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Article

Plasmon Sensitized Heterojunction 2D Ultrathin Ag/AgI-δ-Bi2O3 for Enhanced Photocatalytic Nitrogen Fixation

by
Xiaoming Gao
*,
Yanyan Shang
,
Kailong Gao
and
Feng Fu
*
Department of Chemistry and Chemical Engineering, Shaanxi Key Laboratory of Chemical Reaction Engineering, Yan’an University, Yanan 716000, China
*
Authors to whom correspondence should be addressed.
Nanomaterials 2019, 9(5), 781; https://doi.org/10.3390/nano9050781
Submission received: 11 April 2019 / Revised: 10 May 2019 / Accepted: 12 May 2019 / Published: 22 May 2019
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Abstract

:
A novel 2D ultrathin Ag/AgI-δ-Bi2O3 photocatalyst was constructed by a facile hydrothermal and in situ photodeposition method, which presented a uniform nanosheet structure with an average height of 6 nm. Its composition, morphology and light-harvesting properties were characterized by X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM), transmission electron microscopy (TEM), UV–vis spectrophotometer (UV–vis) and photoluminescence (PL) measurements in detail. The Ag/AgI-δ-Bi2O3 nanocomposites showed an excellent photocatalytic nitrogen fixation performance of 420 μmol L−1 g−1 h−1 in water without any sacrificial agent. The introduction of Ag/AgI nanoparticles caused the morphology modification of δ-Bi2O3, a higher concentration of oxygen vacancy, and the construction of a plasmon sensitized heterojunction, resulting in enhanced light absorption, improved separation efficiency of charge carriers and strong N2 absorption and activation ability, which are responsible for the superior photocatalytic performance of Ag/AgI-δ-Bi2O3.

