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Journal of Nanomaterials
Volume 2012 (2012), Article ID 958593, 6 pages
Facile Hydrothermal Synthesis and Optical Properties of Monoclinic CePO4 Nanowires with High Aspect Ratio
1Department of Chemistry, Faculty of Science, Chiang Mai University, Chiang Mai 50200, Thailand
2Materials Science Research Center, Faculty of Science, Chiang Mai University, Chiang Mai 50200, Thailand
3Department of Materials Science and Technology, Faculty of Science, Prince of Songkla University, Hat Yai, Songkhla 90112, Thailand
4Department of Physics and Materials Science, Faculty of Science, Chiang Mai University, Chiang Mai 50200, Thailand
Received 14 April 2012; Accepted 10 July 2012
Academic Editor: Yanqiu Zhu
Copyright © 2012 Nuengruethai Ekthammathat et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
One-dimensional cerium phosphate (CePO4) nanowires (NWs) were successfully synthesized by a facile and simple hydrothermal method at 200°C for 12 h, using Ce(NO3)3·6H2O and Na3PO4·12H2O as starting materials, and followed by pH adjusting to be 1–3 using HNO3 (conc.). Phase, morphologies, and vibration modes of the as-synthesized CePO4 products, characterized by XRD, SEM, TEM, and FTIR, were proved to be perfect and uniform monoclinic CePO4 nanowires with aspect ratio of more than 250 for the product synthesized in the solution with the pH of 1. The UV-visible and photoluminescence (PL) spectrometers were used to investigate optical properties of the as-synthesized monoclinic CePO4 nanowires.
Since the discovery of carbon nanotubes by Iijima in 1990, a number of one-dimensional (1D) nanotubes, nanorods, and nanowires, have widely attracted interest for worldwide scientists, due to their novel physical and chemical properties caused by their low-dimensional and quantum-sized effects for different applications. In addition, these 1D nanomaterials can play an important role in functional nanodevices for light emitting diodes (LEDs), solar cells, single-electron transistors, lasers, and fluorescence for biological labels. Controling the synthesis of anisotropic nanostructured materials may therefore bring towards some unique properties and further enhance performances for a variety of applications [1–3].
Rare earth phosphate materials with unique 4f-5d and 4f-4f electronic transition have been widely used as high-performance luminescent devices, magnetic materials, catalysts, time-resolved fluorescence labels, and other functional materials. They are well known for the production of phosphor, sensor, and heat-resistant materials. Among them, CePO4 as well as its solid solutions is able to be used as highly efficient emitters for green light of luminescent devices. The monoclinic CePO4 monazite, one of the most stable materials although at a temperature as high as 1200 K, is appropriate for heat-resistant ceramic applications. It exists for billions of years by forming solid solutions with tetravalent actinide ions, such as U4+ and Th4+. Thus it is a promising material for nuclear waste storage. But for hexagonal CePO4, it is able to apply for tribological applications due to its natural layered structure [2–6].
In this paper, synthesis and formation mechanism of monoclinic CePO4 nanowires (NWs) with high aspect ratio by a hydrothermal method without the use of surfactant and template as morphological controlling agents were reported. This method is simple, inexpensive, highly effective, and appropriate for synthesizing of other 1D nanomaterials.
All reagents, Ce(NO3)36H2O, Na3PO412H2O, and HNO3, bought from Sigma-Aldrich Co. LLC., were analytical grade and used without further purification. For a typical synthesis of monoclinic CePO4 NWs, 0.003 mol Ce(NO3)36H2O was dissolved in 10 mL distilled water with the subsequent adding of 10 mL 0.003 M Na3PO412H2O solution. The solution pH was adjusted to 1, 1.5, 2, and 3 using HNO3 (conc.). Then, each of these solutions was transferred into Teflon containers, which were put in home-made stainless steel autoclaves. The autoclaves were tightly closed, heated at 200°C for 12 h in an electric oven, and left naturally cool down to room temperature. Then the as-synthesized precipitates were separated by filtration, washed with deionized water several times and ethanol, and dried at 70°C for 12 h. The final products appeared as light green solid powder.
