Abstract
One-dimensional nanostructures exhibit interesting electronic and optical properties due to their low dimensionality leading to quantum confinement effects. ZnO has received lot of attention as a nanostructured material because of unique properties rendering it suitable for various applications. Amongst the different methods of synthesis of ZnO nanostructures, the hydrothermal method is attractive for its simplicity and environment friendly conditions. This review summarizes the conditions leading to the growth of different ZnO nanostructures using hydrothermal technique. Doping of ZnO nanostructures through hydrothermal method are also highlighted.
Keywords: ZnO, hydrothermal, nanostructures, synthesis, doping
Introduction
Nanostructured ZnO materials have received considerable interest from scientists due to their remarkable performance in electronics, optics and photonics. As early as the 1960s, synthesis of ZnO thin films was an active field because of applications in sensors, transducers and as photocatalysts. In the last few decades, study of one-dimensional material has gained importance in nanoscience and nanotechnology. With reduction in size, novel electrical, mechanical, chemical and optical properties are introduced resulting from surface and quantum confinement effects.
ZnO is a significant technological material. The absence of a centre of symmetry in its wurtzite structure, along with large electromechanical coupling, results in strong piezoelectric and pyroelectric properties. ZnO is therefore widely used in mechanical actuators and piezoelectric sensors. In addition, ZnO is a wide band-gap (3.37 eV) compound semiconductor that is appropriate for short wavelength optoelectronic applications. The high exciton binding energy (60 meV) in ZnO crystal allows efficient excitonic emission at room temperature. ZnO is transparent to visible light and its conductivity can be increased through doping. ZnO nanostructures have a wide range of high technology applications like surface acoustic wave filters [1], photonic crystals [2], photodetectors [3], light emitting diodes [4], photodiodes [5], gas sensors [6], optical modulator waveguides [7], solar cells [8, 9] and varistors [10]. ZnO is also receiving a lot of attention because of its antibacterial property and its bactericidal efficacy has been reported to increase as the particle size decreases [11].
The discovery of carbon nanotubes by Iijima [12] in 1991 has initiated active research leading to the growth and characterization of one-dimensional nanowires of elemental and compound semiconductors such as Si [13], Ge [14], InP [15], GaAs [16] and ZnO [17–19]. Different nanostructures of ZnO have been reported such as nanowires and nanorods [20], nanocombs [21], nanorings [22], nanoloops and nanohelices [23], nanobows [24], nanobelts [25] and nanocages [26]. These structures have been successfully synthesized under explicit growth conditions [27].
ZnO nanostructures can be grown either in solution or from gaseous phase. The gas phase synthesis methods are expensive and complicated. The solution phase synthesis is usually done in water. The hydrothermal process of growing ZnO nanostructures has gained immense popularity due to its simplicity and tolerable growth conditions. As synthesis is carried out in aqueous solution, the growth temperatures are less than the boiling point of water.
Zinc oxide: crystal structure
The ZnO crystal is hexagonal wurtzite and exhibits partial polar characteristics [27] with lattice parameters a=0.3296 and c= 0.52065 nm.
The structure of ZnO can be described as a number of alternating planes composed of tetrahedrally coordinated O2- and Zn2 + stacked alternately along the c-axis, as shown in figure 1. The tetrahedral coordination in ZnO results in piezoelectric and pyroelectric properties due to the absence of inversion symmetry. Another important characteristic of ZnO is polar surfaces. The most common polar surface is the basal plane (0001). One end of the basal polar plane terminates with partially positive Zn lattice sites and the other end terminates in partially negative oxygen lattice sites. The oppositely charged ions produce positively charged Zn-(0001) and negatively charged O-() surfaces, resulting in a normal dipole moment and spontaneous polarization along the c-axis as well as a variance in surface energy. To maintain a stable structure, the polar surfaces generally have facets or exhibit massive surface reconstructions, but ZnO± (0001) surfaces are exceptions: they are atomically flat, stable and exhibit no reconstruction [1, 2]. Efforts to understand the superior stability of the ZnO±(0001) polar surfaces are at the forefront of research in today's surface physics [3–6]. The other two most commonly observed facets for ZnO are and , which are non-polar and have lower energy than the {0001} facets.
Zinc oxide: growth structures
ZnO exhibits a varied range of novel structures. These structures can be grown by tuning the growth rates along three fast growing directions: (, , ); (, , ) and ± [0001]. The relative surface activities of various growth facets under given conditions determine the surface morphology of the grown structure. Macroscopically, a crystal has different kinetic parameters for different crystal planes, which are emphasized under controlled growth conditions. Thus, after an initial period of nucleation and incubation, a crystallite will commonly develop into a three-dimensional object with well-defined, low-index crystallographic faces. Figures 2(a), (b) and (d) show a few typical growth morphologies of 1D nanostructures of ZnO. These structures tend to maximize the areas of the and facets because of the lower energy. The morphology shown in figure 2(b) is dominated by the polar surfaces, which can be grown by introducing planar defects parallel to the polar surfaces. Occasional planar defects and twins can be observed parallel to the (0001) plane, but dislocations are hardly seen [27].
Zinc oxide nanostructures—synthesis methods
The synthesis methods of different zinc oxide nanostructures can broadly be classified as follows:
- Solution phase synthesis: In the solution phase synthesis, the growth process is carried out in a liquid. Normally aqueous solutions are used and the process is then referred to as hydrothermal growth process. Some of the solution phase synthesis processes are
- Gas phase synthesis: Gas phase synthesis uses gaseous environment in closed chambers. Normally the synthesis is carried out at high temperatures from 500 °C to 1500 °C. Some commonly used gas phase methods are
ZAH based sol-gel synthesis of ZnO nanostructures
The sol-gel method has gained a lot of popularity as it offers controlled consolidation, shape modulation and patterning of the nanostructures. Concentrated ethanolic zinc acetate hydrate (ZAH) suspension when refluxed and distilled forms a transparent sol. Small ZnO nanoparticles of dimensions around 5 nm can be grown under high concentration conditions by addition of hydroxides (e.g. LiOH, NaOH, etc) [28]. There are reports of modifications of the ZAH dehydration or dissolution and subsequent condensation for the growth of ZnO nanostructures [29–31].
The search for primary clusters to serve as building blocks for various nanostructures has been going on for quite some time. The isolation and identification of primary clusters is an area of active research. The synthesis of the primary structures depend on various conditions like initial concentration of the salt, the synthesis temperature, heating time as well as nature of the solvent. The ZnO clusters can be members of any of the three different families mentioned below [28]:
Tetrahedral oxy-acetate Zn4O(Ac)6.
