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Optimization, Yield Studies and Morphology of WO3Nano-Wires Synthesized by Laser Pyrolysis in C2H2and O2Ambients—Validation of a New Growth Mechanism
Nanoscale Research Letters volume 3, Article number: 372 (2008)
Laser pyrolysis has been used to synthesize WO3nanostructures. Spherical nano-particles were obtained when acetylene was used to carry the precursor droplet, whereas thin films were obtained at high flow-rates of oxygen carrier gas. In both environments WO3nano-wires appear only after thermal annealing of the as-deposited powders and films. Samples produced under oxygen carrier gas in the laser pyrolysis system gave a higher yield of WO3nano-wires after annealing than the samples which were run under acetylene carrier gas. Alongside the targeted nano-wires, the acetylene-ran samples showed trace amounts of multi-walled carbon nano-tubes; such carbon nano-tubes are not seen in the oxygen-processed WO3nano-wires. The solid–vapour–solid (SVS) mechanism [B. Mwakikunga et al., J. Nanosci. Nanotechnol., 2008] was found to be the possible mechanism that explains the manner of growth of the nano-wires. This model, based on the theory from basic statistical mechanics has herein been validated by length-diameter data for the produced WO3nano-wires.
Amongst many transition metal oxides, WO3 has excellent electro-chromic, gaso-chromatic and photo-chromatic properties. At room temperature it adopts the distorted monoclinic structure of ReO3. For this reason, WO3 has been used to construct flat panel displays, photo–electro–chromic ‘smart’ windows [2–4], writing–reading–erasing optical devices [5, 6], optical modulation devices [7, 8], gas sensors and humidity and temperature sensors [9–11]. Self assembly of these materials has been achieved by hydrothermal techniques, additive-free hydrothermal means, templating either with a polymer or pre-assembled carbon nano-tubes, epitaxial growth, sol-gel, electro-chemical means and hot-wire CVD methods. Recently, WO3 nano-rods produced by a facile chemical route and CVD have been reported [12, 13] in this journal. In laser pyrolysis, authors have reported synthesis of, for instance, ceramics, silicon and silicon compounds, carbon compounds, olefins, chromium oxides, diamond, fullerenes and many other classes of materials. These experiments have largely been performed at high laser powers and hence at high temperatures. At such high levels, where anharmonicity cannot be ruled out, laser pyrolysis is equivalent to traditional pyrolysis with the photo-thermal process overwhelming the photo-chemical one. However, it has long been realized that even at low intensity, the CO2 laser has successfully been used in the synthesis of boron compounds from BCl3 [14, 15]. At these low power values, the laser is used to selectively excite the reactant to a relatively low vibrational level from which a chemical reaction with other reactants present is initiated. One expects to achieve product formation distinctly different from that achieved by traditional pyrolysis for the same chemical reaction provided that the laser energy absorbed is channelled mainly into the chemical process rather than into heating.
In this Letter, we report optimization of parameters that led to the synthesis of WO3nano-spheres and thin films at relatively low laser power (50 W in a 2.4-mm focal region). We demonstrate the role of thermal annealing in the conversion of the spheres and slabs into nano-wires. We also show the morphological differences and yields when carrier gases—C2H2or O2—are used during the synthesis.
