photocatalytic nonadides Essay

Angewandte Chemie Photocatalyis with Visible Light Photocatalytic Nanodiodes for Visible-Light Photocatalysis** Hyun G. Kim, Pramod H. Borse, Wonyong Cho’, and S. Lee* Photocatalysts that respond to visible light (l < 400 nm) are needed to utilize the main part of the solar spectrum for production of hydrogen energy by splitting , 2] purification of water and air, [3] and other applications. [4] Traditional visible-light photocatalysts are either unstable upon illumination with light (e. . , CdS, CdSe)[5] or have low activity (e. g. , W03, Fe203). [6] Recently, some UV-active oxides functioned s visible-light photocatalysts by substitutional doping of metals (as in MTi02 (M = Fe, V, and Nixin1?…na04 reduction of Ti02 (as in -nox (x < and anton doping With N, C, and S (as TaON,[12] and Sm2Ti205S2 [13]). However, these doped materials, in general, show a small absorption in the visible-light region, leading to low activities. 14] New and more efficient visible-light photocatalysts are needed to meet the requirements of future environmental and energy technologies driven by solar energy. Herein we describe a novel configuration of composite solids designated as photocatalytic nanodiodes (PCD). These ontain nano-islands of p-type CaFe204 interfaced over a highly crystalline layered perovskite base lattice (n-type PbBi2Nb1. 9WO. 109), yielding nanodimensional p-n Junctions. Dr. H. G. Kim, Dr. P. H. Borse, Prof. W. Choi, Prof. J. S.

Lee Department of Chemical Engineering and School of Environmental Science & Engineering Pohang University of Science and Technology San-31 HyoJa-dong, Pohang 790-784 (Korea) Fax: (+ 81) 54-279-5528 E-mail: [email protected] ac. kr [**] This work was supported by the Hydrogen Energy R Center, the Research Center for Energy Conversion and Storage, the National R Center for Nano Science nd Technology, the National Research Laboratory Program, and the General Motors R Center. Supporting information for this article is available on the WWW under http:// www. ngewandte. org or from the author. Angew. Chem. Int. Ed. 2005, 44, 4585-4589 2005 Wiley-VCH veriag GmbH & co. KGaA, wetnhetm 4585 Communications This nanodiode material shows greatly enhanced and stable photocatalytic activity for degradation of toxic organic pollutants (acetaldehyde, isopropyl alcohol), oxidation of water to gaseous oxygen, and photocurrent generation, all under visible light (l > 420 nm). In the rational design of this composite material, we employed a combination of concepts that optimize the photocatalytic activity.

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It has been demonstrated in photovoltaic cells and photoelectrochemical (PEC) cells that diode structures made of n- and p-type semiconductors show greatly enhanced activities compared to devices consisting of a single semiconductor. For example, the fundamental unit of current silicon solar cells consists of p-n Junctions with p-type and ntype silicon. Multijunction solar cells and PEC cells with remarkable energy conversion efficiencies have been reported. 1 5] NoJik constructed an n-Ti02/p-GaP diode electrode for a PEC cell that was much more active than either nTi02 or p-GaP single-component electrodes for the decomposition of water. 16] He designated his monolithic device a p-n type photochemical diode. We attempted to create a particulate version of the p-n Junction on a nanometer scale for photocatalytic applications; this Junction should be stable under typical photocatalytic reaction conditions and highly active under visible light. Owing to the employment of the p-n Junction concept, the nanoscale size, and the particulate form of our device aterial, we designated it a p-n type photocatalytic nanodiode (PCD). The first step in fabricating the PCD was to select proper p- and n-type semiconductors that could absorb visible light.