Ethoxy acetate (EtOZnAc)n.
Hydroxy-double salt (Zn-HDS) Zn5 (OH)8(Ac)2(H2 O)2.
When Zn(Ac)2 is heated in alcohol, the following reaction takes place initially
Zn4O(Ac)6 is also called basic zinc acetate. The by-products like H2O, acetic acid etc, can be removed by distillation. ZAH forms a larger homologue Zn10O4 (Ac)12 when it is dehydrated in the presence of acetanhydride and refluxed in EtOH. Continuous refluxing of ZAH sols can result in ZnO nanoparticles [45]. Zn4 O(Ac)6 can be considered as a well designed molecular model of ZnO.
Ethoxy acetates (EtOZnAc)n are formed in solutions having Zn10O4 (Ac)12 clusters. These species are formed gradually with time and after several weeks, large single crystals can be separated. The oxy-acetate clusters most probably generate intermediary zinc acetate monomers as shown by the following reactions:
These Zn(Ac)2 monomers can lead to formation of zinc ethoxy acetate (EtOZnAc)n crystals and acetic acid.
Hydroxy-double salt (Zn-HDS)Zn5 (OH)8 (Ac)2 (H2 O)2 is formed by the titration of ZAH solutions with an aqueous solution of sodium hydroxide. Zn-HDS has been detected in precipitates of preheated alcoholic ZAH sols. At high temperatures and after prolonged refluxing, Zn-HDS can be easily transformed into ZnO nanoparticles.
The occurrence of hydroxy double salts during the growth of ZnO nanoparticles may be due to the following:
- H2O induced reorganization of the tetrahedral species (primary and secondary) formed during initial nucleation. Hydroxyl ions also play a role.
The continuous liberation of zinc acetate during the growth of the ZnO nanoparticles may be another reason for the growth of the hydroxy double salts.
Stability of ZAH derived structures
Spanhel [28] carried out partial charge calculations using the Henry–Livage model. The partial charge values for the ZAH structures are shown in table 1.
Table 1.
Precursor clusters | ||
---|---|---|
Zn(Ac)2 ·2H2O | 0.471 | −0.227 |
Zn(Ac)2 | 0.469 | −0.235 |
Zn4O(Ac)6 | 0.467 | −0.245 |
Zn10O4(Ac)12 | 0.465 | −0.254 |
Zn5(OH)8(Ac)2· 2H2O | 0.463 | −0.269 |
Zn10O4(Ac)12·H2O·7EtOH | 0.429 | −0.462 |
EtOZnAc | 0.411 | −0.567 |
It can be observed that the tetrahedral oxy-acetate clusters are slightly more stable than the zinc acetate hydrate. Further, the stability of Zn10O4 (Ac)12 precursor is strongly increased in the presence of H2O and EtOH. Once a certain amount of water is present, there is a spontaneous formation of zinc hydroxy double salts (Zn-HDS). This is because of the higher stability of the Zn-HDS monomer with respect to the naked oxy-acetate clusters. As seen from the table 1, the most stable precursor cluster is the zinc ethoxy-acetate. An important point to note is that Zn2+ ions do not exist as free ions in alcoholic ZAH solutions as a strong chemical bond exists between Zn2+ ions and Ac ligands in all the compounds in table 1.
ZnO nanostructures through hydrothermal growth
Nanoparticles.
Even though the organometallic synthesis of ZnO nanoparticles in alcoholic medium has received wider acceptance for reasons of faster nucleation and growth as compared to water, still scattered reports of hydrothermal synthesis in aqueous medium are available in the literature. Baruwati et al [46] have reported the aqueous synthesis of ZnO nanoparticles using zinc nitrate hexahydrate. Synthesis was carried out in an autoclave at a temperature of 120 °C after adjusting the pH to 7.5 using ammonium hydroxide. After washing, the particles were dried at 80 °C overnight to obtain the powder form. The as synthesized particles are shown in the transmission electron microscope (TEM) images in figure 3.
Lu et al [47] successfully prepared crystalline ZnO powder through a hydrothermal process using ammonia as the base source. With Zn(NO3)2 as the source of Zn2+ ions, growth was carried out at 100 °C, 150 °C and 200 °C for 2 h and the effect of growth temperature and pH was studied. Figure 4 shows the variation of particle size of the ZnO powder and its yield as functions of growth temperature and pH. With pH<11 in region A of figure 4, the zinc hydroxide precursors are dissolved partially and the ZnO powder is nucleated in a heterogeneous system. On the other hand, in region B with pH≽ 11, all zinc hydroxide precursors are dissolved and a clear solution is formed so that ZnO powder is nucleated in a homogeneous solution. Different nucleation states thus take place in regions A and B with higher probability of nucleation in the heterogeneous solution.
Chen et al [48] synthesized nanoparticles of different morphologies using ZnCl2 and NaOH in a hydrothermal growth process using different organic compounds as template agents. A significant change in the morphology was observed as the synthesis temperature was increased with the particles changing from rod like to polyhedral. It was reported that the morphology also changed with the addition of different organic templates to the reaction mixture when the temperature was maintained at 160 °C. The various morphologies along with the templates used are listed in table 2.
Table 2.
Particle properties | ||
---|---|---|
Additives | Morphology | Size (nm) |
Tributylamine | Rod-like | 200–300 |
Triethylamine | Rod-like | 100–300 |
Triethanolamie | Spindle-like | 100–300 |
Diisopropylamine | Rod-like | 200–400 |
Ammonium phosphate | Rod-like | 200–500 |
1, 6-Hexadianol | Rod-like | 300–700 |
Triethyldiethylnol | Rod-like | 100–300 |
Isopropylamine | Rod or sheet-like | |
Cyclohexylamine | Sheet-like | 300–500 |
n-Butylamine | Sheet-like | 200–400 |
Ammonium chloride | Sheet | 50–200 |
Hexamethylenetetramine | Snow-flake like | 20–50 |
Ethylene glycol | Ellipse | 40–100 |
Ethanolamine | Polyhedron | 50–200 |
A very simple procedure to prepare ZnO nanoparticles at a very high pH∼14 using tetramethylammonium hydroxide (TMAH) as a precipitating agent was suggested by Musić et al [49]. Nanoparticles sized from 10 to 20 nm were precipitated at room temperature by adding TMAH to an ethanolic solution of zinc acetate dehydrate. Addition of water to the ethanolic solution prior to adding TMAH yielded ZnO snowflakes.