Our laser pyrolysis experimental set up was fully described in our previous publication . Briefly, the method involves injecting a stream of very fine droplets of a precursor solution into an infrared laser beam and depositing the resulting aerosol onto a Corning glass substrate. A wavelength tuneable continuous wave (cw) CO2 laser was used in the experiments (Edinburgh Instruments, model PL6). By selecting a wavelength of 10.6 μm, the laser was within, but not exactly on, the absorption region of the pre-made precursor (WCl6 in ethanol or tungsten ethoxide) for the production of WO3. From the fact that (1) the excitation wavelength of 10.6 μm is not exactly at the main resonance peak of the W-ethoxide precursor of 9.44 μm and (2) the laser power of 50 W (focussed into 2.4-mm beam diameter at the waist) is not low enough to rule out anharmonic effects in the excitation, the decomposition of this precursor could be due to both photochemical (resonance) and photo-thermal (anharmonic) processes. The as-produced materials showed decomposition of W-ethoxide into WO3 nano-particles suggesting that the photo-chemical process indeed occurred. Also worth describing here is the carrier gas system which is accomplished by a three-way nozzle having three concentric cylinders. The outer cylinder is connected to an argon supply. The argon guides the aerosol droplets which are carried by either C2H2 (supposedly non-reactive) or O2 (highly reactive) gases interchangeably in the middle and second cylinder. This is illustrated in Fig. 1.
An aliquot of 5.4 mg of dark blue powder of WCl6 (Aldrich 99.99%) was dissolved in 500 mL of ethanol. Since WCl6 is highly reactive with air and moisture, its dissolution was conducted in an argon atmosphere. Particles from this process were collected on Corning glass substrates, placed on a rotating stage, at room temperature and at atmospheric pressure. The particle deposition showed a void at the centre (Fig. 1b) when the encapsulating carrier gas flow-rate was higher than the carrier gas driving the precursor droplets. When the flow-rates were reversed, the deposition showed the profile of a hump (Fig. 1a) showing there was more deposition at the centre of the substrate than in periphery. This was found to be in agreement with Bernoulli’s theorem, which requires that there should be reduced pressure in fast flowing fluids. When the flow rate of the central gas is larger, the pressure is lower in this region and hence the droplets and the particles (after laser pyrolysis) are trapped in this low pressure region. Therefore there is high deposition at the centre of the substrate and vice versa. Table 1 lists the experimental procedures employed. The so-obtained samples were further annealed in argon atmosphere at 500 °C for 17 h. Morphology studies were carried out using a Jeol JSM-5600 scanning electron microscopy (SEM) microscope, which was also equipped for energy dispersive X-ray spectroscopy (EDX). In order to avoid charging effects during SEM analysis, the samples were made conductive by carbon/Au/Pd coating. Infrared and Raman spectroscopy experiments on the as-obtained WO3 are reported elsewhere . Structural studies were done using a Philips Xpert powder diffractometer equipped with a CuKα wavelength of 0.154184 nm. The experimental procedure showed good reproducibility of results.
Lengths and corresponding diameters of the nano-wires were measured by means of a software package ImageTool. As is the required procedure, calibration is initially made against the marker of known length in both the image scale and the real space scale. Then the distance between two points is measured for each point with accuracy that heavily depends on (1) the pixel density of the projecting screen, (2) the random errors from operator’s hand and (3) the magnification of the image.
Laser pyrolysis of tungsten-based precursors, with C2H2 as carrier gas, shows remarkable differences in morphology from when O2 is the carrier gas as shown in Figs. 2 and 3. The C2H2-synthesized sample has a lower yield of WO3 nano-wires after annealing than the O2-synthesized one. These nano-wires in O2-ran sample grow in the crevices of the film. The C2H2-ran sample has nano-wires with a higher aspect ratio than the O2-ran samples. Also the C2H2-ran sample shows the presence of spherical micro-particles where as complete absence of these spheres is observed in the O2-ran sample. This means that C2H2 maintains the spherical shape of the precursor droplets, which is clear evidence that C2H2 is only a sensitizer of the process but does not participate in the decomposition of the precursor. Also, in the presence of tungsten, C2H2 dissociates and forms carbon structures such as carbon nano-tubes. It was shown that vanadium surfaces can be used as catalysts for the growth of carbon nano-tubes  from C2H2. On the other hand, O2 actively participates in the breakdown of the precursor droplets and in the process increases the yield of the WO3 nano-wires at the expense of aspect ratio of the wires in general. The O2-ran sample also has very brittle thin films with cracks in a somewhat ordered manner. This ordered cracking after annealing could be attributed to the growth pressure (thermal stress) from the 1D nano-structures.
