51 ]
The efficiency of the TiO2NWs and the composed filter paper in producing ROS is demonstrated using several experimental techniques, including electron spin resonance (ESR), degeneration of a biological molecule (DNA) detected by atomic force microscopy (AFM) and gel electrophoresis, as well as by the photocatalytic annihilation of E. coli cells tracked by survival counting using UV illumination.
2.3. ESR Study of the ROS Generation on TiO2NWs Surface upon UV Illumination
The documentation of ROS is a defiant task because of their short lifetime, of the order of 10−10 to 10−6 s. One of the best methods is to convert them into stable radicals, which could be easily, selectively, and sensitively identified ESR spectroscopy.[ 55 ] This method is based on spin‐trapping molecules which react with ROS and change their spin state: either the existing spins are scavenged or they produce stable spin‐adducts. Their spectra can be easily integrated and their concentration measured.
The propensity of the herein synthesized TiO2NWs‐based composite to photogenerated ROS was checked in the aqueous milieu using a custom‐designed photoreactor (details in the Supporting Information). The sketch of the corresponding experimental setup is overviewed in Figure 3a, with more details given in Supporting Information. Specifically, the inner wall of the tubular photoreactor was covered with the TiO2NWs‐based composite material, thus forming a photocatalytic lining. The built‐in commercially‐available UV lamp (Hamatsu, λ = 365 nm of 16 mW cm−2) served as a UV light source for inducing the photocatalytic processes at the surface of the TiO2NWs‐based photocatalytic lining.
The stable nitroxide radical, 4‐hydroxy‐2,2,6,6‐tetramethylpiperidine‐1‐oxyl (called TEMPOL), was used as a target molecule for the photogenerated OH ∙ and O2 −∙ radicals. It is well known that the ESR‐active TEMPOL is a water‐soluble antioxidant, reportedly acting as a superoxide dismutase (SOD) mimicking agent.[ 56 ] In particular, reactive pathways of TEMPOL with O2 −∙ and OH ∙ radicals have been reported to introduce structural changes at the 1‐ and 4‐positions of the TEMPOL molecule, respectively.[ 57 , 58 ] Acting in concert, these structural changes induce both the decay of the ESR‐active TEMPOL, as well as the concurrent formation of another ESR‐active radical, 4‐oxo‐TEMPO, i.e., TEMPONE. In Figure 3 photocatalytic decomposition of TEMPOL is shown (the TEMPONE case is given in the Supporting Information).
In aqueous solutions, TEMPOL reveal easily detectable ESR spectra, which are characteristic for NO‐centered radicals bearing one unpaired electron (S = 1/2). In particular, the corresponding ESR signals consist of three well resolved features resulting from the 14N atom‐related hyperfine splitting (I = 1). Due to small differences in hyperfine splitting constants—A 14 N, and spectroscopic g ‐factor values, of 17.1 G/g = 2.0057 for TEMPOL and 16.1 G/g = 2.0056 for TEMPONE—these two nitroxide radicals can be very easily distinguished.
The time‐course of 0–120 min for the photocatalytic decomposition of TEMPOL in the presence of the synthesized TiO2NWs–based photocatalytic material is shown in Figure 3b. As can be seen, the characteristic ESR signal of TEMPOL rapidly decays as a function of time of exposure to the UV light in the photoreactor. Over 120 min of the exposure time, the overall ESR signal intensity of TEMPOL decays by a factor of ≈15. With the photoinactivation of TEMPOL, a concurrent process of the formation of TEMPONE can also be observed (Figure 3c, the weak signal at 3255 G). These two processes—the decay of TEMPOL and the progressive increase of TEMPONE—prove that under UV light exposure the herein synthesized TiO2NWs‐based photocatalytic material generates O2 −∙ and OH ∙ radicals.