Vishwanathan and Gupta [50] have shown that supercritical water can also be a good reaction medium for the hydrothermal synthesis of ZnO nanoparticles. Spherical ZnO nanoparticles were synthesized by oxidation of zinc acetate in supercritical water in a continuous tubular reactor. Particle size and morphology can be controlled by varying conditions like temperature, pressure or the reaction atmosphere. Nanoparticles with diameters ranging between 39 and 320 nm were synthesized using this method.
The synthesis time has been significantly reduced through the use of microwave irradiation and the ZnO nanocrystallites thus formed were observed to be more defective than the ones synthesized over a few hours of hydrolysis [51]. Nanoparticles with inherent defects are capable of exhibiting visible light photocatalysis even without doping with transition metals, which is the normally followed method.
Nanowires and nanorods.
Andres-Vergés et al [52] first reported the hydrothermal method of growing ZnO nanostructures. However, this could not instil much interest till Vayssieres et al [53] successfully used the method for the controlled fabrication of ZnO nanowires on glass and Si substrates by the thermal decomposition of methenamine and zinc nitrate. To initiate the growth from the substrate, a thin layer of ZnO nanoparticles was grown on the substrate. Methenamine, also known as hexamethylenetetramine (HMT) or hexamine is a highly water soluble, non-ionic tetradentate cyclic tertiary amine. Thermal degradation of HMT releases hydroxyl ions which react with Zn2+ ions to form ZnO [54]. This can be summarized in the following equations:
It is a general acceptance that the role of HMT is to supply the hydroxyl ions to drive the precipitation reaction [55]. Apart from that, some also opine that HMT acts as a buffer as the rate of its hydrolysis decreases with increasing pH and vice versa [56]. Ashfold et al [55] have demonstrated that the rate of decomposition of HMT is independent of the reaction that yields ZnO indicating that HMT does act as a kinetic buffer. In oxide formation, the phase that is thermodynamically less stable will precipitate out faster [56]. In the initial growth stage, the pH and the concentration of Zn2+ ions is such that the ZnO growth will be through Zn(OH)2. With the gradual increase in the pH and the decrease in the concentration of the Zn ions, Zn(OH)2 becomes thermodynamically unstable and the Zn(OH)2 formed on the substrate will start dissolving. Further growth of the nanostructures will have to be through direct deposition of ZnO [55].
The contribution of HMT in the growth process of ZnO nanowires has also been discussed by Sugunan et al [57] in a totally different approach. It was proposed that HMT, being a long chain polymer and a nonpolar chelating agent, will preferentially attach to the non polar facets of the zincite crystal, thereby cutting off the access of Zn2+ ions to them leaving only the polar (001) face for epitaxial growth. HMT therefore acts more like a shape-inducing polymer surfactant rather than as a buffer. Figure 5 shows the mechanism of attachment of hexamine on the nonpolar facets.
There is a lot of literature reporting investigation on the growth and properties of ZnO nanorods synthesized using zinc nitrate and HMT such as the effect of substrates and seed layers on the morphology of nanorods and nanotubes [58–60], growth on different substrates [20] and the control of aspect ratio through the addition of citrate anions [61]. Pal and Santiago [62] have managed to control the morphology of ZnO nanostructures by varying the amount of a soft surfactant, ethylenediamine and the pH of the reaction mixture of zinc acetate, sodium hydroxide and the surfactant. Homogenous growth was observed at a pH of 12 with inhomogeneity creeping in as the pH decreases. A 10% concentrated ethylenediamine gave higher aspect ratio than 5% concentration. Figure 6 shows scanning electron microscope (SEM) images of hydrothermally grown ZnO nanorods using zinc nitrate and hexamine.
ZnO nanowires and nanorods have been successfully synthesized using different surfactants and numerous reports are available. Tang et al [63] synthesized ZnO nanorods using zinc acetylacetonate Zn(acac)2·H2O as a single source precursor and investigated the growth of the rods in the presence of four different surfactants: polyvinyl alcohol (PVA), polyethylene glycol (PEG), sodium dodecyl sulphate (SDS) and cetyltrimethyl ammonium bromide (CTAB). The use of PVA resulted in more regular and defect free rods than PEG, SDS and CTAB. Li et al [64] has reported the growth of tapered ZnO nanorods with diameter decreasing from 400 nm at the body to about 80 nm at the tip from CTAB assisted hydrothermal growth. Zinc acetate dehydrate was used as the precursor and the pH was adjusted to 13 using KOH. The use of carbamide CO(NH2)2 as a surfactant [65] in a hydrothermal growth with ZnSO4 and NaOH yielded highly crystalline ZnO nanobelts. Chen et al [66] studied the effect of potassium iodide (KI) as a surfactant in the crystallization of ZnO nanorod clusters from a chemical bath containing zinc nitrate hexahydrate Zn(NO3)2·6H2 O and hydrazine hydrate N2H4·H2O. They obtained step growth of hexagonal nanorod clusters, and this morphology is attributed to the presence of iodine ions in the growth bath. Stepped columns of ZnO were also observed using CTAB as the surfactant [67]. Experiments further showed that the source of Zn ions can also affect the morphology of the end product. Ni et al [67] obtained ZnO nanorods in place of stepped columns simply by changing the source of Zn ions from Zn(Ac)2 to ZnCl2 and keeping all other conditions same. This may be due to the change in pH of the growth bath.
Water soluble amphiphilic block copolymers, PEO-PPO-PEO, due to their unique properties are being used as templates for the ingenious morphologies of inorganic materials such as nanoparticles, mesoporous materials and hierarchically ordered oxides [68–72]. Zhang et al [73] managed to control the shape of bundles of ZnO nanostructures through a macromolecular surfactant (L64 and F68) assisted hydrothermal growth route. The bundles of ZnO nanostructures are shown in figure 7.
