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Photocatalytic Silica–Resin Coating for Environmental Protection of Paper as a Plastic Substitute
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Industrial & Engineering Chemistry Research

Cite this: Ind. Eng. Chem. Res. 2022, 61, 20, 6967–6972
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https://doi.org/10.1021/acs.iecr.2c00784
Published May 13, 2022

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Abstract

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We developed an easy silica–resin coating technique to compensate for paper’s weaknesses, including its lack of water resistance and strength, and proposed its use as an environmentally friendly alternative to plastic. We demonstrate here that 2 nm anatase TiO2 nanoparticles were finely dispersed in a coating film with a thickness of several micrometers formed on the paper’s cellulose fibers and exhibited moderate photocatalytic effects such as methylene blue degradation and antibacterial activity. Additionally, the porous silica–resin film has a high adsorptive capacity, efficiently capturing organic pollutants until they decompose via photocatalytic reactions. As a result, the stable silica–resin–TiO2 composite coating protects paper from the environment for an extended period of time, transforming it into an excellent plastic substitute with enhanced functionality.

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1. Introduction

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Environmental protection and a sustainable society require the development of a de-plasticization technology. (1) However, finding a substitute for cheap, easy-to-process, and chemically stable plastic is not easy. We focused on paper, a naturally occurring and environmentally friendly material, and developed a coating technology that enables paper to be used in place of plastic. (2,3) By using a low-viscosity alkoxysilane-based liquid and drying it at ambient temperature, a silica–resin layer several micrometers thick was formed around the cellulose fibers of the paper (Figure 1a). The siloxane-bonded film reinforces the paper while retaining its flexibility and texture, and the alkyl groups such as methyl groups left in the voids of the film provide the paper with water resistance (Figure 1b). Thus, coated paper can be used in place of the majority of plastics and degrades in an environmentally benign manner after disposal.

Figure 1

Figure 1. Silica–resin coating on cellulose fibers. (a) SEM image (left top) illustrates the morphology of paper composed of intertwined cellulose fibers that are a few tens of micrometers in diameter. The fibers’ edges appear relatively bright because of the enhanced backscattering of secondary electrons from Si, which is heavier than carbon, cellulose’s primary component. The corresponding elemental maps for carbon, silicon, and titanium, which were obtained using the energy-dispersive X-ray analysis, demonstrate the formation of a silica layer on the cellulose fibers: the brighter the image, the higher the concentration. Note that a trace of titanium is concentrated around the surface layer. (b) Water resistance demonstration: after 2 weeks in water at room temperature, an origami crane made of silica–resin-coated Japanese paper retained its shape (main panel), but an origami crane made of uncoated Japanese paper lost its shape after 24 h (inset).

The silica–resin film formation reaction is basically an improved sol–gel method that does not require additional water or an acid/base catalyst, which was required in the conventional sol–gel method; (4) naturally, a high water concentration accelerates the decomposition of paper. It is believed that a trace amount of tetraisopropyl titanate (TPT, [(CH3)2CHO]4Ti) is required for the reaction. (2) Because TPT is more easily hydrolyzed than alkoxysilane, (5) it can act as an accelerator for the hydrolysis and polymerization of alkoxysilane, resulting in the quick formation of a silica–resin film in the presence of very little water from moisture and paper.
Although no experimental evidence has been provided, it is believed that the thus-consumed Ti will be integrated into the silica network or will remain in the film as titanium dioxide TiO2. If the coating contains TiO2, a photocatalytic effect is expected, leading to the development of novel functions as TiO2 nanoparticles exhibit superior photocatalytic activity (Supporting Information 1). (6−10) Indeed, previous research demonstrated that TiO2-containing paper prepared by combining a softwood craft pulp and TiO2 aqueous sol with a binder had a high photocatalytic activity, indicating that paper pulp serves as an excellent matrix. (11) The goal of this study is to characterize the presence and morphology of TiO2 in the coating film and to investigate unique capabilities of coated paper that add values and broaden possibilities of the silica–resin coating.

2. Experimental Section

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2.1. Coating Agents and Sample Preparations

We prepared a standard coating liquid that contained silane compounds and TPT at a concentration of 6.8 mol % per Si (liquid C1) (Supporting Information 2). We examined both a piece of handmade Japanese paper or filter paper treated with liquid C1 (paper C1) and a solidified bulk sample (bulk C1). Additionally, we prepared coating agents with TPT concentrations that were 2, 5, and 10 times that of standard C1 (liquids C2, C5, and C10, respectively).