We identified PbBi2Nb209 as a suitable n-type semiconductor. This material is an Aurivillius-phase layered perovskite, and is an efficient photocatalyst for the oxidation of water to 02 and the degradation of isopropyl alcohol to C02 under visible light. [17] For PbBi2Nb209 to show n-type semiconductivity, it was doped with tungsten(vi) to provide n-PbBi2Nb1. 9WO. 109. In addition to the valency, the similarity in size between wv” (0. 4 nm) and NbV (0. 78 nm) was a further consideration in our choice. For the p-type semiconductor we chose CaFe204, a metal oxide with a bulk band gap of 1. eV. [18] The material by itself shows very low photocatalytic activity under visible light. Yet, we selected it because of its p-type challenge was to combine these two semiconductor particles to form a p-n Junction. For the efficient use of such a diode structure, the interfacing area should be maximized. However, in preliminary experiments, we learned that PbBi2Nb1. 9WO. 109 must be in a highly crystalline state to obtain high activity; his requires a high-temperature synthesis that inevitably produces large particles of 0. -1 mm in diameter. We therefore devised the confguration of the diode particles as follows: 1) Nanocrystals of p-type CaFe204 and 2) a perovskite lattice of n-type PbBi2Nb1. 9WO. 109 as a submicron-sized base material. The CaFe204 nanoparticles and PbBi2Nb1. 9WO. 109 submicron particles were synthesized individually by sol-gel methods and a solid-state reaction, respectively. The individual components were then combined by placing them in a hydrothermal reactor (1 50 8C for 7 d) to form CaFe204 nano- slands over larger particles of PbBi2Nb1. WO. 109. 4586 Figure 1 . a) HRTEM image of the p-n type photocatalytic nanodiode (PCD). The magnified views show the nanocrystalline p-type CaFe204 (b) interfaced on layers of the n-type PbBi2Nb1. 9WO. 109 base Figure 1 a shows a HRTEM image ofa typical PCD particle. It clearly exhibits the existence of nano-islands dispersed over a single particle of perovskite base material. The micrograph shows many nanocrystalline islands of 5- 10 nm, and the magnified view of a nano-island reveals the nanocrystallinity of CaFe204 (Figure 1 b).

The magnified view of the fringes also emonstrates the existence of a highly crystalline, layered base material corresponding to PbBi2Nb1. 9WO. 109 (layer thickness 0. 4 nm, Figure 1 c). The phase identification was also confirmed by elemental analysis with in situ energy- dispersive X-ray microanalysis carried out during the microscopic study. Based on these experimental observations we propose a model for the PCD as illustrated in Figure 2 a. Each island forms a nanoscale p-n Junction at the interface, which plays a crucial role in the photocatalytic process.

The working principle of PND is shown as an energy band model for one p-n Junction (Figure 2 b). At thermal equilibrium, the Fermi levels of two semiconductors align. When the device is immersed in an electrolyte, the band edges of the conduction and valence bands bend as indicated. The operation of the semiconductors. Photogenerated holes and electrons separate under the influence of the electric field, corresponding to the energy diagram in Figure 2 b. Thus, Figure 2. a) Schematic drawing of a PCD.

B) Schematic drawing of the energy band model of a PCD showing the formation of the p-n Junction and the process of water oxidation. The band positions were derived from flat band potential measurements s described in the Supporting Information. CB = conduction band, VB = valence band, NHE = normal hydrogen electrode. www. angewandte. org holes move to the p-CaFe204 side, and electrons to the nPbBi2Nb1. 9WO. 109 side. The net effect of the p-n diode formation is the efficient separation of electron-hole pairs to minimize the energy-wasteful electron-hole recombination.

This effect leads to the higher photocatalytic activity. The optical properties of these compounds were probed by IJVNls diffuse reflectance spectroscopy (Figure 3 a). Then a comparison was made with the base material, PbBi2Nb209, nd nitrogen-doped Ti02, that is, Ti02?…xNx. The latter material is considered to be the standard example of a visible-light photocatalyst; the band structure of Ti02 is modified by nitrogen doping to induce absorption of visible light. [10] From these spectra, we estimated the band gap energies of these materials (Table 1).

The PCD powders showed a steep onset of absorption around I = 530 nm, corresponding to green light; the band corresponding to this onset covers a major part of the visible region, compared to the other two standards considered here. The Ti02?…xNx sample showed two absorption edges typical of doped aterials, the main edge due to the oxide at 390 nm and a shoulder due to the nitride at 451 nm. PbBi2Nb209 and the PCD showed single sharp edges. Thus, the PCD would absorb more visible-light photons than Ti02?…xNx, although their absorption edges were almost the same around 450 nm.