2.4. AFM and Electrophoresis Demonstration of the DNA Rupturing by ROS
After demonstrating that TiO2NWs can very efficiently generate ROS, we checked its effect on an important biomolecule, the DNA, in an experimental configuration described in the Supporting Information. We used a commercial DNA pUC19, which after treatment with an enzyme remain stayed open, and not supercoiled, with a length of 913 nm. A suitable solution of TiO2NWs and DNA was exposed to 365 nm UV radiation (see sketch in Figure 4a), with a particular cycle (30 s of irradiation followed by 2 min of shaking and rotation without irradiation) to avoid overheating which could lead to false results.
Variable exposure times to UV illumination were employed: 3, 5, 10, and 15 min. The TiO2/DNA solution was finally deposited, with a suitable procedure, see Supporting Information paragraph 4, on a smooth mica substrate for AFM observation.
The AFM imaging technique made it possible to observe the presence or disappearance of the DNA strands in a very local area. In particular, the tapping mode AFM images shown in Figure 4b clearly demonstrate that, with increasing illumination times, the DNA strands are being progressively degraded and, after 10 min of exposure, only their debris could be detected.
This observation is concomitant with the gel electrophoresis experiment. DNA strands and their fragments migrate through the agarose gel with different velocities, v, where v = E × z/f. These velocities result from the differences in the strength of the local electric field (E), the net charge (z), and the friction force (f). The latter parameter, f, is a quantity dependent on the DNA strand size.
The location of the DNA strands and their fragments in the gel was visualized by means of attaching a suitable fluorescent dye, GelRed from Biotium. One can see (Figure 4c) that in the case of no UV exposure, the DNA strands are slowly spreading in the gel due to their large sizes and important friction. In contrast, due to low friction from their small size, after 15 min of UV exposure small DNA debris quickly moved to the upper side of the gel.
As can also be seen in Figure 4c, the control electrophoresis experiments for DNA suspended in distilled water, in the absence of contact with TiO2NWs and performed both in the dark and under UV light illumination, did not reveal any marked fragmentation of the DNA strands. Thus, the potential photolytic impact of the uniquely employed UV light turned out to be quite negligible as compared to the synergetic photocatalytic action of TiO2NWs and UV illumination.
In brief, the electrophoresis experiments performed on the DNA strands corroborate the ESR and AFM studies results, which both point to the strength of TiO2NWs photocatalytic action when exposed to UV light illumination.
2.5. The Efficiency of the TiO2NWs Photocatalytic Filter in the Case of E. Coli
The next step was testing the TiO2NWs‐based filters performance in killing microorganisms. By the filtering action, these can be stopped as they adhere to the fibers of humid TiO2NWs. Humidity is always present under typical daily conditions, especially if such a filter paper is used for air‐conditioning applications, where, after switching the air‐conditioner off, the water condensation commonly occurs. Such an environment is therefore favorable for bacterial proliferation, unless it is disinfected by UV light.
Here, we used the reference bacteria for such studies, the E. coli. From a bacterial suspension of known concentration of 2 × 108 CFU per mL, a volume of 5 µL was dropped on the filter surface (see the illustration in Figure 5a) and exposed to illumination at 365 nm wavelength from a UV light source with a power density of 16 mW cm−2, for discrete time intervals of 20, 60, 100, and 200 s. After each illumination run, the E. coli was washed off the membranes by placing them in Eppendorf tubes containing physiological salt, and rinsing for 60 min to retrieve the survived cells back into solution. Next, serial dilutions were prepared from the solution containing cells/membrane, and 10 µL of each dilution was spotted on LB agar plates. Agar plates were incubated overnight at 37 °C. The cell concentration per mL (CFU per mL) was extrapolated from the colonies counted at the appropriate spots for TiO2NWs membrane, from which the survival rate could be determined. In the control experiment, non‐UV exposed E. coli bacteria were washed off the TiO2NWs filter paper and underwent the same protocol, thus making it possible to reproduce the initial concentration of bacteria.
As can be seen in the scanning electron microscopy (SEM) image in Figure 5b, already after the initial exposure to UV light for 30 s, numerous damaged bacteria could be identified, as highlighted by the yellow stars in this figure. Clearly, the actual population of nonviable (inactivated) cells was markedly larger.