2.2. Characterization Methods

The structures were characterized using powder X-ray diffraction (XRD) experiments, electron diffraction (ED), and transmission electron microscopy (TEM) (Supporting Information 3.1). The porosity of coating layers was determined using nitrogen adsorption experiments (Supporting Information 3.2). The X-ray absorption near-edge structure (XANES) spectra of Ti K-edge were obtained using synchrotron radiation (Supporting Information 3.3). The photocatalytic activity was determined by measuring the rate of decomposition of methylene blue (MB) (Supporting Information 3.4). Antibacterial performance tests were conducted using Staphylococcus aureus (Supporting Information 3.5).

3. Results and Discussion

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3.1. Porous Film Formation

The powder XRD patterns for bulk C1, C2, C5, and C10 are shown in Figure 2. There are two broad peaks whose diffraction angles correspond to the characteristic distances between Si atoms in the silica–resin network: the high-angle peak indicates the presence of short Si–Si bonds characteristic of crystalline or vitreous SiO2, while the low-angle peak indicates the presence of large voids containing methyl groups (Supporting Information 4).

Figure 2

Figure 2. Powder XRD patterns of a C1 bulk sample and of C2, C5, and C10 bulk samples with increasing TPT concentrations in coating liquids. The pattern of sample E obtained via the hydrolysis of TPT is also shown. The patterns are vertically offset for clarity. The arrow and vertical broken line indicate the location of the anatase 1 0 1 diffraction peak at 25.4°.

The low density of bulk C1 (0.925 g cm–3), which is significantly less than that of ordinary silica glass (∼2.5 g cm–3), revealed the coated film’s porous structure as well. The surface area of paper C1 was determined using nitrogen adsorption experiments, the results of which are shown in Figure 3. In comparison to pristine filter paper, paper C1 adsorbs a significant amount of nitrogen as the pressure increases, implying the formation of a porous film with a large surface area on the cellulose fibers. The desorption curve is similar to the adsorption curve for pristine paper, but they diverge as the pressure decreases for paper C1, indicating that nitrogen gas is still adsorbing. This hysteresis is caused by the slow kinetics of nitrogen physisorption: (12) due to the small bottleneck in the micropores, nitrogen molecules cannot enter easily and are difficult to exit once inside; thus, an equilibrium adsorption state was not achieved for paper C1. Bulk C1, on the other hand, has a much lower adsorption capacity because the powdered sample was composed of large crystallites with a submicrometer size distribution.

Figure 3

Figure 3. Nitrogen physisorption. (a) Adsorption–desorption isotherms of coated paper (circles), uncoated paper (triangles), and bulk C1 (squares). The volume of the adsorbate (nitrogen) adsorbed at standard temperature and pressure is denoted by V, the equilibrium pressure of the adsorbate is denoted by P, and the saturated pressure is denoted by P0. The filled and open symbols represent the adsorption and desorption processes, respectively. (b) BET plots fitted with linear functions, the slopes of which yield the SSA.

The specific surface area (SSA) and pore size were determined from the plot in Figure 3b using the Brunauer–Emmett–Teller (BET) theory. The SSA increased from 0.55 m2 for pristine paper to at least 4.3 m2 for paper C1 per unit volume of cubic centimeters; however, because an equilibrium state was not reached during the experiments, the actual SSA value of paper C1 must be significantly larger. The total volume and average diameter of pores in paper C1 (pristine paper) were determined to be 0.004 (0.007) cm3/g and 3.9 (23.1) nm, respectively; these values of pristine paper are in good agreement with those of dried cellulose. (13)