Both PbBi2Nb209 and Ti02?…xNx are yellow, and the PCD is orange, indicating that all these materials absorb visible light. We then examined the photocatalytic properties of these aqueous suspensions of the materials containing acetate (donor) and Fe3+ (acceptor) were illuminated with visible light (l > 420 Figure 3 b indicates that the PCD enerates a photocurrent approximately three and five times faster than PbBi2Nb209 and Ti02?…xNx, respectively. The higher activities of PCD and PbBi2Nb209 for photocurrent generation result from the beneficial effect of forming photocatalytic p-n nanodiodes.

Unmodified Ti02, with a wide band gap, as well as all catalysts in the dark did not generate a photocurrent, as expected. The generation of photoelectrons is the critical initial step of photocatalytic reactions upon absorption of light, and the rate should directly correlate with the photocatalytic activity of the material. The materials were then tested for the photooxidation of acetaldehyde, a hazardous air pollutant as well as a common model compound to test the photodegradation capability of photocatalysts.

Figure 3 c shows the time curves of C02 evolution from the reaction CH3CHO + 5/2 02 12 C02 + 2 H20. The concentration of C02 increased steadily with irradiation time at a decomposition rate of about 0. 02 mmol h?…1 under irradiation with light. The C02 production stopped when the light was turned off and resumed at the same rate when the light was turned on again. No intermediate reaction products were detected. The superiority of the PCD over PbBi2Nb209 and Ti02?…xNx, as expected from the photocurrent generation behavior, was confirmed.

Similar results were obtained for the photodecomposition of isopropyl alcohol, another common organic pollutant of air (not shown). As the final test reaction, we studied the photodecomposition of water in the presence of sacrificial agents. These Angew. Chem. Int. Ed. 2005, 44, 4585-4589 Figure 3. a) IJVNls absorbance A of the various catalysts tested. b) Photocurrent I generated with time under visible light over various materials suspended with acetate and Fe3+. ) Concentration c of evolved C02 as a function of time during photooxidation of acetaldehyde with various photocatalysts (0. g). The acetaldehyde (200 ppm) was mixed with air in a 500-mL Pyrex reaction cell. experiments give individual hydrogen- and oxygen-producing activities from each half-reaction of water splitting. In these reactions, two reference catalysts were loaded with 0. 1 wt% Pt as a co-catalyst to collect photoelectrons away from holes by forming a Schottky-type Junction structure. [16] The rates of oxygen evolution from water in the presence of AgN03 as the electron scavenger (2 H20 + 4 Ag+! 2 + 4 H+) are listed in Table 1 .

Again, the PCD demonstrated the best performance 4587 Table 1 : Photocatalytic activities for oxygen evolution from an aqueous AgN03 solution as tested for the various catalysts. [a] Catalyst Band gap energy Eg [eV] lab Oxygen evolution caFe204/PbBi2Nb1. 9WO. 109 PbBi2Nb209 Ti02?…XNX 2. 75 2. 88 2. [email protected] 675 520 221 450 431 451 29 14 [a] Catalyst 0. 3 g; light source 450-W Xe-arc lamp (Oriel) with UV cut-off filter (l ! 420 nm). The reaction was performed in an aqueous AgN03 solution (0. 05 mol L?…I, 200 mL). b] The wavelength at the absorption edge was determined as the intercept on he wavelength axis for a tangent drawn on absorption spectra. [c] Per gram of catalyst and hour. [d] QY = quantum yield (see the Experimental Section). [e] The minimum energy of photoabsorption was estimated from the intercept of the shoulder peak onset. even without a co-catalyst. The quantum yield of 02 evolution over the PCD was our knowledge, this is the highest value ever reported for the reaction over semiconductor photocatalysts under visible light. The hydrogen evolution with methanol as a hole scavenger was also studied (H20 + CH30H! H2 + C02). The relative activity trend among the three photocatalysts was the same, but the ates were lower than those for oxygen evolution by factors of at least 10, and thus are not reported herein. It has been demonstrated that PCD is a highly active novel photocatalyst. Application of the p-n diode concept commonly employed in the synthesis of monolithic energy conversion devices and the employment of techniques for nanomaterial synthesis have allowed the production of a nanocomposite between the high-order oxides with a unique confguration.