The TEM micrograph of a typical wire grown from O2-run WO3particles shown in Fig. 4b revealed a core-shell structure (redrawn in Fig. 4c) with the WO x wire at the core (EDS in Fig. 4a) and the carbon–Au–Pd composite around the wire as a shell (EDS in Fig. 4e). C–Au–Pd is a material used in the prior-to-SEM coating to improve conduction for enhanced imaging. The shell is thicker on one side than on the other; that is, the wire is not centred through the C–Au–Pd wrapping. This shell served as a contamination, which obscured the electron diffraction of the wire so that the stoichiometry studies of the WO x nano-wire could not be accomplished. In line with our previous studies, we can speculate that the wire is WO x withx being less than three due to oxygen loss during annealing even as elaborated in chemical reactions of the type in Eq. 4.
In order to observe the growth of nano-wires, we sonicated a few spheres of WO3into iso-propanol and placed them on carbon-holey Cu grid for in-situ annealing and imaging in a Jeol CM200 transmission electron microscope. A series of images, shown in Fig. 5, were taken periodically of intervals of 45 min whilst heating at temperatures ranging from 700 °C to 900 °C using a heating device specially tailored for this microscope. The images showed no indication of growth of one-dimensional structures. This is attributed to the vacuum typical of TEM. Any atoms that are sublimated from the spheres are immediately removed by the high vacuum giving a very small probability of condensing and growing into 1D nano-structured geometry. However, the shrinking of the spheres is an indication that the atoms are indeed evaporating from the surface. However, not all sublimated atoms are removed from their parent spheres; some return to make small mounds on the sphere surface making the sphere rougher. The rate of sphere size reduction due to loss of atoms is depicted in Fig. 5b. It is interesting to note that the smaller sphere C shrank faster than the larger sphere B. This means that wires grown from small spheres grow faster than those that grow from large spheres.
For us to understand the novel growth of these nano-wires, it is important to briefly review some related growth mechanisms available in literature. Sir Frederick Frank proposed the ‘screw dislocation theory’ in 1949. Central to this dislocation theory were Polanyi, Orowan, Taylor, Burger and Mott & Nabarro . Defects and dislocation in the initial crystals initiate one-dimensional growth; “…the crystal face always has exposed molecular terraces on which growth can continue, and the need for fresh 2D nucleation never arises…” . In 1964, detailed studies on the morphology and growth of silicon whiskers by Wagner & Ellis  led to a new concept of crystal growth from vapour, which was called the vapour–liquid–solid (VLS) mechanism. The new growth mechanism was built around three important facts: (a) silicon whiskers did not contain an axial screw dislocation (b) an impurity was essential for whisker growth and (c) a small globule was always present at the tip of the whisker during growth. From fact (a), it was clear that growth from vapour did not occur according to Frank’s screw dislocation theory and from, facts (b) and (c), it was important that a new growth mechanism be studied.
In 1975, Givarzigozov  introduced the fundamental aspects of the VLS mechanism. Emphasis was placed on the dependence of the growth rate on the whisker diameter. It was found that the growth rate decreased abruptly for submicron diameters and vanished at some critical diameter d c ≤ 0.1 μ m in accordance with the Gibbs–Thomson effect. Basing on this effect, which states that the solubility limit of a precipitate (β) in a matrix (α) varies with the precipitate’s radius, Givarzigozov suggested that the effective difference between the chemical potential of the precipitate in the vapour phase and in the terminal precipitate [whisker], Δμ, is given by
Δμ 0 is the difference at a plane boundary (when diameter,D, of the precipitate tends to ∞), Λ is the atomic volume of the precipitate andσ is the surface free energy of the precipitate. The dependence of growth rate, G, on the super-saturation (Δμ/k B T) given byV = b(Δμ/k B T)n, whereb andn are coefficients to be evaluated from experimental data, was used to derive an expression
The main characteristics of VLS mechanism are (1) the presence of a catalyst and (2) direct proportionality of the diameter of the nanostructure to the growth rate. Thick whiskers grow longer than thinner ones because this growth can be afforded by the continual supply of building blocks in the CVD system. Plotting the growth rate, V,  or terminal length l ∞  of the whisker versus D gives curves with a positive ascent. A plot of V 1/n versus 1/D gives a straight line graph with a negative slope .