It was deduced that the nanobundle superstructures of ZnO result from a two-step mechanism in aqueous solutions with initial nucleation followed by the growth of the nanorods around these nuclei. Overall size and arm lengths are probably controlled by the growth velocity of ZnO particles and the micelle dimension of PEO–PPO–PEO copolymers. ZnO is a polar crystal, O2- is in hexagonal closest packing, and each Zn2+ lies within a tetrahedral group of four oxygen ions [74]. Zn and O atoms are stacked alternatively along the c-axis and the top face (0001) consists of tetrahedral zinc having a terminal OH ligand as shown in figure 8. The formation of hexagonal prism and pyramid like ZnO crystals is attributed to the difference in the growth velocities of various crystal facets. The growth velocities under hydrothermal conditions along the different directions are known to follow the pattern V(0001)> V(1011)> V(1010) [73]. The relative growth rate of these crystal faces will determine the final shape and aspect ratio of the ZnO nanostructures. The preferential growth along the (0001) polar direction proceeds unabated and the ZnO nanorods would appear in the end products. Although the chemical reaction is relatively simple, the growth process of ZnO nanobundles is quite complicated. It can be presumed that the faster the growth rate, the quicker the disappearance of the plane. The (0001) plane disappears due to its high growth velocity leading to the pointed shape at the end of the c-axis. As a consequence of the slow growth of the (1010) plane, the crystal remains to form the hexagonal prisms, while the (1011) plane corresponds to the formation of the hexagonal pyramid like tips.
Wang et al [75] has shown that it is possible to efficiently synthesize large two-dimensional arrays of obelisk shaped ZnO nanorods on quartz or glass substrates through a simple hydrothermal deposition method with zinc nitrate, ammonia and ammonium hydroxide as the precursors. The single-crystalline obelisk rods with diameters ranging between 300 and 400 nm and lengths of about 5 μm were grown in Teflon vessel at 95 °C for 30 min and the SEM images are shown in figure 9.
The mechanism for the formation of ZnO crystals using ammonia can be summarized in the following equations [76, 77].
or ZnO may also form from the complex ion Zn(OH)42+ as below:
The complex ions Zn(NH3)42 + and Zn(OH)42− formed due to the mixing of zinc nitrate, ammonia and ammonium hydroxide, dehydrate to initiate heterogeneous nucleation of ZnO on the substrate. The possible formation of the obelisk-shaped single-crystalline rods is attributed to multiple layered structures as explained in figure 10.
The presence of Zn2+ containing salts is not a necessity for the growth of ZnO nanostructures through the hydrothermal growth method. Li et al [78] has successfully grown large scale arrays of ZnO nanorods on zinc foil without the assistance of any template, oxidant or coating of metal oxide layers, simply by dipping the foil into a 25% aqueous solution of ammonia (NH4OH) and heating at a temperature 80 °C in a Teflon-lined stainless steel autoclave. Four different samples were prepared by varying the concentration of ammonia in a 80 ml growth bath and the growth duration as shown in table 3. The SEM images are shown in figure 11.
Table 3.
Sample | NH4OH (g) | Reaction time (h) |
---|---|---|
A1 | 1.5 | 12 |
A2 | 1.5 | 24 |
A3 | 3.5 | 12 |
A4 | 3.5 | 24 |
It was observed that the thickness, density and morphology of the ZnO nanorod arrays are affected by the alkalinity of the solution in the growth bath. The sharp tips of the nanorods are probably due to the concentration gradient of Zn2+ from the base to the tip. The increase in growth time only led to thicker rods with the lengths remaining almost comparable. With the increase in concentration of ammonia, no growth was observed till 12 h but a very dense growth of uneven pointed rods was observed when the growth duration was increased to 24 h.
Flower-like and cabbage-like nanostructures.
Flower-like structures are very typical of ZnO and can be synthesized using simple hydrothermal methods. Wahab et al [79] has reported the growth of flower-like ZnO using hydrothermal method. The flowers, composed of hexagonal ZnO nanorods, were synthesized at a temperature of 90 °C using zinc acetate dehydrate and sodium hydroxide in aqueous solutions. The flowers, with nanorod petals as long as 2–4 μm, could be synthesized in just 30 min. SEM images of the nanoflowers are shown in figure 12. All the pointed nanorods emerged from a single centre thereby acquiring the spherical shape.
Flower-like ZnO nanostructures with nanosheet petals was synthesized by Shao et al [80] through a hydrothermal route using zinc chloride and ammonia as the reactants. The flowers, averaging in size of about 30 μ m, are composed of sheets of thickness about 150–250 nm. SEM images (figure 13) reveal numerous well distributed nanostructures formed all over the copper plate substrate.
Li et al [81] has reported the growth of flower-like and cabbage-like nanostructures using CTAB as the surfactant in a hydrothermal growth process at temperatures of 120, 150 and 180 °C. They obtained flower-like micro and nanostructures consisting of ZnO nanorods at a temperature of 120 °C. As the synthesis temperature was increased to 150 and 180 °C, cabbage-like structures were formed due to the repeated growth of two-dimensional ZnO nanosheets. The thickness of the nanosheets obtained at 150 °C was about 50 nm and at 180 °C about 100 nm. The nanostructures obtained are shown in figure 14. The authors have tried to explain the growth of the nanostructures with the schematic diagram shown in figure 15.
CTAB being a cationic surfactant reduces the surface tension and as such inhibits the formation of a new phase. CTAB acts as a transport medium to transport Zn(OH)42 − growth units which come together to form individual rod-like structures at 120 °C which then self-assemble into the ZnO nanoflowers. However, at temperatures of 150 and 180 °C, two-dimensional nanosheets are formed which then self-assemble into the cabbages.
Three-dimensional ZnO nanostructures have also been successfully synthesized through a simple hydrothermal process using ammonia and zinc acetate dihydrate at 95 °C [82]. Different morphologies were observed when the pH of the growth solution was changed between 9 and 11.8. The SEM micrographs are shown in figure 16 and a summary of the results is presented in table 4.
Table 4.
pH | Morphology | Shape | |
---|---|---|---|
9.0 | Coalescence of Zno | Coalescence | Budding flower |
9.5 | Nano-particles | ↑ | |
10.0 | Zno nanorod | Blossom | |
10.5 | Separation sharp rods | Separation | Chestnut but |
or echinoid | |||
11.0 | Separation of thick rods | ↓ | Dense chestnut |
bur | |||
11.5 | Coalescence of rods | Gingko leaves | |
11.8 | Archetype of thick rods | Coalescence | Dendelion |
Hydrothermal synthesis using microwaves
Another method of synthesis of nanostructures which is receiving a lot of interest lately is the use of microwave heating in place of conventional heating. Use of microwaves for synthesis was first reported in 1986 by Gedye et al [83] following which there has been an increase in the use of microwaves for nanostructure synthesis [51, 84, 85]. Ma et al [86] have synthesized ZnO micro and nanostructures using zinc nitrate hexahydrate and pyridine in a hydrothermal process through microwave irradiation at 90 °C for 10 min. Adjusting the concentration of pyridine in the reaction bath, various morphologies of ZnO could be synthesized like hexagonal columns, linked hexagonal needles, hollow structures and hexagonal nanorings. Some of the structures are shown in figure 17.