3.2. Anatase Nanoparticles

Figure 2 illustrates the powder XRD pattern of bulk C1 with a shoulder on the high-angle side of the high-angle peak. At similar diffraction angles, the shoulder grows with the increasing TPT content, suggesting that Ti compounds are responsible for its formation. The diffraction angle is identical to that of the main 1 0 1 peak for crystalline anatase TiO2 but not to those of rutile and brookite. The observed broadening indicates either a small particle size or a crystal structure that is highly disordered. Indeed, anatase nanoparticles prepared previously exhibited a single broad peak at ∼25°. (14,15) On the other hand, the XRD pattern of sample E obtained via hydrolysis of TPT under similar conditions in Figure 2 resembles that of anatase in the bulk, indicating the formation of larger crystallites with improved crystallinity, as previously observed. (14) Thus, under the mild reaction conditions used in the present study, TPT in the coating liquid may have been converted to anatase nanoparticles.
We used TEM to observe bulk C5 to confirm the presence of anatase nanoparticles and to investigate their size, dispersity, and distribution within the matrix. As shown in Figure 4, dark circular spots with a diameter of ∼2 nm are embedded in the granular contrast of the matrix. The dark contrast should be due to Ti atoms having a greater mass than that of Si atoms, while the granular contrast should be due to the amorphous structure of Si–O compounds. The enlarged photographs in Figure 4b,c show lattice images of anatase’s tetragonal structure. Therefore, anatase nanoparticles form and disperse uniformly throughout the silica–resin glass matrix. The diameter of the nanoparticles is always ∼2 nm, indicating a good dispersity. In comparison, as shown in Figure 4d, sample E from TPT hydrolysis contains well-crystallized anatase particles with extended (1 0 1) lattice fringes.

Figure 4

Figure 4. TEM images from bulk C5 and sample E. For bulk C5, a thin section of the fragment in (a) was observed at high magnification, as shown in (b,c). The image in sample E depicts densely packed and well-crystalized anatase nanoparticles (d). The lattice images in (c,d) with spacings of 0.35, 0.26, and 0.22 nm correspond to the anatase (1 0 1), (1 0 3), and (0 0 4)/(1 1 2) lattice planes, respectively. Insets show ED patterns of a holo pattern from an amorphous material in (b) and Debye rings from a crystalline material in (d).

The XANES spectra of bulk C1 and paper C1 are nearly identical to each other and are closer to the standard anatase spectrum than the rutile and brookite spectra (Figure 5; Supporting Information 5). On the other hand, in the pre-edge spectra below ∼4.98 keV, the A2 peak is significantly enhanced in the C1 samples compared with the A1 and A3 peaks. (14−17) It is established that the A2 component increases sensitively with the increasing structural disorder, such as a lower Ti coordination number, as well as with the decreasing particle size. (14,16,17) The observed increase in A2 is even greater than that previously reported for anatase nanoparticles prepared using the standard sol–gel method, and their shapes resemble those previously reported for 2 nm size “amorphous” TiO2 particles prepared in a specific way at 0 °C by Zhang et al. (15)

Figure 5

Figure 5. XANES spectra of bulk C1, paper C1, and bulk E. For comparison, the spectra of the standard anatase, rutile, and brookite samples measured in the same experimental setup are also included. The inset enlarges the pre-edge region to demonstrate the presence of disordered anatase nanoparticles in both bulk C1 and paper C1.

Therefore, we conclude that the TPT in the coating liquid resulted in highly disordered anatase nanoparticles. It is unknown why such amorphous-like anatase particles with a diameter of 2 nm form during our coating process. Perhaps the silane compounds play a role in the production. We hypothesize that hydrolyzed TPT is incorporated into the siloxane network during the initial reaction while it is still loose and that the Ti atom is discharged from the network as the reaction proceeds because Ti does not prefer the tetrahedral coordination of Si and instead prefers an octahedral coordination, as realized in anatase. As a result of the mild and slow reaction conditions, the Ti atoms aggregate to form anatase nanoparticles with a high degree of structural disorder that are embedded in the silica–resin network.

3.3. Photocatalytic Activity

MB degradation is frequently used to determine the photocatalytic activity of TiO2 and other semiconductors. (18−21) When a portion of the methyl groups are degraded by the catalytic reaction of TiO2, a hypochromic shift occurs, and the blue color of MB solutions becomes weaker. Finally, MB oxidizes to form water, carbon dioxide, and other inorganic molecules. (20)
We analyzed two samples. As shown in Figure 6, one is a film deposited on a glass substrate from coating liquid C1, and the other is paper C1. After 48 h, a significant difference is observed for C1 on glass: compared to a slight decrease for uncoated glass, the MB concentration becomes 32 and 1.6% of the starting composition of 10 μmol L–1 for coated glasses in the dark and in the light under UV illumination, respectively. The former reduction occurs as a result of adsorption onto a porous film, while the latter involves an additional photocatalytic reaction. Within a 3 h period, the variations are nearly linear in time, as illustrated in Figure 6b. The coefficients are obtained by fitting the data to the linear form: −3.74(3) and −9.35(2) nmol L–1 min–1, respectively, for dark and light conditions. The photodegradation index calculated as the difference between them is 5.6 nmol L–1 min–1, which is almost equal to the photocatalytic activity criteria of 5 nmol L–1 min–1 established by the Photocatalysis Industry Association of Japan (PIAJ). (22) Thus, our coating exhibits a moderate photocatalytic activity due to the presence of anatase nanoparticles; we did not observe a complete decomposition of MB.

