Dynamic control of photoluminescence for self-assembled nanosheet films intercalated with lanthanide ions by using a photoelectrochemical reaction
Dynamic control of photoluminescence for self-assembled nanosheet films intercalated with lanthanide ions by using a photoelectrochemical reaction
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DOI:
10.1002/anie.200704608
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发表时间:
2008-01-01
影响因子:
16.6
通讯作者:
Matsumoto, Yasumichi
中科院分区:
文献类型:
--
作者:
Ida, Shintaro;Ogata, Chikako;Matsumoto, Yasumichi
Semiconductor oxide nanosheets synthesized by exfoliation of layered oxides are two-dimensional crystals with a thickness of about 1 nm.[1–4] New layered materials and their films can be reassembled by electrostatic self-assembly deposition (ESD)[5] and by layer-by-layer (LBL)[6–8] techniques, respectively. Since the nanosheets have a negative charge in aqueous solution they can be used with various cationic species as the starting materials. Layered materials prepared from nanosheets and lanthanide (Ln) ions are promising as new functional materials because Ln ions have unique properties, such as luminescence and magnetic properties, that are attributable to the 4f electron orbital. For example, the titanate layered oxide intercalated with Eu3+ ions prepared from titanate nanosheets and Eu3+ ions has unique luminescence properties.[9–11] The layered oxide gives a red emission from the Eu3+ ions which is induced by energy transfer through excitation of the bandgap of the titanate nanosheet,[9, 10] and the emission from the Eu3+ ions is promoted by intercalated water molecules.[10] Furthermore, spectral hole burning caused by the intercalated water molecules was observed in the excitation spectra at room temperature.[11] Nanosheets of TiOx, NbOx, and TaOx give a high photocurrent during the photoelectrochemical reaction under UV illumination with an energy higher than that of the bandgap.[12] This finding indicates that a large charge separation is produced between the holes in the valence band and the electrons in the conduction band during excitation of the bandgap. Consequently, layered oxide materials intercalated with Ln ions simultaneously exhibit both photoluminescence and a photoelectrochemical reaction during excitation of the bandgap on illumination with UV light. The study reported herein demonstrates a new form of dynamic control over the photoluminescence of Ln ions intercalated in self-assembled nanosheet films of TiOx and NbOx. The photoluminescence properties of Ln ions are changed by factors such as a change in the pHvalue and the addition of anionic species.[13–17] However, it is difficult to dynamically control the photoluminescence properties of Ln3+ ions. In the present system, the emission intensities of the intercalated Eu3+ and Tb3+ ions can be readily controlled by varying the applied potential. The nanosheet/Ln3+(Ti1. 81O4 nanosheet/Eu3+(TiO/Eu) and Nb6O17 nanosheet/Tb3+(NbO/Tb)) films were prepared and fixed on boron-doped diamond electrodes by the LBL technique. The chemical compositions of the TiO/Eu and NbO/Tb films were EuxTi1. 81O4 (x= 0.20–0.30) and TbyNb6O17 (y= 1.30–1.50), respectively. These are close to the theoretical neutral compositions (Eu0. 25Ti1. 81O4 and Tb1. 33Nb6O17). The Ln3+ ions were sandwiched between nanosheets (see Figure S-1 in the Supporting Information). Figure 1 shows a schematic illustration of the system used for the measurement of the photoluminescence. The photoelectrochemical cell with three electrodes, with the nanosheet/Ln3+ film acted as a working electrode, was placed in the sample chamber of a fluorescence spectrophotometer. A 0.1 m K2SO4 solution (pH 6.5) was used as the electrolyte solution. Figure 2 shows the emission intensities of the TiO/Eu and NbO/Tb films under illumination by UV light (wavelength: 260 nm) as a function of potential (sweep rate: 20 mVsÀ1). The red emission of the Eu3+ ions (614 nm, 5D0-7F2) appeared in the potential region above about À1. 2 V, but disappeared in the potential region below this potential. The same profile was obtained when the emission was monitored at 592 nm (5D0 …