Chemical double dip technique
Vijayan et al [87] have successfully grown thin films of ZnO using a double dip technique using sodium zincate (Na2ZnO2) as the first dipping solution followed by a second dipping in hot water. The conversion of sodium zincate into zinc oxide in presence of water follows the simple reaction
Polycrystalline thin films with high preferential orientation along the (002) plane could be obtained using the double dip technique. The microstructural parameters were dependent upon the temperature of the hot water bath, the pH as well as the amount of Zn(SO4)2 used for preparing the sodium zincate solution.
Crystal structure of hydrothermally grown ZnO nanostructures
The hydrothermally grown ZnO nanostructures are single crystalline and exhibit the wurtzite structure of ZnO. X-ray diffraction (XRD) analyses for different ZnO nanostructures grown through hydrothermal methods revealed the hexagonal wurtzite structure, and the peaks could be indexed according to JCPDS card No. 79-2205 with a= 0.3249 nm and c=0.5205 nm [46, 77, 81]. Some of the XRD results are shown in figure 18.
Further structural characterizations can be performed using high resolution transmission electron microscopy (HRTEM). Fast Fourier transforms (FFT) and inverse FFT of HRTEM images of ZnO nanoparticles [51] confirmed the wurtzite structure. One of the imaged particles is shown in figure 19(B) and the corresponding FFT and Inverse FFTs are shown in figures 19(C)–(E). Lattice spacings of 0.28 nm and 0.16 nm indicate the presence of the (100) and (110) planes.
Another method of confirming the crystal structure is through the use of selected area electron diffraction (SAED) setup which comes as an accessory with TEMs. The SAED pattern for ZnO nanorods synthesized through a hydrothermal method [79] is shown in figure 20 along with low and high magnification TEM images. Figure 20(a) shows a low resolution TEM image of pointed tip ZnO nanorods. The corresponding SAED pattern (inset) confirmed that the rods are single crystalline and grew along the [0001] direction.
The lattice fringe spacing in the HRTEM image is 0.52 nm which corresponds to the hexagonal wurtzite structure of ZnO and indicates that the growth occurred along the [0001] direction. The SAED pattern (inset) agrees with the HRTEM observation [79].
Doping of ZnO nanostructures through hydrothermal routes
Doping of semiconducting nanostructured materials is the primary technique for controlling properties like bandgap, electrical conductivity and ferromagnetism. Transition metal doping of II–VI and III–V semiconductors is generating a lot of interest from researchers for possible applications in spintronics and visible light photocatalysis. A lot of work has been done in the area of transition metal doping of ZnO single crystals and thin films [88–92]. However, a few reports on the synthesis and characterization of ZnO nanostructures doped with different impurities like Al, Sn, Ga, In, Sb, Cu, etc are available in the literature [93–98]. Li et al [99] has synthesized ZnO nanorods doped with manganese (Mn), chromium (Cr) and cobalt (Co) in a hydrothermal synthesis using zinc nitrate, transition metal nitrate and hexamethylenetetramine. It was observed that the doping was good with Mn (8% doping from a 10% solution) and Co (17% doping from a 10% solution) dopants and poor with Cr (4% doping from a 10% solution). The morphology of the doped ZnO nanorods was different from that of the undoped nanorods, the SEM images of which are shown in figure 21.
Yuhas et al [100] has communicated the successful doping of ZnO nanorods with Co by the thermal decomposition of zinc acetate and cobalt (II) acetate in refluxing trioctylamine. The reaction temperature was set at 310 °C and the reaction was allowed to continue from 45 to 180 min to obtain rods of different diameters. The hydrothermal synthesis of Al-doped ZnO nanopowders was reported by Piticescu et al [101]. The synthesis was carried out in a 2L computer-controlled Teflon autoclave using KOH as a mineralizing agent. Indium doping of ZnO nanorods was done after the rods were grown hydrothermally through a post deposition thermal annealing in an inert atmosphere [102]. Indium doping during the hydrothermal synthesis could not be carried out due to the formation of In(OH)3 phase. Doping was carried out successfully for 0.5, 1 and 2%.
Conclusion
Hydrothermal synthesis of ZnO nanostructures is simple and efficient and it is receiving a lot of attention of late. Various additives are used in aqueous medium to successfully synthesize ZnO nanostructures of different morphologies, a mixture of zinc nitrate and hexamine are the most popular. ZnO nanostructures are attractive candidates for applications in a host of devices like solar cells, sensors, detectors, energy generators as well as artificial structures for tissue engineering. ZnO nanostructures are being increasingly used as photocatalysts for degrading harmful contaminants like pesticides from ground water. Within the next decade, ZnO nanostructures are most likely to move into industrial applications.
Acknowledgments
The authors would like to acknowledge partial financial support from the National Nanotechnology Center, belonging to the National Science and Technology Development Agency (NSTDA), Ministry of Science and Technology (MOST), Thailand and the Centre of Excellence in Nanotechnology at the Asian Institute of Technology.