Figure 6

Figure 6. Photocatalytic activity of the silica–resin coating. Time evolutions of the MB concentration in a C1 film on glass (a and b) and in paper C1 (b) are shown. The terms “dark” and “light” refer to measurements obtained in the dark and under 1 mW cm–2 UV light, respectively, while “blank” refers to a measurement obtained under UV light for uncoated glass. The lines serve as guides for the viewer’s eye. Another set of initial measurements for paper C1 are also plotted in (b). The green crosses represent data for uncoated blank paper exposed to UV light. The lines drawn on the “dark” and “light” data for C1 on glass are linear fits.

Paper C1 exhibits larger initial reductions than the C1 film on glass, as plotted in Figure 6b. This is probably because of the enhanced adsorption to the porous film produced on the cellulose fibers of paper, as demonstrated by nitrogen adsorption experiments; the coated film on paper has a higher porosity than on glass. The difference between the dark and light curves is comparable to that of C1 on glass, indicating a similar photocatalytic activity, irrespective of the kind of the substrate. Note that the porous structure of the silica–resin matrix is advantageous for applications because it can capture pollutant molecules and keep them for a long time until they are degraded by the embedded TiO2 nanoparticles.

3.4. Antibiotic Susceptibility

The photochemical sterilization of microbial cells using TiO2 has been extensively studied. (9,10,23,24)Figure 7 illustrates the results of the antibacterial performance evaluation on our samples. After 8 h on uncoated paper (ref), the number of colonies of S. aureus increased from 9000 to 83,000 and 22,000 cfu in the dark and light, respectively; the mild UV light utilized (0.25 mW cm–2), which approximates the brightness near a window during the day, was insufficient to kill them. By comparison, significant reductions in colony numbers were observed for coated paper: the colony number decreased by 1 order of magnitude in the dark and by 2 orders of magnitude in the light; for paper C1, the number decreased from 9000 to 3000 and 80 cfu, respectively, in the dark and light. As a result, the coated paper is extremely antibiotic-resistant.

Figure 7

Figure 7. Antibiotic activity of the silica–resin coating. Evolution of the viable cell count (colony forming unit: cfu) for S. aureus in 50 × 50 mm2 papers; uncoated paper (ref) and coated papers D and C1 after 8 h in darkness and light. Paper D was prepared with liquid D composed mainly of tetraethyl orthosilicate (Supporting Information 2).

The significant increase in activity when exposed to UV light indicates that the photocatalytic activity of the anatase nanoparticles in the covering film is critical for sterilization. The antibacterial activity value, SL, which is the standard index for determining antibiotic susceptibility (Supporting Information 6), is 2.4 (2.3) for paper C1 (D), which is greater than the PIAJ-defined threshold value of 2.0 for efficient photocatalytic activity but much less than the SL > 20 determined for efficient TiO2-based photocatalysts. (22) On the other hand, the light irradiation efficiency ΔS of paper C1 (D) is estimated to be 0.4 (0.9). Furthermore, these ΔS values exceed the PIAJ threshold value of 0.3. (22) Therefore, our silica–resin coating exhibits moderate photocatalytic activity, not a strong one as in conventional photocatalysts.