Consequently, for the experiment performed on the surface of the TiO2NWs filter paper, after 60 s of UV light exposure one can hardly identify any bacteria which could still proliferate (red trace in Figure 5c). Although the control experiment performed with E. coli bacteria on the wet Teflon filter surface reveals some photodegradation (blue trace in Figure 5c), the actual degree of bacterial photoinactivation is definitely noncommensurable with the one observed for the TiO2NWs‐based photocatalytic filter. This points to the extreme efficiency of our TiO2NWs filter paper in killing bacteria. This filter paper may also kill other microbial pathogens, such as viruses, which can be filtered out and photocatalytically inactivated at its surface.
One could also notice that the deleterious effects of UV exposures are occurring at different timescales: for the ESR experiments with TEMPOL it is of 120 min, while for the E. coli bacteria it rather happens on a timescale of 120 s. This is due to the fact that ROS, although extremely reactive, are short‐lived, and correspondingly, their radius of action is very limited. Thus, the mutual distances between the biological species and TiO2NWs are important. The E. coli bacteria are anchored to the filter surface, so the effect of ROS is very efficient, while for the ESR, the organic molecules pass by in flow condition. For the AFM and electrophoresis studies, the DNA and TiO2NWs are in a confined space, and the timescale is intermediate to the two other configurations.
3. Conclusion and Outlook
The immediate importance of such a filter is rendered by the Covid‐19 crisis urgency, which has rapidly spread into a pandemic. Since the transmission routes of its vector, SARS‐CoV‐2 virus, are still far from understood, wearing personal protective masks is of great importance.[ 59 ] Moreover, according to some health experts, the currently used disposable facemasks do not block all pathogens, neither can they inactivate the viruses. Thus, used and discarded masks can even become a vector for disease, especially if the virus survives on a disposable mask.
Therefore, easily sterilizable and reusable masks with antiviral properties could provide a potent prevention tool against the rapid spread of SARS‐CoV‐2 and other coronaviruses that have evolved into more severe illnesses such as SARS and MERS. We estimate that such a TiO2 NWs based light‐sterilizable mask may be reused more than 1000 times. A prototype of such a mask has been developed and is shown in Figure 6 . Evidently, this design addresses an impending mask shortage crisis. In addition, it should also reduce the environmental and public health issues related to the millions of masks discarded daily worldwide outside of the medical environment, where infectious and hazardous medical waste is properly treated and disposed.
As of today, the technology we propose, exclusively under laboratory conditions, will allow for the filter production capacity of about 100–200 m2 per week. This is enough to fabricate 40 000–80 000 reusable masks monthly. Clearly, there is no upper limit of this technology for an industrial production line. It should be mentioned that such a nanoporous photocatalytic filter can also be used for other purposes, such as air conditioners and water purification.[ 60 ]
Conflict of Interest
The authors declare no conflict of interest.
Supporting information
Acknowledgements
E.H. gratefully acknowledges the support of the support of Zeno Karl Schindler, MBR Global Water Award, Swiss‐African Research Cooperation (SARECO) and Tech4impact Playgrant EPFL. We would also like to thank Lenke Horváth, Rita Smajda, Raphaël Foschia, Giovanni Dietler and Jérôme Gabathuler for their help in the experiments. A special thanks to Claude Marion for his continous interest for the project.