1. Introduction

Ammonia (NH3) is one of the most important chemical products due to its role in natural biological processes as a hydrogen carrier and for the synthesis of many nitrogenous compounds [1]. The traditional artificial ammonia synthesis is accomplished by the Haber–Bosch process using N2 and H2, which operates at high temperatures and high pressures with high energy input and a high demand for H2, producing a serious environmental impact [2]. Therefore, it is highly desirable to realize nitrogen fixation under a mild, cost-effective, and environmentally friendly method.
In recent years, photocatalytic N2 fixation driven by solar energy has attracted considerable attention because it uses earth-abundant water as a reductant and can be conducted at atmospheric pressure and room temperature [3,4]. Therefore, a series of materials, namely, g-C3N4, MoO3−x, TiO2, Ni2P/Cd0.5Zn0.5S, BiOCl, BiOBr, and Bi5O7Br, have been developed for photocatalytic N2 fixation [4,5,6,7,8,9,10,11]. Although numerous studies have been conducted, there is still a bottleneck in developing an ideal photocatalytic nitrogen fixation [5,6,12], such as (1) the indispensable provision of abundant electrons due to six electrons being used for the reduction of one molecule of N2, (2) the need to provide higher energy to activate and cleave the triple bond owing to the presence of stable nitrogen molecules, and (3) the necessary requirement of N2 adsorption for photocatalytic nitrogen fixation [8,9,11,13,14]. Hence, in order to solve these problems and obtain higher performance of photocatalytic nitrogen fixation, the core issues remain focused on photocatalyst design. As one of the attractive inorganic materials, the p-type Bismuth oxide (Bi2O3) semiconductor has been widely investigated as a promising visible light photocatalytic material with appropriate band gaps [15,16]. In particular, δ-Bi2O3 was of great interest to our research because it is much richer in anion oxygen vacancies [17,18], which may act as potential candidates for photocatalytic N2 fixation. It has been reported that the presence of oxygen vacancies can promote light harvesting and charge carrier separation efficiency, especially improving the adsorption and activation ability of N2 in the photocatalytic nitrogen fixation reaction [6,19,20]. However, δ-Bi2O3 is known to have a high-temperature stable phase of higher than 700 °C [15,17], and it is still a challenge to evolve a facile and effective strategy for the synthesis of δ-Bi2O3 with high concentrations of oxygen vacancies at a low temperature. Besides, special morphological structure control with a large surface area to provide more active sites should be considered [21]. In addition, the rational construction of a nano-heterojunction is also a feasible route for enhancing photocatalytic performance [22,23]. Recently, the new plasmon resonance photocatalyst silver/silver halides (Ag/AgX, X = Cl, Br, I) attracted much attention when combined with other semiconductor photocatalytic materials, because Ag/AgX hybrid materials dramatically increase visible light utilization and promote photogenerated charge separation [24,25,26]. Simultaneously, Ag/AgX semiconductor materials exhibit aexcellent photocatalytic activity owing to the localized surface plasmon resonance (LSPR) effect, which is described as the resonant photon-induced collective oscillation of valence electrons when the frequency of photons matches the natural frequency of surface electrons oscillating against the restoring force of the positive nuclei [27,28]. So, the combination of δ-Bi2O3 and Ag/AgX composites could provide new opportunities for developing highly efficient visible-light driven nitrogen fixation photocatalysts due to the LSPR effect and the heterostructure. Up until now, there have been few reports on photocatalytic N2 fixation application by δ-Bi2O3 based photocatalysts with well-designed morphology and heterojunction structure.
In this work, we developed a facile hydrothermal method to synthesize δ-Bi2O3 microcrystals at a low temperature, and a Ag/AgI-δ-Bi2O3 photocatalyst was further prepared via a precipitation and photoreduction route, which was then used as the photocatalyst for nitrogen fixation which achieved remarkably improved N2 photoconversion activity compared to that of a pure δ-Bi2O3 photocatalyst. Meanwhile, the influences of the ultrathin nanosheets structure of the δ-Bi2O3 and Ag/AgI combination on photocatalytic activity were systematically discussed. The mechanism of photocatalytic nitrogen fixation of the Ag/AgI-δ-Bi2O3 photocatalyst was also proposed according to the results of systematic analysis, such as photoluminescence (PL), alternating current (AC) impedance, photocurrent response, and fluorescence life and DMPO (5,5-dimethyl-1-pyrroline-N-oxide)–electron spin resonance (ESR).

2. Experimental Section

2.1. Synthesis of Photocatalysts

A total of 0.4851 g Bi(NO3)3·5H2O was dissolved in a mixed solution containing 8 mL ethylene glycol and 32 mL tert-butyl alcohol, followed by vigorous stirring. Subsequently, the mixture solution was put into a Teflon-lined stainless steel autoclave with a capacity of 50 mL. The autoclave was heated and maintained at 160 °C for 8 h, cooled to room temperature, and dried in a vacuum at 80 °C for 48 h. The mixture solution was formed by adding 0.466 g of δ-Bi2O3, 0.2 mL (0.5 mL, 1 mL, 3 mL, 5 mL) AgNO3 solution (0.01 mol/L), and 0.1 mL (0.25 mL, 0.5 mL, 1.5 mL, 2.5 mL) KI solution (0.01 mol/L) into deionized water. Afterwards, the above solution was stirred for 1 h and then illuminated by 400 W gold halide lamp for 2 h. Then, the samples were washed by deionized water and dried in a vacuum at 80 °C for 48 h. The as-prepared samples were named Ag/AgI–BiO-1, Ag/AgI–BiO-2, Ag/AgI–BiO-3, Ag/AgI–BiO-4, and Ag/AgI–BiO-5 (0.2%Ag/AgI-δ-Bi2O3, 0.5%Ag/AgI-δ-Bi2O3, 1%Ag/AgI-δ-Bi2O3, 3%Ag/AgI-δ-Bi2O3, and 5%Ag/AgI-δ-Bi2O3), respectively.