The crystalline phases and crystalline degree of the as-synthesized nanostructured products were analyzed by X-ray diffractometer (XRD, Philips X’Pert MPD) operating at 45 kV 35 mA and using Cu Kα line in 2θ = –. The morphology investigation was carried out by field emission scanning electron microscope (FE-SEM, JEOL JSM-6335F) operating at 15 kV, transmission electron microscope (TEM, JEOL JEM-2010), and high resolution transmission electron microscope (HRTEM) using LaB6 electron gun operated at 200 kV. The samples for EM analysis were prepared by sonicating of dry products in absolute ethanol for 15 min. For SEM analysis, the solutions were dropped on aluminum stubs, dried in ambient atmosphere, and coated by Au sputtering to increase electrical conductivity. But for TEM analysis, 3–5 drops of the suspensions were put on carbon-coated copper grids which were dried in ambient atmosphere. Fourier transform infrared (FTIR, PerkinElmer RX 1) spectrophotometer was carried out in the range of 4000 to 400 cm−1 with 4 cm−1 resolution. Their optical properties were studied by a UV-visible (UV-vis) spectrometer (Lambda 25 PerkinElmer) using a UV lamp with the resolution of 1 nm and a fluorescence spectrophotometer (LS50BPerkinElmer) using 450 W Xe lamp with 0.2 nm resolution.
3. Results and Discussion
Phase of the product was characterized by X-ray powder diffraction (XRD) as shown in Figure 1. The XRD pattern was readily specified as monoclinic CePO4 structure of the JCPDS database number 32-0199 . There were no detection of any peaks of impurities of CeO2 and hexagonal CePO4 in this paper. Its lattice parameters (a, b, and c) and volume (V) of unit cell were calculated from the equations for monoclinic structure below where , , and are the Miller indices, d is the plane spacing, and β is the angle between the a and c axes (103.46°) . The calculated lattice parameters of monoclinic CePO4 structure were = 6.7852 Å, = 7.0802 Å, and = 6.4523 Å—in good accordance with those of the JCPDS database ( = 6.8004 Å, = 7.0231 Å, and = 6.4717 Å). The calculated cell volume of the as-synthesized CePO4 NWs was 301.45 Å3, higher than that of its bulk of 300.60 Å3. The increase in the cell volume indicated that lattice of the NWs was more distorted than that of their bulk [9, 10].
Figure 2 shows FTIR spectra of CePO4 NWs synthesized by the hydrothermal reaction at the pH of 1 adjusted by HNO3 solution. The vibrations of CePO4 NWs were due to the tetrahedrons, belonging to the A1(R) + E(R) + 2F2(IR + R). The (A1) (symmetric stretching mode) and (E) (symmetric bending mode) are Raman (R) active, and the (F2) (asymmetric stretching mode) and (F2) (asymmetric bending mode) are R and IR doubly active modes. The symmetry of ions in the CePO4 crystals decreases from Td to C1, and thus the non-IR modes become IR active . The broad band at 3460 cm−1 was assigned as the O–H stretching vibration of water molecules, adsorbed on surface of the product. The bands at 1200–400 cm−1 wavenumbers were assigned as the vibrations of groups. Those centered at 1052 cm−1 were specified as the asymmetric stretching vibrations of the groups and those at 609 cm−1 and 536 cm−1 were as the O–P–O bending vibrations. Four medium-intensity peaks between 700 and 400 cm−1 were caused by bending of P–O links in distorted tetrahedrons. The P–O stretching peak was split bands due to the removal of degeneracy of tetrahedral vibrations, corresponding to the characteristic peaks of phosphate groups of monoclinic cerium phosphate. In the monazite monoclinic phase, the tetrahedral phosphate groups are distorted in the nine fold coordination of lanthanide atoms and the phosphate absorptions are split accordingly. The stretching modes appeared as a cluster of very strong peaks at 954, 993, 1052, and 1092 cm−1. The adsorption of anions (1380 and 878 cm−1) from the precursor was not detected, indicating that the product was very pure phase [10–13].
The product morphology (Figure 3) was characterized by a scanning electron microscope (SEM), and was able to specify the evolution in the length of one-dimensional CePO4 product-influenced by pH of the solutions. Only the monoclinic CePO4 nanorods with 200 to 300 nm long and 10 nm in diameter were synthesized by the 200°C and 12 h hydrothermal reaction of the precursor solution with the pH of 3. Upon adjusting the pH values to 2 and 1.5, some CePO4 nanorods were transformed into CePO4 nanowires (NWs) with 1 to 5 μm in length and 15 to 20 nm in diameter. At the precursor solution pH of 1, the whole CePO4 NWs with aspect ratio > 250 were synthesized. The aspect ratios for different solution pH were summarized in Table 1, which showed the influence of pH values on the lengths and diameters of 1D CePO4. In this paper, uniform CePO4 NWs with high aspect ratio were successfully synthesized by the 200°C and 12 h hydrothermal reaction of the solution with the pH of 1.