Reference
- Emanetoglu N W, Gorla C, Liu Y, Liang S. and Lu Y. Mater. Sci. Semicond. Process. 1999;2:247. doi: 10.1016/S1369-8001(99)00022-0. [DOI] [Google Scholar]
- Chen Y, Bagnall D and Yao T. 2000. Mater. Sci. Eng. B 75 190 10.1016/S0921-5107(00)00372-X [DOI] [Google Scholar]
- Liang S, Sheng H, Liu Y, Hio Z, Lu Y. and Chen H. J. Cryst. Growth. 2001;225:110. doi: 10.1016/S0022-0248(01)00830-2. [DOI] [Google Scholar]
- Saito N, Haneda H, Sekiguchi T, Ohashi N, Sakaguchi I. and Koumoto K. Adv. Mater. 2002;14:418. doi: 10.1002/1521-4095(20020318)14:6<418::AID-ADMA418>3.0.CO;2-K. [DOI] [Google Scholar]
- Lee J Y, Choi Y S, Kim J H, Park M O. and Im S. Thin Solid Films. 2002;403:533. doi: 10.1016/S0040-6090(01)01550-4. [DOI] [Google Scholar]
- Mitra A, Chatterjee A P. and Maiti H S. Mater. Lett. 1998;35:33. doi: 10.1016/S0167-577X(97)00215-2. [DOI] [Google Scholar]
- Koch M H, Timbrell P Y. and Lamb R N. Semicond. Sci. Technol. 1995;10:1523. doi: 10.1088/0268-1242/10/11/015. [DOI] [Google Scholar]
- Gratzel M. MRS Bull. 2005;30:39374. [Google Scholar]
- Baxter J B, Walker A M, van Ommering K. and Aydil E S. Nanotechnology. 2006;17:S304. doi: 10.1088/0957-4484/17/11/S13. [DOI] [Google Scholar]
- Lin Y, Zhang Z, Tang Z, Yuan F. and Li J. Adv. Mater. Opt. Electron. 1999;9:205. doi: 10.1002/1099-0712(199909/10)9:5<205::AID-AMO383>3.0.CO;2-8. [DOI] [Google Scholar]
- Padmavathy N. and Vijayaraghavan R. Sci. Technol. Adv. Mater. 2008;9:035004. doi: 10.1088/1468-6996/9/3/035004. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Iijima S. Nature. 1991;354:56. doi: 10.1038/354056a0. [DOI] [Google Scholar]
- Cui Y, Lauhon L J. and Gudiksen M S. Appl. Phys. Lett. 2001;78:2214. doi: 10.1063/1.1363692. [DOI] [Google Scholar]
- Burghard G M, Kim G T, Dusberg G S, Chiu P W, Krstic V, Roth S. and Han W Q. J. Appl. Phys. 2001;90:5747. doi: 10.1063/1.1413495. [DOI] [Google Scholar]
- Duan X, Huang Y, Cui Y, Wang J. and Lieber C M. Nature. 2001;409:66. doi: 10.1038/35051047. [DOI] [PubMed] [Google Scholar]
- Bai Z G, Yu D P, Zhang H Z, Ding Y, Gai S Q, Hang X Z, Hiong Q L. and Feng G C. Chem. Phys. Lett. 1999;303:311. doi: 10.1016/S0009-2614(99)00066-4. [DOI] [Google Scholar]
- Huang M H, Wu Y, Feick H, Tran N, Webe E. and Yang P. Adv. Mater. 2001;13:113. doi: 10.1002/1521-4095(200101)13:2<113::AID-ADMA113>3.0.CO;2-H. [DOI] [Google Scholar]
- Huang M H, Mao S, Feick H, Yan H, Wu Y, Kind H, Weber E, Russo R. and Yang P. Science. 2001;292:1897. doi: 10.1126/science.1060367. [DOI] [PubMed] [Google Scholar]
- Shi G, Mo C M, Cai W L. and Zhang L D. Solid State Commun. 2005;115:253. doi: 10.1016/S0038-1098(00)00169-1. [DOI] [Google Scholar]
- Baruah S, Thanachayanont C. and Dutta J. Sci. Technol. Adv. Mater. 2008;9:025009. doi: 10.1088/1468-6996/9/2/025009. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Huang Y, Zhang Y, Bai X, He J, Liu J. and Zhang X. J. Nanosci. Nanotechnol. 2006;6:2566. doi: 10.1166/jnn.2006.545. [DOI] [PubMed] [Google Scholar]
- Hughes W L. and Wang Z L. Appl. Phys. Lett. 2005;86:043106. doi: 10.1063/1.1853514. [DOI] [Google Scholar]
- Kong X Y. and Wang Z L. Nano Lett. 2003;3:1625. doi: 10.1021/nl034463p. [DOI] [Google Scholar]
- Hughes W L. and Wang Z L. J. Am. Chem. Soc. 2004;126:6703. doi: 10.1021/ja049266m. [DOI] [PubMed] [Google Scholar]
- Sun T, Qiu J and Liang C. 2008. J. Phys. Chem. C 112 715 10.1021/jp710071f [DOI] [Google Scholar]
- Snure M. and Tiwari A. J. Nanosci. Nanotechnol. 2007;7:485. doi: 10.1166/jnn.2007.139. [DOI] [PubMed] [Google Scholar]
- Wang Z L. J. Phys.: Condens. Matter. 2004;16:R829. doi: 10.1088/0953-8984/16/25/R01. [DOI] [Google Scholar]
- Spanhel L. J. Sol–Gel Sci. Technol. 2006;39:7. doi: 10.1007/s10971-006-7302-5. [DOI] [Google Scholar]
- Ma X, Zhang H, Ji Y, Xu J. and Yang D. Mater. Lett. 2005;59:3393. doi: 10.1016/j.matlet.2005.05.076. [DOI] [Google Scholar]
- Kohls M, Bonnani M. and Spanhel L. Appl. Phys. Lett. 2002;81:3858. doi: 10.1063/1.1518774. [DOI] [Google Scholar]
- Xu H Y, Wang H, Zhang Y C, Wang S, Zhu M. and Yan H. Cryst. Res. Technol. 2003;38:429. doi: 10.1002/crat.200310053. [DOI] [Google Scholar]
- Shingubara S. J. Nanoparticle Res. 2003;5:17. doi: 10.1023/A:1024479827507. [DOI] [Google Scholar]
- Krunks M. and Mellikov E. Thin Solid Films. 1995;270:33. doi: 10.1016/0040-6090(95)06893-7. [DOI] [Google Scholar]
- Ayouchi R, Martin F, Leinen D. and Ramos-Barrado J R. J. Cryst. Growth. 2003;247:497. doi: 10.1016/S0022-0248(02)01917-6. [DOI] [Google Scholar]
- Wang Y C, Leu I C, Chung Y W. and Hon M H. Nanotechnology. 2006;17:4445. doi: 10.1088/0957-4484/17/17/027. [DOI] [Google Scholar]