2.2. Characterization

The composition and crystal phase of the samples was identified by 7000 powder X-ray diffraction (Shimadzu, Tokyo, Japan) using an X-ray diffractometer with Cu-Kα radiation under 40 kV and 30 mA. The X-ray photoelectron spectroscopy of the as-prepared samples was performed on an ESCALAB 250 Xi X-ray photoelectron spectrometer (ThermoScientific, Waltham, MA, USA). The morphologies of the samples were shown on a JSM-6700F scanning electron microscope (JEOL, Tokyo, Japan). The determination of element composition was measured using an energy dispersive spectrometer (Bruker, Bremen, Germany). High-resolution transmission electron images of the as-prepared samples were measured on a JEM-2100 electron microscope (JEOL, Tokyo, Japan). The ultrathin structure of the as-prepared sample was determined by Cypher S atomic force microscopy (Oxford, UK). The UV–vis diffuse reflectance spectroscopy (DRS) was measured by a UV–2550 spectrophotometer (Shimadzu, Tokyo, Japan) with BaSO4 as a reference. The photo–electro–chemical properties of the samples were collected on a CHI660D electrochemical workstation (Chenhua, Shanghai, China). An F-4500 fluorescence spectrograph (Hitachi, Tokyo, Japan) was used to analyze the fluorescence spectra of samples. The Brunauer–Emmett–Teller specific surface area was analyzed by a V-Sorb2800P analyzer using adsorption and desorption of N2, and N2 temperature-programmed desorption (TPD) was performed by 3 Flex Chemi instrument (Micromeritics, Norcross, GA, USA). The electron paramagnetic resonance (EPR) spectra of the samples were determined with an ES-ED3X Endor spectrometer (JEOL, Tokyo, Japan).

2.3. Photocatalytic Reaction

Photocatalytic nitrogen fixation experiments were carried out on a quartz glass photochemical reactor under the irradiation of a 400 W xenon lamp with a 420 nm cutoff filter. A total of 0.2 g photocatalyst was dispersed in 200 mL of deionized water, and nitrogen flow was kept bubbling through the solution at a rate of 10 mL/min. Before irradiation, the mixture solution was stirred constantly in the dark for 30 min. Then, 5 mL of aqueous solution was taken out after 30 min, and the NH4+ concentration was determined by a Metrohm 833 Ions Chromatography (Herisau, Switzerland).