Horváth E., Rossi L., Mercier C., Lehmann C., Sienkiewicz A., Forró L., Photocatalytic Nanowires‐Based Air Filter: Towards Reusable Protective Masks. Adv. Funct. Mater. 2020, 30, 2004615. 10.1002/adfm.202004615
References
- 1. Ksiazek T. G., Erdman D., Goldsmith C. S., Zaki S. R., Peret T., Emery S., Tong S., Urbani C., Comer J. A., Lim W., Rollin P. E., Dowell S. F., Ling A.‐E., Humphrey C. D., Shieh W.‐J., Guarner J., Paddock C. D., Rota P., Fields B., DeRisi J., Yang J.‐Y., Cox N., Hughes J. M., LeDuc J. W., Bellini W. J., Anderson L. J., N. Engl. J. Med. 2003, 348, 1953. [DOI] [PubMed] [Google Scholar]
- 2. Drosten C., Günther S., Preiser W., van der Werf S., Brodt H.‐R., Becker S., Rabenau H., Panning M., Kolesnikova L., Fouchier R. A. M., Berger A., Burguière A.‐M., Cinatl J., Eickmann M., Escriou N., Grywna K., Kramme S., Manuguerra J.‐C., Müller S., Rickerts V., Stürmer M., Vieth S., Klenk H.‐D., Osterhaus A. D. M. E., Schmitz H., Doerr H. W., N. Engl. J. Med. 2003, 348, 1967. [DOI] [PubMed] [Google Scholar]
- 3. Tsang K. W., Ho P. L., Ooi G. C., Yee W. K., Wang T., Chan‐Yeung M., Lam W. K., Seto W. H., Yam L. Y., Cheung T. M., Wong P. C., Lam B., Ip M. S., Chan J., Yuen K. Y., Lai K. N., N. Engl. J. Med. 2003, 348, 1977. [DOI] [PubMed] [Google Scholar]
- 4. Lee N., Hui D., Wu A., Chan P., Cameron P., Joynt G. M., Ahuja A., Yung M. Y., Leung C. B., To K. F., Lui S. F., Szeto C. C., Chung S., Sung J. J. Y., N. Engl. J. Med. 2003, 348, 1986. [DOI] [PubMed] [Google Scholar]
- 5. Poutanen S. M., Low D. E., Henry B., Finkelstein S., Rose D., Green K., Tellier R., Draker R., Adachi D., Ayers M., Chan A. K., Skowronski D. M., Salit I., Simor A. E., Slutsky A. S., Doyle P. W., Krajden M., Petric M., Brunham R. C., McGeer A. J., N. Engl. J. Med. 2003, 348, 1995. [DOI] [PubMed] [Google Scholar]
- 6. World Health Organization (WHO) , 2003.
- 7. Fraser C., Donnelly C. A., Cauchemez S., Hanage W. P., van Kerkhove M. D., Hollingsworth T. D., Griffin J., Baggaley R. F., Jenkins H. E., Lyons E. J., Jombart T., Hinsley W. R., Grassly N. C., Balloux F., Ghani A. C., Ferguson N. M., Rambaut A., Pybus O. G., Lopez‐Gatell H., Alpuche‐Aranda C. M., Chapela I. B., Zavala E. P., Guevara D. M. E., Checchi F., Garcia E., Hugonnet S., Roth C., Science 2009, 324, 1557. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 8. Garten R. J., Davis C. T., Russell C. A., Shu B., Lindstrom S., Balish A., Sessions W. M., Xu X., Skepner E., Deyde V., Okomo‐Adhiambo M., Gubareva L., Barnes J., Smith C. B., Emery S. L., Hillman M. J., Rivailler P., Smagala J., de Graaf M., Burke D. F., Fouchier R. A. M., Pappas C., Alpuche‐Aranda C. M., López‐Gatell H., Olivera H., López I., Myers C. A., Faix D., Blair P. J., Yu C., Keene K. M., Dotson P. D., Boxrud D., Sambol A. R., Abid S. H., George K. S., Bannerman T., Moore A. L., Stringer D. J., Blevins P., Demmler‐Harrison G. J., Ginsberg M., Kriner P., Waterman S., Smole S., Guevara H. F., Belongia E. A., Clark P. A., Beatrice S. T., Donis R., Katz J., Finelli L., Bridges C. B., Shaw M., Jernigan D. B., Uyeki T. M., Smith D. J., Klimov A. I., Cox N. J., Science 2009, 325, 197.19465683 [Google Scholar]