- Tang C C, Fan S S, Lamy de la, Chapelle M. and Li P. Chem. Phys. Lett. 2001;333:12. doi: 10.1016/S0009-2614(00)01326-9. [DOI] [Google Scholar]
- Pan Z W, Dai Z R. and Wang Z L. Science. 2001;291:1947. doi: 10.1126/science.1058120. [DOI] [PubMed] [Google Scholar]
- Wang Z and Li H L. 2002. Appl. Phys. A 74 201 10.1007/s003390100856 [DOI] [Google Scholar]
- Miao L, Ieda Y, Tanemura S, Cao Y G, Tanemura M, Hayashi Y, Toh S. and Kaneko K. Sci. Technol. Adv. Mater. 2007;8:443. doi: 10.1016/j.stam.2007.02.012. [DOI] [Google Scholar]
- Dalal S H, Baptista D L, Teo K B K, Lacerda R G, Jefferson D A. and Milne W I. Nanotechnology. 2006;17:4811. doi: 10.1088/0957-4484/17/19/005. [DOI] [Google Scholar]
- Satoh Y, Ohshio S. and Saitoh H. Sci. Technol. Adv. Mater. 2005;6:215. doi: 10.1016/j.stam.2004.11.017. [DOI] [Google Scholar]
- Yasuda T and Segawa Y. 2004. Phys. Status Solidi b 241 676 10.1002/pssb.200304209 [DOI] [Google Scholar]
- Li Z W. and Gao W. Thin Solid Films. 2007;515:3323. doi: 10.1016/j.tsf.2006.09.026. [DOI] [Google Scholar]
- Lagashetty A, Havanoor V, Basavaraja S, Balaji S D. and Venkataraman A. Sci. Technol. Adv. Mater. 2007;8:484. doi: 10.1016/j.stam.2007.07.001. [DOI] [Google Scholar]
- Tokumoto M, Briois V, Santili C V. and Pulcinelli S H. J. Sol–Gel Sci. Technol. 2003;26:547. doi: 10.1023/A:1020711702332. [DOI] [Google Scholar]
- Baruwati B, Kumar D K and Manorama S V. 2006. Sensors Actuators B 119 676 10.1016/j.snb.2006.01.028 [DOI] [Google Scholar]
- Lu C H. and Yeh C H. Ceram. Int. 2000;26:351. doi: 10.1016/S0272-8842(99)00063-2. [DOI] [Google Scholar]
- Chen D, Jiao X. and Cheng G. Solid State Commun. 2000;113:363. doi: 10.1016/S0038-1098(99)00472-X. [DOI] [Google Scholar]
- Musić S, Popović S, Maljković M. and Dragčević D. J. Alloys Compd. 2002;347:324. doi: 10.1016/S0925-8388(02)00792-2. [DOI] [Google Scholar]
- Vishwanathan R. and Gupta R B. J. Supercritical Fluids. 2003;27:187. doi: 10.1016/S0896-8446(02)00236-X. [DOI] [Google Scholar]
- Baruah S, Rafique R F and Dutta J. 2008. Nano at press [Google Scholar]
- Andres-Vergés M, Mifsud A. and Serna C J. J. Chem. Soc. Faraday Trans. 1990;86:959. doi: 10.1039/ft9908600959. [DOI] [Google Scholar]
- Vayssieres L, Keis K and Lindquist S E. 2001. J. Phys. Chem. B 105 3350 10.1021/jp010026s [DOI] [Google Scholar]
- Schmidt-Mende L. and MacManus-Driscoll J L. Mater. Today. 2007;10:40. doi: 10.1016/S1369-7021(07)70078-0. [DOI] [Google Scholar]
- Ashfold M N R, Doherty R P, Ndifor-Angwafor N G, Riley D J. and Sun Y. Thin Solid Films. 2007;515:8679. doi: 10.1016/j.tsf.2007.03.122. [DOI] [Google Scholar]
- Govender K, Boyle D S, Kenway P B. and O'Brien P. J. Mater. Chem. 2004;14:2575. doi: 10.1039/b404784b. [DOI] [Google Scholar]
- Sugunan A, Warad H C, Boman M. and Dutta J. J. Sol–Gel Sci. Technol. 2006;39:49. doi: 10.1007/s10971-006-6969-y. [DOI] [Google Scholar]
- Vayssieres L, Keis K, Lindquist S E and Hagfeldt A. 2001. J. Phys. Chem. B 105 3350 10.1021/jp010026s [DOI] [Google Scholar]
- Vayssieres L. Adv. Mater. 2003;15:464. doi: 10.1002/adma.200390108. [DOI] [Google Scholar]
- Sun Y, Riley D J and Ashfold M N R. 2006. J. Phys. Chem. B 110 15186 10.1021/jp062299z [DOI] [PubMed] [Google Scholar]
- Tian Z R, Voigt J A, Liu J, Mckenzie B, Mcdermott M J, Rodriguez M A, Konishi H. and Xu H. Nat. Mater. 2003;2:821. doi: 10.1038/nmat1014. [DOI] [PubMed] [Google Scholar]
- Pal U and Santiago P. 2005. J. Phys. Chem. B 109 15317 10.1021/jp052496i [DOI] [PubMed] [Google Scholar]
- Tang L, Bao X-B, Zhou H and Yuan A-H. 2008. Physica E 40 924 10.1016/j.physe.2007.11.024 [DOI] [Google Scholar]
- Li F, Hu L, Li Z. and Huang X. J. Alloys Compd. 2007;465:L14. doi: 10.1016/j.jallcom.2007.11.009. [DOI] [Google Scholar]
- Zhang X Y, Dai J Y, Ong H C, Wang N, Chan H L W. and Choy C L. Chem. Phys. Lett. 2004;393:17. doi: 10.1016/j.cplett.2004.06.012. [DOI] [Google Scholar]
- Chen Y, Yu R, Shi Q, Qin J. and Zheng F. Mater. Lett. 2007;61:4438. doi: 10.1016/j.matlet.2007.02.028. [DOI] [Google Scholar]
- Ni Y H, Wei X-W, Ma X. and Hong J-M. J. Cryst. Growth. 2005;283:48. doi: 10.1016/j.jcrysgro.2005.05.048. [DOI] [Google Scholar]
- Zhao D Y, Feng J L, Huo Q S, Melosh N, Fredrickson G H, Chmelka B F. and Stucky G D. Science. 1998;279:548. doi: 10.1126/science.279.5350.548. [DOI] [PubMed] [Google Scholar]
- Yang P D, Deng T, Zhao D Y, Feng P Y, Pine D, Chmelka B F, Whitesides G M. and Stucky G D. Science. 1998;282:2244. doi: 10.1126/science.282.5397.2244. [DOI] [PubMed] [Google Scholar]