3. Results and Discussion

The phase structure of the as-prepared samples was characterized by the XRD. As shown in Figure 1a, the diffraction peaks located at 28.0°, 32.3°, 46.3°, and 55°, corresponded to the crystal planes of (111), (200), (220), and (311), and can be indexed to the cubic planes of δ-Bi2O3 (JCPDS No. 27-0052, Pn3m (224), a = b = c = 5.525 Å). The diffraction peaks located at 25.35°, 32.76°, and 39.20°, corresponded to the crystal planes of (101), (102) and (110), and can be assigned to β-AgI (JCPDS No.09–0374). As far as Ag/AgI–BiO-3, Ag/AgI–BiO-4 and Ag/AgI–BiO-5 are concerned, there were two main diffraction peaks at 38.12° and 44.28°, corresponding to the crystal planes of (111) and (220) of Ag (JCPDS No.04–0783). It is implied that Ag deposited on the surface of BiO can be detected from the added content of Ag. From the unit cell parameter of the as-prepared samples (Table 1), the cell volume of Ag/AgI–BiO changed slightly in comparison with BiO, indicating that the Ag/AgI deposited was only deposited on the surface of BiO, and did not change the original lattice of δ-Bi2O3. The surface chemical composition of the as-prepared sample was measured by X-ray photoelectron spectroscopy (XPS). As shown in the survey spectra of Ag/AgI–BiO-4 (Figure 1b), the sample was composed of Bi, O, Ag, and I, which confirmed the chemical composition of the as-prepared sample. From the narrow spectrum of the Bi element (Figure 1c), there were two peaks at 159.2 and 164.7 eV, ascribed to the characteristic peaks of Bi4f7/2 and Bi 4f5/2, respectively, which indicated that Bi existed in the as-prepared sample in the form of Bi3+. Two obvious characteristic peaks at 529.7 and 532.8 eV were observed in the narrow spectrum of the O element (Figure 1d), which corresponded to the Bi–O band and the absorbed O2 or H–O bond, respectively. From Figure 1e, the two characteristic peaks that appeared in the 368.2 and 374.2 eV corresponded to the Ag 3d5/2 and Ag 3d3/2, indicating the existence of Ag+; meanwhile, the characteristic peaks that appeared at 367.2 and 373.2 eV showed the presence of Ag0 on the surface of the sample. The peaks at 619.3 and 630.9 eV can be assigned to the characteristic peaks of I3d5/2 and I3d3/2 (Figure 1f). An energy dispersive spectrometer (EDS) result indicated that the elements of Bi, O, Ag, and I were well distributed on the surface of the photocatalyst (Figure 2).
The morphology and microstructure of pure δ-Bi2O3 and Ag/AgI–BiO-4 were observed by scanning electron microscopy (SEM) and transmission electron microscopy (TEM). As presented in Figure 3a,b, the pure δ-Bi2O3 (without modification) displayed a microsphere hierarchically structure, which was built from numerous pliable nanosheets aligned to the spherical surface. However, it was observed that the structure of δ-Bi2O3 turned into an ultrathin two-dimension layered nanosheet morphology after the deposition of Ag/AgI nanoparticles by mild precipitation and photoreduction reaction processes (as shown in Figure 3c,d). This remarkable change may be achieved by the photo-assisted Ag exfoliation effect [29]. In such a specific structure, the multilayer nanosheets do not only provide more exposure space for photocatalytic reaction but can also promote the photogenerated electron transport within the photocatalyst. The photogenerated carriers are more easily transported to the surface of the photocatalyst to participate in chemical reactions after irradiation, thus further reducing the recombination rate of photogenerated electrons and holes. However, the Ag/AgI nanoparticles failed to be observed in SEM images due to their small size and content. More detailed structural information of the Ag/AgI–BiO-4 composite was further revealed by TEM images, as presented in Figure 3e,f, where Ag/AgI–BiO-4 presented as a 2D ultrathin nanosheet structure with a size of hundreds nanometers, and many small nanoparticles of about several nanometers corresponding to Ag and AgI were deposited on the surface of the δ-Bi2O3 nanosheet. From the high resolution transmission electron microscopy (HR–TEM) of Ag/AgI–BiO-4 (Figure 3g), clear lattices with spaces of 0.35 nm, corresponding to the (111) facets of δ-Bi2O3 and the deposited phase of Ag/AgI, were observed clearly.
Furthermore, the height of the single nanosheet was observed by atom force microscopy (AFM), as shown in Figure 4, where the average height of the single nanosheet was approximately 6 nm. However, a thickness of about 12 nm was also found, which implied the stacking of two single nanosheets. Generally, the especially ultrathin nanosheets and nanoparticle (<10 nm) structures of the Ag/AgI–BiO composite display unusual physical and chemical properties due to prominent quantum surface effects and distinct electronic structures.