It appears that the p-n diode formation results in the efficient separation of electron-hole pairs to minimize the energy-wasteful electron-hole ecombination, which leads to the high photocatalytic activity. The materials involved are all stable oxides, which means less stability problems under irradiation with light. Indeed, the crystal structure did not change during the reaction, and the postreaction analysis showed no indication of dissolved catalyst components, even after more than 100 h of water decomposition.

The PCD catalyst appears to be particularly active for photooxidation reactions. The activity could be directly exploited for the degradation of toxic organic pollutants, as demonstrated for acetaldehyde and isopropyl alcohol. Cheap and abundant sunlight or weak indoor lighting could be employed as the light source. The high activity for the oxidation of water and the generation of a photocurrent could be of advantage for producing a photoelectrochemical cell that converts optical energy into chemical energy by decomposing water. 2] The overall performance of such a device is determined by the ability of the semiconductor anode[2] to oxidize water, and our PCD photocatalyst with the remarkable oxygen-producing capability could be used for this purpose. Furthermore, since the concept of PCD fabrication ould be applied for other visible-light absorbing semiconductors, further improvement in performance may be possible by a materials screening of a wider scope. 4588 Experimental Section solid-state method. A stoichiometric mixture of PbO (Aldrich 99. 999 %), Bi203 (Aldrich 99. 9 Nb205 (Aldrich 99. 999 %), and W03 (Aldrich 99. 999 %) was ground in a mortar. The pelletized powders were calcined at 1123 K for 24 h in static air and sintered at 1323 K for 24 h. Next, the sol-gel route was adopted to synthesize the CaFe204 nanoparticles: A stoichiometric ratio of H20 (Aldrich 99. 999 and H20 (Aldrich 99. 99 %) was mixed in 30 % aqueous NH3 solution, and the mixture was stirred at room temperature for 24 h. The PCD composite of CaFe204/ pbBi2Nb2?…xWx09 was made by hydrothermal treatment of preformed PbBi2Nb1. 9WO. 09 and ca?¦204 sol at 150 8C for 7 d to obtain 2 ca?¦204 loading on PbBi2Nb2?…xwx09. The ca?¦204/ PbBi2Nb1. 9WO. 109 thus obtained was characterized by high-resolution transmission electron microscopy (HRTEM, Phillips Model CM 200) and I-JVNis diffuse reflectance spectroscopy (Shimadzu, UV 2401). Prior to the water-splitting reactions, all the catalysts (except the PCD) were loaded with 0. wt % Pt by impregnation with PtC12. The photocatalytic reactions in aqueous solution were carried out at room temperature in a closed system using a 450-W Xe-arc lamp (Oriel) with UV cut-off filter (l ! 20 nm) placed in an inner irradiation-type 200-mL Pyrex reaction cell. The H2 evolution was examined in an aqueous solution (distilled H20 (170 mL) + CH30H (30 mL)), and the 02 evolution in an aqueous AgN03 solution (0. 05 mol L?…I, 200 mL), both containing 0. 3 g of the catalyst. The quantum yield (QY) was calculated as twice the number of generated H2 molecules or four times the umber of generated 02 molecules divided by the number of photons absorbed by the photocatalyst.

The number of absorbed photons was determined with a light flux meter (181 5-C, Newport) with the light sensor attached to the photocatalytic reactor. About 200 ppm of gaseous CH3CHO or isopropyl alcohol was injected into a 500-mL Pyrex reaction cell filled with air and containing 0. 3 g of a catalyst. The concentration of the reaction products (H2, 02, C02) was determined by a gas chromatograph equipped with a thermal conductivity detector and a molecular sieve 5-0 column. For photocurrent measurements, 25 mg of photocatalyst was suspended in distilled H20 (75 mL) containing acetate (0. m) and Fe3+ (0. 1 mm) as an electron donor and acceptor, respectively, and the pH value of the suspension was adjusted to 1. 4 with HC104. A Pt plate (1 0 1 cm2, 0. 125 mm thick, both sides exposed to solution), a saturated calomel electrode (SCE), and a Pt gauze were immersed in the reactor as working (collector), reference, and counter electrodes, respectively. With continuous N2 purging of the suspension, photocurrents were measured by applying a potential (+ 0. 6 V vs. SCE) to the Pt electrode using a potentiostat (EG&G).

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