- Melosh N A, Davidson P. and Chmelka B F. J. Am. Chem. Soc. 2000;122:823. doi: 10.1021/ja992801b. [DOI] [PubMed] [Google Scholar]
- Yu C Z, Tian B, Fan J, Stucky G D. and Zhao D Y. J. Am. Chem. Soc. 2002;124:4556. doi: 10.1021/ja025548f. [DOI] [PubMed] [Google Scholar]
- Zhang R, Liu J, Han B X, He J, Liu Z M. and Zhang J L. Langmuir. 2003;19:8611. doi: 10.1021/la0352265. [DOI] [Google Scholar]
- Zhang Z. and Mu J. J. Colloid Interface Sci. 2007;307:79. doi: 10.1016/j.jcis.2006.10.035. [DOI] [PubMed] [Google Scholar]
- Peterson R B, Fields C L. and Gregg B A. Langmuir. 2004;20:5114. doi: 10.1021/la049683c. [DOI] [PubMed] [Google Scholar]
- Wang Z, Qian X-F, Yin J. and Zhu Z-K. J. Solid State Chem. 2004;177:2148. [Google Scholar]
- Li W J, Shi E W, Zhong W Z. and Yin Z W. J. Cryst. Growth. 1999;203:186. doi: 10.1016/S0022-0248(99)00076-7. [DOI] [Google Scholar]
- Zhang J, Sun L D, Yin J L, Su H L, Liao C S. and Yan C H. Chem. Mater. 2002;14:4172. doi: 10.1021/cm020077h. [DOI] [Google Scholar]
- Li Z, Huang X, Liu J, Li Y, Ji X. and Li G. Mater. Lett. 2007;61:4362. doi: 10.1016/j.matlet.2007.02.003. [DOI] [Google Scholar]
- Wahab R, Ansari S G, Kim Y S, Seo H K, Kim G S, Khang G. and Shin H-S. Mater. Res. Bull. 2007;42:1640. doi: 10.1016/j.materresbull.2006.11.035. [DOI] [Google Scholar]
- Shao S, Jia P, Liu S. and Bai W. Mater. Lett. 2008;62:1200. doi: 10.1016/j.matlet.2007.08.049. [DOI] [Google Scholar]
- Li F, Hu L, Li Z. and Huang X. J. Alloys Compd. 2008;465:L14. doi: 10.1016/j.jallcom.2007.11.009. [DOI] [Google Scholar]
- Jang J M, Kim S D, Choi H M, Kim J Y and Jung W G. 2008. Mater. Chem. Phys. doi: 10.1016/j.matchemphys.2008.07.108 [DOI] [Google Scholar]
- Gedye R, Smith F, Westaway K, Humera A, Baldisera L, Laberge L. and Rousell L. Tetrahedron Lett. 1986;27:279. doi: 10.1016/S0040-4039(00)83996-9. [DOI] [Google Scholar]
- Zhu Y J, Wang W W, Qi R J. and Hu X L. Angew. Chem., Int. Ed. Engl. 2004;43:1410. doi: 10.1002/anie.200353101. [DOI] [PubMed] [Google Scholar]
- Tsuji M, Hashimoto M, Nishizawa Y, Kubokawa M. and Tsuji T. Chem. Eur. J. 2005;11:440. doi: 10.1002/chem.200400417. [DOI] [PubMed] [Google Scholar]
- Ma M-G, Zhu Y J, Cheng G F. and Huang Y H. Mater. Lett. 2007;62:507. doi: 10.1016/j.matlet.2007.05.072. [DOI] [Google Scholar]
- Vijayan T A, Chandramohan R, Valanarasu S, Thirumalai J, Venkateswaran S, Mahalingam T. and Srkumar S R. Sci. Technol. Adv. Mater. 2008;9:035007. doi: 10.1088/1468-6996/9/3/035007. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Jung S W, An S-J, Yi G C, Jung C U, Lee S-I. and Cho S. Appl. Phys. Lett. 2002;80:4561. doi: 10.1063/1.1487927. [DOI] [Google Scholar]
- Cheng X M. and Chien C L. J. Appl. Phys. 2003;93:7876. doi: 10.1063/1.1556125. [DOI] [Google Scholar]
- Yoon S W, Cho S-B, We S C, Yoon S, Suh B J, Song H K. and Shin Y J. J. Appl. Phys. 2003;93:7879. doi: 10.1063/1.1556126. [DOI] [Google Scholar]
- Fukumura T, Jin Z, Kawasaki M, Shono T, Hasegawa T. and Koinuma H. Appl. Phys. Lett. 2001;78:958. doi: 10.1063/1.1348323. [DOI] [Google Scholar]
- Robers B K, Pakhomov A B, Shutthanandan V S. and Krishnan K M. J. Appl. Phys. 2005;97:10D310. doi: 10.1063/1.1847914. [DOI] [Google Scholar]
- Bae S Y, Na C W, Kang J H and Part J. 2005. J. Phys. Chem. B 109 2526 10.1021/jp0458708 [DOI] [PubMed] [Google Scholar]
- Cimitan S, Albonetti S, Forni L, Peri F. and Lazzari D. J. Colloid Interface Sci. 2009;329:73. doi: 10.1016/j.jcis.2008.09.060. [DOI] [PubMed] [Google Scholar]
- Majumder S B, Jain M, Dobal P S and Katiyar R S. 2003. Mater. Sci. Eng. B 103 16 10.1016/S0921-5107(03)00128-4 [DOI] [Google Scholar]
- Xu C, Kim M, Chun J. and Kim D. Appl. Phys. Lett. 2005;86:133107. doi: 10.1063/1.1888035. [DOI] [Google Scholar]
- Zuo J, Xu C, Zhang L, Xu B. and Wu R. J. Raman Spectrosc. 2001;32:979. doi: 10.1002/jrs.761. [DOI] [Google Scholar]
- Agne T, Guan Z, Li X M, Wolf H, Wichert T, Natter H. and Hempelmann R. Appl. Phys. Lett. 2003;83:1204. doi: 10.1063/1.1598289. [DOI] [Google Scholar]
- Li D, Liu Z T, Leung Y H, Djurisic A B, Xie M H. and Chan W K. J. Phys. Chem. Solids. 2008;69:616. doi: 10.1016/j.jpcs.2007.07.080. [DOI] [Google Scholar]
- Yuhas B D, Zitoun D O, Pauzauskie P J, He R. and Yang P. Angew. Chem., Intl. Ed. Engl. 2006;45:420. doi: 10.1002/anie.200503172. [DOI] [PubMed] [Google Scholar]
- Piticescu R R, Piticescu R M. and Monty C J. J. Eur. Ceram. Soc. 2006;26:2979. doi: 10.1016/j.jeurceramsoc.2006.02.015. [DOI] [Google Scholar]
- Morales A E, Zaldivar M H. and Pal U. Opt. Mater. 2006;29:100. doi: 10.1016/j.optmat.2006.03.010. [DOI] [Google Scholar]