The light absorption and optical response range of the as-prepared samples was investigated by the UV–vis DRS. As shown in Figure 5a, all of the as-prepared samples had evident absorption from the UV to visible range. In comparison with BiO, the red shift was not obvious for Ag/AgI deposited BiO, but the as-prepared Ag/AgI–BiO samples appeared to have obvious enhancement of visible light absorption, which is mainly attributed to the strong surface plasmon resonance of Ag nanocrystals and the synergistic effect between Ag/AgI and δ-Bi2O3 [24,30], resulting in better visible light utilization. The recombination efficiency of the photogenerated carriers of the as-prepared samples was investigated by photoluminescence spectroscopy. From Figure 5b, the fluorescence emission intensity of Ag/AgI–BiO was lower than that of pure BiO, indicating that the deposition of Ag/AgI can obviously reduce the recombination rate of the photogenerated carriers. In comparison with the Ag/AgI–BiO, Ag/AgI–BiO-4 and Ag/AgI–BiO-5 have nearly the same lowest fluorescence emission intensity, indicating that the energy loss of the recombination of the photogenerated carriers is weak. The transmission speed of the photogenerated carrier of the catalysts was measured by the electrochemical impedance spectroscopy, which reflected the charge transfer resistance between the solid interface and surface, and the smaller the arc radius of the Nyquist spectra of electrochemical impedance, the easier the separation of the photogenerated carrier. As shown in Figure 5c, the electrochemical impedance spectrum of Ag/AgI–BiO-4 had the lowest arc radius, which implies a faster transmission speed and a more efficient separation for the interfacial transfer of the photogenerated carrier. The photocurrent density can be used to explain the separation efficiency of the photogenerated carrier. As shown in Figure 5d, the transient photocurrent of the as-prepared samples presented stable cycles with a light on or off. The BiO had a weaker light current response of 0.11 μA cm−1, and the Ag/AgI–BiO-4 owned the largest photocurrent density, which was about 3.74 μA cm−1. The significantly enhanced photocurrent density implies the significant improvement of separation efficiency of the photogenerated carriers. The fluorescence lifetime of the photogenerated carriers of the as-prepared samples was measured by time-resolved fluorescence spectroscopy. As shown in Table 2, the fitting factor χ2 was close to 1. The fluorescence life of BiO was 0.192 ns, which was shorter than that of Ag/AgI–BiO. Especially, Ag/AgI–BiO-4 possessed the longest fluorescence life of 0.765 ns. The prolonged fluorescence lifetime indicates a slow recombination rate of the photogenerated carriers.
The photocatalytic nitrogen fixation efficiencies were tested using water as the proton source without any scavenger under light irradiation. As shown in Figure 6, under normal temperature and atmospheric pressure conditions, the NH4+ in water was almost undetectable under light irradiation and bubbling nitrogen. However, all samples exhibited a near linear increase of nitrogen fixation performance over the entire reaction time under light irradiation, suggesting good stability during the photocatalytic N2 fixation process. After visible light irradiation for 3 h in the case of pure BiO, the NH4+ concentration in water was about 64 μmol/L (Figure 6a), and the NH4 fixation rate was 107 μmol L−1 g−1 h−1 (Figure 6b). In comparison, a significant improvement in the photocatalytic nitrogen fixation activities was observed with the addition of Ag/AgI, and the Ag/AgI–BiO-4 nanocomposite exhibited the highest nitrogen fixation rate of 420 μmol L−1 g−1 h−1, with the corresponding amount of NH4+ reaching 250 μmol/L, which was four times higher than that of BiO. The apparent quantum efficiency (AQE) was measured under the same reaction conditions except in incident light, which is 420 nm monochromatic light. The NH3 amount was measured after 1 h of irradiation, and the AQE calculated as the reference [4,9]. The AQE of Ag/AgI–BiO-4 (4.1%) was approximately two times than that of BiO (2.0%). This enhancement in the nitrogen fixation rate can be attributed to the two-dimensional ultrathin nanosheet morphology of Ag/AgI–BiO with its higher specific surface area and more active sites for promoting surface nitrogen fixation kinetics. Meanwhile, as characterized in UV–vis and photoelectrochemical tests, the enhanced light harvesting capacity and the improved carrier separation efficiency caused by the introduction of Ag/AgI are important reasons for enhanced photocatalytic performance. In addition, the recycle experiments for photocatalytic nitrogen fixation were carried out, and the results are shown in Figure 6c. After being used five times, the NH4+ concentration over Ag/AgI–BiO-4 was virtually identical, which indicates that the catalyst can be continuously applied in photocatalytic N2 fixation.