- 9. Smith G. J. D., Vijaykrishna D., Bahl J., Lycett S. J., Worobey M., Pybus O. G., Ma S. K., Cheung C. L., Raghwani J., Bhatt S., Peiris J. S. M., Guan Y., Rambaut A., Nature 2009, 459, 1122. [DOI] [PubMed] [Google Scholar]
- 10. Barry A., Ahuka‐Mundeke S., Ali Ahmed Y., Allarangar Y., Anoko J., Archer B. N., Aruna Abedi A., Bagaria J., Belizaire M. R. D., Bhatia S., Bokenge T., Bruni E., Cori A., Dabire E., Diallo A. M., Diallo B., Donnelly C. A., Dorigatti I., Dorji T. C., Escobar Corado Waeber A. R., Fall I. S., Ferguson N. M., FitzJohn R. G., Folefack Tengomo G. L., Formenty P. B. H., Forna A., Fortin A., Garske T., Gaythorpe K. A., Gurry C., Hamblion E., Harouna Djingarey M., Haskew C., Hugonnet S. A. L., Imai N., Impouma B., Kabongo G., Kalenga O. I., Kibangou E., Lee T. M.‐H., Lukoya C. O., Ly O., Makiala‐Mandanda S., Mamba A., Mbala‐Kingebeni P., Mboussou F. F. R., Mlanda T., Mondonge Makuma V., Morgan O., Mujinga Mulumba A., Mukadi Kakoni P., Mukadi‐Bamuleka D., Muyembe J.‐J., Bathé N. T., Ndumbi Ngamala P., Ngom R., Ngoy G., Nouvellet P., Nsio J., Ousman K. B., Peron E., Polonsky J. A., Ryan M. J., Touré A., Towner R., Tshapenda G., Van De Weerdt R., Van Kerkhove M., Wendland A., Yao N. K. M., Yoti Z., Yuma E., Kalambayi Kabamba G., de J. Lukwesa Mwati D., Mbuy G., Lubula L., Mutombo A., Mavila O., Lay Y., Kitenge E., Lancet 2018, 392, 213.30047375 [Google Scholar]
- 11. Yang Z., Duckers H. J., Sullivan N. J., Sanchez A., Nabel E. G., Nabel G. J., Nat. Med. 2000, 6, 886. [DOI] [PubMed] [Google Scholar]
- 12. World Health Organization (WHO) , Ebola health update – DRC, 2019, https://www.who.int/emergencies/diseases/ebola/drc‐2019.
- 13. Rohde H., Qin J., Cui Y., Li D., Loman N. J., Hentschke M., Chen W., Pu F., Peng Y., Li J., Xi F., Li S., Li Y., Zhang Z., Yang X., Zhao M., Wang P., Guan Y., Cen Z., Zhao X., Christner M., Kobbe R., Loos S., Oh J., Yang L., Danchin A., Gao G. F., Song Y., Li Y., Yang H., Wang J., Xu J., Pallen M. J., Wang J., Aepfelbacher M., Yang R., N. Engl. J. Med. 2011, 365, 718. [DOI] [PubMed] [Google Scholar]
- 14. Mellmann A., Harmsen D., Cummings C. A., Zentz E. B., Leopold S. R., Rico A., Prior K., Szczepanowski R., Ji Y., Zhang W., McLaughlin S. F., Henkhaus J. K., Leopold B., Bielaszewska M., Prager R., Brzoska P. M., Moore R. L., Guenther S., Rothberg J. M., Karch H., PLoS One 2011, 6, e22751. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 15. Bielaszewska M., Mellmann A., Zhang W., Köck R., Fruth A., Bauwens A., Peters G., Karch H., Lancet Infect. Dis. 2011, 11, 671. [DOI] [PubMed] [Google Scholar]
- 16. Kunsmann L., Rüter C., Bauwens A., Greune L., Glüder M., Kemper B., Fruth A., Wai S. N., He X., Lloubes R., Schmidt M. A., Dobrindt U., Mellmann A., Karch H., Bielaszewska M., Sci. Rep. 2015, 5, 13252. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 17. Muder R. R., Yu V. L., Woo A. H., Arch. Intern. Med. 1986, 146, 1607. [PubMed] [Google Scholar]
- 18. Bitar D. M., Molmeret M., Abu Kwaik Y., Int. J. Med. Microbiol. 2004, 293, 519. [DOI] [PubMed] [Google Scholar]