3.5. Performance of the Silica–Resin-Coated Paper

Our silica–resin coating film does not display a high photocatalytic effect, in part due to the low concentration of TiO2: the resulting TiO2 amounts only to 9.3 mg in the 50 × 50 mm2 paper used for the antibiotic test. The effect, however, is expected to last a long time due to the chemical and mechanical stability of the matrix silica coating, as well as its affinity for the substrate. In addition, the superior adsorptive property of the silica–resin film, owing to its porous structure, is advantageous for organic pollutant removal, and the persistence of the mild photocatalytic effect allows the decomposition reaction to proceed slowly. As a result, the substrate is protected for an extended period. Furthermore, the coated paper will be used as an organic pollutant remover that can be disposed harmlessly in nature after use.
The majority of commercially available photocatalytic materials are composed of anatase TiO2 nanoparticles. (25) For practical applications, a dispersant is required to keep them from aggregating. Additionally, a binder is required to adhere the TiO2 nanoparticles to the substrate surface, and an interfacial layer must be formed to prevent the substrate from decomposing due to the photocatalytic effect. However, because of TiO2’s overwhelming photocatalytic action, it is usually difficult to completely prevent the decomposition of these extra constituents, resulting in instability. Another issue is the high cost of manufacturing binders and interface layers. In stark contrast, the present coating enables the self-organization of a persistent protective film containing anatase nanoparticles with mild photocatalytic activity merely by applying a coating liquid. We believe that the genuine benefit of the photocatalytic effect stems from its protective function in a mild environment, not from its quick breakdown activity. Our silica–resin coating is well-suited for long-term use.
Our silica–resin coating technique is likely to find a wide range of applications. For instance, coated paper would provide waterproof and antimicrobial cutlery that is readily disposed of without causing environmental harm. A recent study demonstrated the formation of a protective silica–resin film containing an antimicrobial agent such as hinokitiol on the surface of nonwoven fabric used in medical masks. (26) This protective coating was found to have an excellent antimicrobial effect. We believe that our silica–resin coating technology can be applied to a wide variety of products, from everyday necessities to industrial products, to assist in the transition to a more sustainable and safe society through the use of paper or other materials rather than plastics.

4. Conclusions

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We report a novel silica–resin coating technique for paper that can change paper to plastic using a simple method at a low cost. The thus-obtained organic–inorganic hybrid materials can replace many plastic products and are easily decomposed in the natural environment without causing pollution. This technique will provide us with a breakthrough to solve the existing environmental problems.

Supporting Information

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The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.iecr.2c00784.

  • Titanium dioxides and its photocatalytic activity, coating agents and sample preparation, characterization techniques, XRD results, XANES spectra, antibiotic susceptibility, and references (PDF)

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Most electronic Supporting Information files are available without a subscription to ACS Web Editions. Such files may be downloaded by article for research use (if there is a public use license linked to the relevant article, that license may permit other uses). Permission may be obtained from ACS for other uses through requests via the RightsLink permission system: http://pubs.acs.org/page/copyright/permissions.html.

Author Information

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  • Corresponding Author
  • Authors
    • Yoko Iwamiya - Choetsu Kaken Co., Ltd., Suehiro, Tsurumi, Yokohama, Kanagawa 230-0045, Japan
    • Daisuke Nishio-Hamane - Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan
    • Kazuhiro Akutsu-Suyama - Neutron Science and Technology Center, Comprehensive Research Organization for Science and Society, Tokai, Ibaraki 319-1106, JapanOrcidhttps://orcid.org/0000-0002-4797-6604
    • Hiroshi Arima-Osonoi - Neutron Science and Technology Center, Comprehensive Research Organization for Science and Society, Tokai, Ibaraki 319-1106, Japan
    • Mitsuhiro Shibayama - Neutron Science and Technology Center, Comprehensive Research Organization for Science and Society, Tokai, Ibaraki 319-1106, JapanOrcidhttps://orcid.org/0000-0002-8683-5070
  • Author Contributions

    Y.I. conceived the project and conducted the design. D.N.-H. performed the XRD and SEM measurements. K.A.-S. and H.A.-O. performed nitrogen absorption and XANES experiments. Y.I., M.S., and Z.H. carried out the data analysis. All authors contributed to the manuscript preparation and discussion.

  • Notes
    The authors declare no competing financial interest.

Acknowledgments

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The authors are also grateful to K. Satomura, R. Hoshino, and R. Iwamiya for their helpful comments; T. Muroi, A. Fukui, and D. Hirai for their assistance in the XRD measurements; D. Aoki and Y. Akutsu for their assistance in the MB and antibiotic experiments; and K. Itoh and S. Takada for their assistance in the nitrogen adsorption measurements. They also thank M. Mochida and K. Taba for their help in improving the visual picture. The nitrogen adsorption measurements were conducted at the J-PARC center. The XANES experiments were conducted at the BL5S1 beamline of the Aichi Synchrotron Radiation Center, Aichi Science & Technology Foundation, Aichi, Japan (proposal no. 202104025). The sample preparation for the XANES experiments was conducted at the User Experiment Preparation Lab III operated by the Comprehensive Research Organization for Science and Society (CROSS).