Furthermore, EPR was performed to analyze the concentration of oxygen vacancies in the photocatalysts. As shown in Figure 7a, two obviously symmetrical EPR signals at the g value of 2.00 were observed, which were identified as the electrons trapped on the oxygen vacancies [31,32]. It was observed that the EPR intensity of Ag/AgI–BiO-4 was significantly stronger than that of BiO, which demonstrated a higher surface oxygen vacancy concentration for Ag/AgI–BiO-4. This phenomenon probably occurs because of the morphological modification of the δ-Bi2O3 ultrathin nanosheet with more exposed surfaces owing to the photo-assisted Ag exfoliation effect. Besides, it is known that the oxygen vacancies can promote the adsorption and activation of N2 in a more feasible pathway, so N2-TPD was carried out to understand the N2 chemical adsorption on the surface of photocatalysts. As shown in Figure 7b, the two desorption peaks at 242 and 328 °C corresponded to the physical adsorption and chemical adsorption of N2, respectively, and the Ag/AgI–BiO-4 photocatalyst displayed a much higher adsorption ability compared to BiO, which is consistent with photocatalytic N2 fixation activity. These results suggest that the combination of Ag/AgI can introduce more oxygen vacancies in a catalyst system, which benefits the conversion efficiency of nitrogen photofixation.
In order to explain the photocatalytic mechanism, the energy band structures of δ-Bi2O3 and AgI were further determined by Mott–Schottky analysis and valence-band XPS spectra. The Mott–Schottky plots of δ-Bi2O3 and AgI are shown in Figure 8a. According to the intercept of the plots on the abscissa axis, the Efb vs. NHE (normal hydrogen electrode) of δ-Bi2O3 and AgI were calculated to be 2.28 and −1.07 eV, respectively. The negative slope of the δ-Bi2O3 confirmed its p-type semiconductivity, and the AgI showed an n-type semiconductor character. Besides, as it is known that the Efb is about 0.3 eV above valence-band (VB) potential for n-type semiconductor and 0.3 eV below the conduction-band (CB) potential for n-type semiconductors [33,34], we can conclude that the EVB of δ-Bi2O3 is calculated as 2.58 eV vs. NHE and that the ECB of AgI is determined as −1.37 eV vs. NHE. Additionally, as shown in Figure 8b, the band gap energy can be estimated from the intercept of the UV–vis DRS plots, which were 2.85 eV for δ-Bi2O3 and 2.79 eV for AgI, respectively. Consequently, ECB of δ-Bi2O3 can be calculated as −0.27 eV, and EVB of AgI at approximately 1.42 eV—those values agreeing with the VB XPS spectra (Figure 8c). Due to the direct contact between δ-Bi2O3 and AgI, a heterojunction with band matching can be established due to the staggered band alignment, where an electric field can form at the interface to promote the electron-hole separation and migration, which is in favor of photocatalytic N2 fixation.
Based on these results, the reasons for the enhanced photocatalytic activity and probable photogenerated charge carriers transport mechanism of the Ag/AgI–BiO nanocomposite were supposed. Due to the introduction of Ag/AgI, δ-Bi2O3 exhibited a great change in morphology as ultrathin nanosheets, which provided more reactive sites for N2 fixation. More importantly, the concentration of surface oxygen vacancies showed a significant increase to facilitate the adsorption and activation of inert N2 molecules. As shown in Figure 9, under light irradiation, electrons and holes were generated on the CB and VB of AgI and δ-Bi2O3. On account of the heterojunction characteristic and the staggered band alignment structure between δ-Bi2O3 and AgI, photoinduced holes tended to migrate from δ-Bi2O3 to AgI, and the photoexcited electrons of AgI were transferred to δ-Bi2O3 and then trapped by oxygen vacancies with a defective state. Simultaneously, the metal Ag nanoparticles absorbed photons to form free electrons with higher energy states owing to the LSPR effect, and the hot electrons migrated from Ag to δ-Bi2O3 subsequently [35]. Therefore, photogenerated electrons and holes were effectively separated. The photogenerated electrons were subsequently consumed by adsorbing N2 molecules and H+ to form NH4+, and the photogenerated holes participated in the oxidation of H2O to O2. According to the above analyses, more activated nitrogen and electrons can be supplied for the photocatalytic reaction over the Ag/AgI–BiO system, resulting in a superior photocatalytic nitrogen fixation performance.