- 19. Bartfeld S., Engels C., Bauer B., Aurass P., Flieger A., Brüggemann H., Meyer T. F., Cell. Microbiol. 2009, 11, 1638. [DOI] [PubMed] [Google Scholar]
- 20. Bagley S. T., Infect. Control Hosp. Epidemiol. 1985, 6, 52. [Google Scholar]
- 21. Struve C., Krogfelt K. A., FEMS Microbiol. Lett. 2003, 218, 149. [DOI] [PubMed] [Google Scholar]
- 22. Brisse S., Passet V., Grimont P. A. D., Int. J. Syst. Evol. Microbiol. 2014, 64, 3146. [DOI] [PubMed] [Google Scholar]
- 23. Delincé M. J., Bureau J.‐B., Teresa López‐Jiménez A., Cosson P., Soldati T., McKinney J. D., Lab Chip 2016, 16, 3276. [DOI] [PubMed] [Google Scholar]
- 24. Lowy F. D., N. Engl. J. Med. 1998, 339, 520. [DOI] [PubMed] [Google Scholar]
- 25. Loir Y. L., Gautier M., in Encyclopedia of Molecular Mechanisms of Disease (Ed.: Lang F.), Springer, Berlin, Heidelberg, 2009, pp. 1974–1975. [Google Scholar]
- 26. Foster T. J., Höök M., Trends Microbiol. 1998, 6, 484. [DOI] [PubMed] [Google Scholar]
- 27. Baldoni D., Hermann H., Frei R., Trampuz A., Steinhuber A., J. Clin. Microbiol. 2009, 47, 774. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 28. World Health Organization (WHO) , Coronavirus Disease (COVID‐19) – events as they happen, https://www.who.int/emergencies/diseases/ebola/drc‐2019.
- 29. Náfrádi B., Náfrádi G., Martin‐Hamka C., Forró L., Horváth E., Langmuir 2017, 33, 9043. [DOI] [PubMed] [Google Scholar]
- 30. Matsunaga T., Tomoda R., Nakajima T., Wake H., FEMS Microbiol. Lett. 1985, 29, 211. [Google Scholar]
- 31. Watts R. J., Kong S., Orr M. P., Miller G. C., Henry B. E., Water Res. 1995, 29, 95. [Google Scholar]
- 32. Herrera Melián J. A., Doña RodrıÍguez J. M., Viera Suárez A., Tello Rendón E., Valdés do Campo C., Arana J., Pérez Peña J., Chemosphere 2000, 41, 323. [DOI] [PubMed] [Google Scholar]
- 33. Araña J., Herrera Melián J. A., Doña RodrıÍguez J. M., González DıÍaz O., Viera A., Pérez Peña J., Marrero Sosa P. M., Espino Jiménez V., Catal. Today 2002, 76, 279. [Google Scholar]
- 34. Dunlop P. S. M., Byrne J. A., Manga N., Eggins B. R., J. Photochem. Photobiol. A: Chem. 2002, 148, 355. [Google Scholar]
- 35. Ibáñez J. A., Litter M. I., Pizarro R. A., J. Photochem. Photobiol. A: Chem. 2003, 157, 81. [Google Scholar]
- 36. Gogniat G., Thyssen M., Denis M., Pulgarin C., Dukan S., FEMS Microbiol. Lett. 2006, 258, 18. [DOI] [PubMed] [Google Scholar]
- 37. Tétreault N., Horváth E., Moehl T., Brillet J., Smajda R., Bungener S., Cai N., Wang P., Zakeeruddin S. M., Forró L., Magrez A., Grätzel M., ACS Nano 2010, 4, 7644. [DOI] [PubMed] [Google Scholar]
- 38. Rosales M., Zoltan T., Yadarola C., Mosquera E., Gracia F., García A., J. Mol. Liq. 2019, 281, 59. [Google Scholar]
- 39. Nakata K., Fujishima A., J. Photochem. Photobiol., C 2012, 13, 169. [Google Scholar]
- 40. Mantulnikovs K., Szirmai P., Kollár M., Stevens J., Andričević P., Glushkova A., Rossi L., Bugnon P., Horváth E., Sienkiewicz A., Forró L., Náfrádi B., J. Phys.: Photon. 2020, 2, 014007. [Google Scholar]
- 41. Nie J., Ren Z., Bai Y., Shao J., Jiang T., Xu L., Chen X., Wang Z. L., Adv. Mater. Technol. 2019, 4, 1800300. [Google Scholar]
- 42. Horváth E., Forró L., Magrez A., Titanium oxide aerogel composites US Patent No. US2016030908 (A1), 2016.