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Industrial & Engineering Chemistry Research

Cite this: Ind. Eng. Chem. Res. 2022, 61, 20, 6967–6972
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  • Abstract

    Figure 1

    Figure 1. Silica–resin coating on cellulose fibers. (a) SEM image (left top) illustrates the morphology of paper composed of intertwined cellulose fibers that are a few tens of micrometers in diameter. The fibers’ edges appear relatively bright because of the enhanced backscattering of secondary electrons from Si, which is heavier than carbon, cellulose’s primary component. The corresponding elemental maps for carbon, silicon, and titanium, which were obtained using the energy-dispersive X-ray analysis, demonstrate the formation of a silica layer on the cellulose fibers: the brighter the image, the higher the concentration. Note that a trace of titanium is concentrated around the surface layer. (b) Water resistance demonstration: after 2 weeks in water at room temperature, an origami crane made of silica–resin-coated Japanese paper retained its shape (main panel), but an origami crane made of uncoated Japanese paper lost its shape after 24 h (inset).

    Figure 2

    Figure 2. Powder XRD patterns of a C1 bulk sample and of C2, C5, and C10 bulk samples with increasing TPT concentrations in coating liquids. The pattern of sample E obtained via the hydrolysis of TPT is also shown. The patterns are vertically offset for clarity. The arrow and vertical broken line indicate the location of the anatase 1 0 1 diffraction peak at 25.4°.

    Figure 3

    Figure 3. Nitrogen physisorption. (a) Adsorption–desorption isotherms of coated paper (circles), uncoated paper (triangles), and bulk C1 (squares). The volume of the adsorbate (nitrogen) adsorbed at standard temperature and pressure is denoted by V, the equilibrium pressure of the adsorbate is denoted by P, and the saturated pressure is denoted by P0. The filled and open symbols represent the adsorption and desorption processes, respectively. (b) BET plots fitted with linear functions, the slopes of which yield the SSA.

    Figure 4

    Figure 4. TEM images from bulk C5 and sample E. For bulk C5, a thin section of the fragment in (a) was observed at high magnification, as shown in (b,c). The image in sample E depicts densely packed and well-crystalized anatase nanoparticles (d). The lattice images in (c,d) with spacings of 0.35, 0.26, and 0.22 nm correspond to the anatase (1 0 1), (1 0 3), and (0 0 4)/(1 1 2) lattice planes, respectively. Insets show ED patterns of a holo pattern from an amorphous material in (b) and Debye rings from a crystalline material in (d).

    Figure 5

    Figure 5. XANES spectra of bulk C1, paper C1, and bulk E. For comparison, the spectra of the standard anatase, rutile, and brookite samples measured in the same experimental setup are also included. The inset enlarges the pre-edge region to demonstrate the presence of disordered anatase nanoparticles in both bulk C1 and paper C1.

    Figure 6

    Figure 6. Photocatalytic activity of the silica–resin coating. Time evolutions of the MB concentration in a C1 film on glass (a and b) and in paper C1 (b) are shown. The terms “dark” and “light” refer to measurements obtained in the dark and under 1 mW cm–2 UV light, respectively, while “blank” refers to a measurement obtained under UV light for uncoated glass. The lines serve as guides for the viewer’s eye. Another set of initial measurements for paper C1 are also plotted in (b). The green crosses represent data for uncoated blank paper exposed to UV light. The lines drawn on the “dark” and “light” data for C1 on glass are linear fits.

    Figure 7

    Figure 7. Antibiotic activity of the silica–resin coating. Evolution of the viable cell count (colony forming unit: cfu) for S. aureus in 50 × 50 mm2 papers; uncoated paper (ref) and coated papers D and C1 after 8 h in darkness and light. Paper D was prepared with liquid D composed mainly of tetraethyl orthosilicate (Supporting Information 2).

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  • Supporting Information

    Supporting Information


    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.iecr.2c00784.

    • Titanium dioxides and its photocatalytic activity, coating agents and sample preparation, characterization techniques, XRD results, XANES spectra, antibiotic susceptibility, and references (PDF)


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