4. Conclusions

In summary, we have developed a facile hydrothermal–photodeposition strategy to prepare 2D ultrathin Ag/AgI-δ-Bi2O3 photocatalysts with a highly efficient photocatalytic N2 fixation activity, which exhibits obviously superior photocatalytic activity with a N2 fixation rate of about 420 μmol L−1 g−1 h−1 compared with δ-Bi2O3 photocatalysts. On the basis of detailed characterizations and tests, the morphology modification of δ-Bi2O3 resulted in a bigger specific surface area and more exposed oxygen vacancies, with the enhanced photocatalytic performance of Ag/AgI-δ-Bi2O3 nanocomposite being attributed to the increased visible light absorption, the improved carrier separation efficiency forming the plasmonic effect, and the heterojunction and enhanced N2 adsorption and activation caused by oxygen vacancies. This work offers a novel approach to the design and construction of high-efficiency Bi2O3 based photocatalysts in the field of solar-driven ammonia synthesis.

Author Contributions

X.G. designed the experiments and wrote the paper; Y.S. and K.G. performed the experiments and analyzed the data, F.F. designed the experiments.

Funding

This research was funded by the National Natural Science Foundation of China (No. 21663030) and the National Natural Science Foundation of China (No. 21766039).

Conflicts of Interest

The authors declare no conflict of interest.