- 43. Horváth E., Kukovecz Á., Kónya Z., Kiricsi I., Chem. Mater. 2007, 19, 927. [Google Scholar]
- 44. Horváth E., Ribič P. R., Hashemi F., Forró L., Magrez A., J. Mater. Chem. 2012, 22, 8778. [Google Scholar]
- 45. Szirmai P., Náfrádi B., Arakcheeva A., Szilágyi E., Gaál R., Nemes N. M., Berdat X., Spina M., Bernard L., Jaćimović J., Magrez A., Forró L., Horváth E., Catal. Today 2017, 284, 52. [Google Scholar]
- 46. Szirmai P., Stevens J., Horváth E., Ćirić L., Kollár M., Forró L., Náfrádi B., Catal. Today 2017, 284, 146. [Google Scholar]
- 47. Szabó T., Tóth V., Horváth E., Forró L., Szilagyi I., Langmuir 2015, 31, 42. [DOI] [PubMed] [Google Scholar]
- 48. Rossi L., Berdat X., Spina M., Brown S., Bernard L., Katrych S., Forró L., Horváth E., Ceram. Int. 2020, 46, 16321. [Google Scholar]
- 49. Rossi L., Foschia R., Glushkova A., Forró L., Horváth E., Ceram. Int. 2020, 46, 17729. [Google Scholar]
- 50. Jaćimović J., Vaju C., Magrez A., Berger H., Forró L., Gaál R., Cerovski V., Žikić R., Europhys. Lett. 2012, 99, 57005. [Google Scholar]
- 51. Nosaka Y., Nosaka A. Y., Chem. Rev. 2017, 117, 11302. [DOI] [PubMed] [Google Scholar]
- 52. Chen M., Ma J., Zhang B., Wang F., Li Y., Zhang C., He H., Appl. Catal., B 2018, 223, 209. [Google Scholar]
- 53. Ireland J. C., Klostermann P., Rice E. W., Clark R. M., Appl. Environ. Microbiol. 1993, 59, 1668. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 54. Cho M., Chung H., Choi W., Yoon J., Appl. Environ. Microbiol. 2005, 71, 270. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 55. Marchand V., Charlier N., Verrax J., Buc‐Calderon P., Levêque P., Gallez B., PLoS One 2017, 12, e0172998. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 56. Lu H., Zhen J., Wu T., Peng A., Ye T., Wang T., Yu X., Vaziri N. D., Mohan C., Zhou X. J., Am. J. Physiol.‐Renal Physiol. 2010, 299, F445. [DOI] [PubMed] [Google Scholar]
- 57. Wilcox C. S., Pharmacol. Ther. 2010, 126, 119. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 58. Marshall D. L., Christian M. L., Gryn'ova G., Coote M. L., Barker P. J., Blanksby S. J., Org. Biomol. Chem. 2011, 9, 4936. [DOI] [PubMed] [Google Scholar]
- 59. Leung N. H. L., Chu D. K. W., Shiu E. Y. C., Chan K.‐H., McDevitt J. J., Hau B. J. P., Yen H.‐L., Li Y., Ip D. K. M., Peiris J. S. M., Seto W.‐H., Leung G. M., Milton D. K., Cowling B. J., Nat. Med. 2020, 26, 676. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 60.The EPFL's invention awarded second place by the UAE's 28 Water Aid Foundation 2017, https://www.suqia.ae.
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