To further show the real morphologies of the as-synthesized monoclinic CePO4 at the pH of 1–3, the products were characterized by a transmission electron microscope (TEM) (Figure 4). At the pH of 3, the product was structurally uniform nanorods. Their average diameter was 10 nm and length was up to 300 nm. Mixed nanowires and nanorods were detected at the pH of 2 and 1.5. The whole CePO4 NWs with longer than 5 μm and diameter of 20 nm were synthesized at the pH of 1. The growth direction of monoclinic CePO4 NWs was investigated by high resolution transmission electron microscope (HRTEM) as shown in the inset of Figure 4(d). It shows that the lattice spacing was about 4.81 Å, corresponding to the (−110) plane, with the growth direction of single monoclinic CePO4 crystal along the direction-parallel to the (−110) plane.
In general, the anisotropic growth of one-dimensional materials was driven by several factors such as surface energy, structure, electrostatic force, and surfactant. In this paper, the anisotropic CePO4 NWs was controlled by the chemical potential. The faster ionic migration usually promoted the reversible pathway between fluid and solid phases, leaving ions to reside in the right positions of crystal lattice . The formation mechanism of CePO4 NWs is able to explain as follows:
Ce(NO3)36H2O and Na3PO412H2O were mixed in distilled water, with the following of pH adjusting using HNO3 (conc.). During the hydrothermal treatment of the solution with the pH of 1, the clear colorless solution was heated up under high pressure. Concurrently, the Ce3+ and chemical potentials were raised up, including the faster ionic migration in the solution. During cooling, these ions combined to form light green precipitates of monoclinic CePO4 NWs—in accordance with the reports of Zhang and Guan .
The optical properties of CePO4 NWs hydrothermally synthesized in the solution with the pH of 1 were investigated by UV-visible and photoluminescence (PL) spectroscopy. The CePO4 NWs for the analyses were ultrasonically dispersed in absolute ethanol for 10 min. Their UV-visible absorption spectrum (Figure 5) is in the range of 220 to 650 nm. The absorption was detected as a strong band in the ultraviolet range, caused by the f–d electron transition of Ce3+ atoms in the lattice. It shows the major absorption peak at 274 nm coupled with a small shoulder at 257 nm. These bands were overlapping as the excited states were strongly split by the crystal field. Moreover, these results are in consistent with the data for transition from the 2F5/2 (4f1) ground state to the five crystal field split levels of the 2D (5d1) excited states, namely, the 2D5/2 and 2D3/2 [9, 15].
Figure 6 shows the PL spectrum at room temperature of CePO4 NWs using the excitation wavelength of 325 nm. It displays a broad emission peak of the CePO4 NWs over the 325 to 625 nm range. To estimate the contribution of each, it was necessary to deconvolute the PL spectrum. By using the Gaussian analysis, the deconvoluted results shows that the PL profile was at the best for five deconvoluted peaks. The first, second, and third were in the ultraviolet spectrum, the fourth in the blue range, and the fifth in the green wavelength. Each component represents different types of electronic transition, linked with the atomic arrangement and surface defects. The PL spectrum exhibits strong emission peaks centered at 388.24 nm (ultraviolet) and 438.46 nm (violet) [13, 16, 17]. Emission wavelength, color, and intensity of each component of CePO4 NWs are shown in Table 2. The strongest intensity of the PL spectrum for CePO4 NWs corresponded to the 438.46 nm violet wavelength with 38.49% of the whole emission.
In summary, uniform CePO4 NWs with aspect ratio of more than 250 were synthesized by the facile hydrothermal method. Their formation mechanism was also discussed in this paper. Different lengths and sizes of CePO4 products were influenced by the pH values. The uniform monoclinic CePO4 NWs were synthesized in the solution with the pH of 1. These NWs show the strong absorption in the ultraviolet range due to the f–d electron transition of Ce3+ atoms in crystal lattice. Their PL emission shows a broad band of 325 to 625 nm range with the strongest emission at 438.46 nm in the violet region.
The authors wish to thank the Thailand’s Office of the Higher Education Commission for providing financial support through the National Research University Project for Chiang Mai University (CMU) and the Human Resource Development Project in Science Achievement Scholarship of Thailand (SAST), and the Faculty of Science Research Fund, Prince of Songkla University (PSU), including the Graduate School of CMU through the general support.
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