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Nanomaterials 09 00781 g001 550
Figure 1. (a) X-ray diffraction (XRD) of as-prepared samples; (b) The survey spectra and the high-resolution X-ray photoelectron spectroscopy (XPS) spectra of Ag/AgI–BiO-4; (c) Bi 4f; (d) O1s; (e) Ag3d; (f) I3d.
Figure 1. (a) X-ray diffraction (XRD) of as-prepared samples; (b) The survey spectra and the high-resolution X-ray photoelectron spectroscopy (XPS) spectra of Ag/AgI–BiO-4; (c) Bi 4f; (d) O1s; (e) Ag3d; (f) I3d.
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Nanomaterials 09 00781 g002 550
Figure 2. (a) The scanning electron microscopy (SEM); (b) the total element distribution; and (c–f) the element distribution of Bi, O, Ag, and I of 3%Ag/AgI-δ-Bi2O3.
Figure 2. (a) The scanning electron microscopy (SEM); (b) the total element distribution; and (c–f) the element distribution of Bi, O, Ag, and I of 3%Ag/AgI-δ-Bi2O3.
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Figure 3. (a,b) The SEM images of pure δ-Bi2O3 sample, and (c,d) SEM, (e,f) transmission electron microscopy (TEM) images and (g) the high resolution TEM images of Ag/AgI–BiO-4.
Figure 3. (a,b) The SEM images of pure δ-Bi2O3 sample, and (c,d) SEM, (e,f) transmission electron microscopy (TEM) images and (g) the high resolution TEM images of Ag/AgI–BiO-4.
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Nanomaterials 09 00781 g004 550
Figure 4. (a) Atom force microscopy (AFM) image and (b) the corresponding height of Ag/AgI–BiO-4.
Figure 4. (a) Atom force microscopy (AFM) image and (b) the corresponding height of Ag/AgI–BiO-4.
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Nanomaterials 09 00781 g005 550
Figure 5. (a) The UV–vis diffuse reflectance spectroscopy (DRS) of as-prepared samples; (b) the photoluminescence (PL) of the as-prepared samples; (c) the Nyquist spectra of alternating current (AC) impedance of the as-prepared samples; (d) the photocurrent of the as-prepared samples.
Figure 5. (a) The UV–vis diffuse reflectance spectroscopy (DRS) of as-prepared samples; (b) the photoluminescence (PL) of the as-prepared samples; (c) the Nyquist spectra of alternating current (AC) impedance of the as-prepared samples; (d) the photocurrent of the as-prepared samples.
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Figure 6. (a) NH4+ concentration in water; (b) photocatalytic nitrogen fixation rate over the different catalysts; and (c) effect of recycling use of Ag/AgI–BiO-4 to the NH4+concentration in water.
Figure 6. (a) NH4+ concentration in water; (b) photocatalytic nitrogen fixation rate over the different catalysts; and (c) effect of recycling use of Ag/AgI–BiO-4 to the NH4+concentration in water.
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Figure 7. (a) Low-temperature EPR spectra and (b) the N2-TPD of Ag/AgI–BiO-4.
Figure 7. (a) Low-temperature EPR spectra and (b) the N2-TPD of Ag/AgI–BiO-4.
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Figure 8. (a) Mott–Schottky plots (b) band gap energy and (c) valence-band (VB) XPS spectra of AgI and δ-Bi2O3.
Figure 8. (a) Mott–Schottky plots (b) band gap energy and (c) valence-band (VB) XPS spectra of AgI and δ-Bi2O3.
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Nanomaterials 09 00781 g009 550
Figure 9. The possible photocatalytic degradation mechanism.
Figure 9. The possible photocatalytic degradation mechanism.
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Table
Table 1. The unit cell parameter of the as-prepared catalyst.
Table 1. The unit cell parameter of the as-prepared catalyst.
SampleUnit Cell Volume (Å3)a (Å)b (Å)c (Å)
δ-Bi2O3168.655.5255.5255.525
0.2%Ag/AgI-δ-Bi2O3168.565.5245.5245.524
0.5%Ag/AgI-δ-Bi2O3168.385.5225.5225.522
1%Ag/AgI-δ-Bi2O3168.205.5205.5205.520
3%Ag/AgI-δ-Bi2O3168.835.5275.5275.527
5%Ag/AgI-δ-Bi2O3168.925.5285.5285.528
Table
Table 2. The fluorescence life of the as-prepared samples.
Table 2. The fluorescence life of the as-prepared samples.
Sampleτ1τ2χ2τ
BiO0.1/94.931.92/5.071.1940.192
Ag/AgI–BiO-10.37/96.741.39/3.241.1290.403
Ag/AgI–BiO-20.38/94.581.47/5.421.1350.439
Ag/AgI–BiO-30.42/90.251.53/9.471.1120.524
Ag/AgI–BiO-40.57/84.531.83/15.471.0920.765
Ag/AgI–BiO-50.49/88.531.56/11.471.1040.613

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Gao, X.; Shang, Y.; Gao, K.; Fu, F. Plasmon Sensitized Heterojunction 2D Ultrathin Ag/AgI-δ-Bi2O3 for Enhanced Photocatalytic Nitrogen Fixation. Nanomaterials 2019, 9, 781. https://doi.org/10.3390/nano9050781

AMA Style

Gao X, Shang Y, Gao K, Fu F. Plasmon Sensitized Heterojunction 2D Ultrathin Ag/AgI-δ-Bi2O3 for Enhanced Photocatalytic Nitrogen Fixation. Nanomaterials. 2019; 9(5):781. https://doi.org/10.3390/nano9050781

Chicago/Turabian Style

Gao, Xiaoming, Yanyan Shang, Kailong Gao, and Feng Fu. 2019. "Plasmon Sensitized Heterojunction 2D Ultrathin Ag/AgI-δ-Bi2O3 for Enhanced Photocatalytic Nitrogen Fixation" Nanomaterials 9, no. 5: 781. https://doi.org/10.3390/nano9050781

APA Style

Gao, X., Shang, Y., Gao, K., & Fu, F. (2019). Plasmon Sensitized Heterojunction 2D Ultrathin Ag/AgI-δ-Bi2O3 for Enhanced Photocatalytic Nitrogen Fixation. Nanomaterials, 9(5), 781. https://doi.org/10.3390/nano9050781

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