Recently, an in situ growth profile in real time for tungsten oxide nano-wires was followed by Kasuya et al. (2008)  by injecting ultra-small flow-rates of O2 on a heated tungsten surface placed on a scanning electron microscope stage. It was difficult to ascertain if the length-and-diameter data would be in agreement with the VLS mechanism because the images were rather poor. This was due to the poor vacuum caused by the intentional injection of O2, which was useful for the targeted reaction. The length of the nano-wire as a function time l(t) was found to take the form of
where l 0 is the final length and α is the growth or decay coefficient.
We however study the final state of the fully grown WO3 nanostructures. Our present length-diameter data for the nano-wires could not agree with the above VLS theory for two conflicting reasons: (1) no particular catalyst could be identified with certainty (2) we found an inverse proportionality between length and diameter of the nano-wires. It was therefore important to study a new model to attempt to explain the new findings. Since the production of solid-state nano-wires is after annealing of the solid-state particles, the mechanism of growth can neither be according to liquid-based “Solution-Liquid-Solid” mechanism proposed by Trenter and Buhro [24, 25] nor in line with the “Super-Critical Fluid Synthesis” mechanism proposed by Holmes  and which has been later supported by Korgel and co-workers . These data certainly support our newly proposed “Solid–Vapour–Solid (SVS)” mechanism reported in our previous publication  where we reported solid-state W18O49 nano-tips produced by annealing solid-state WO3 nano-spheres (prepared by ultrasonic spray pyrolysis) in argon environment. Synthesis of solid materials from solid precursors is not new. Solid-state reactions are very slow and difficult to carry out to completion unless carried out at very high temperatures where reacting atoms can diffuse through solid material to the reaction front more easily. Transformation of one phase to another (with the same chemical composition) can also occur in solid state, either at elevated temperatures or elevated pressures (or both). For the growth rate of many solid-state reactions (including tarnishing), inter-diffusion of ions through the product layer increases the thickness Δx parabolically with time (Δx)2 ∝ t. This is a sharply different dependence from the Eq. 1 proposed by Kasuya et al.  above. In some solid-state processes, nucleation can be homogeneous. This is often the case for thermal decomposition, for example, as is the case in the current reactions
In this Letter, we introduce for the first time the statistical-mechanical aspects of this proposed SVS model and fit the ensuing mathematical expressions to the data.
For the sake of simplicity, we consider the source of molecules to be a solid sphere of radius R 0, containing molecules of mass, M and assume the molecules to be spherical of average molecular diameter, Ω. We assume further that in changing the morphology from a sphere to a wire, only the surface molecules can migrate from the sphere to the newly forming wire or rod. For instance it has been demonstrated  that the surface diffusive flux, J S of atoms on a surface of a slab of length L given by J S = −(dc/dx)∫0 L D(y)dy is different from the more familiar bulk diffusive flux written from the first Fick’s law as J B = −D B(dc/dx)L where dc/dx is the concentration gradient. In this case, transformation from sphere to rod takes place layer after layer. The sphere shrinks but the as-forming rod lengthens as illustrated in Fig. 6.
If the sphere is amorphous and the wire is crystalline as normally observed experimentally, then the densities of the material in the initial sphere and the final wire are different and can be written, respectively, asρ am and ρ cryst. The number of atoms in the first layer of the sphere can therefore be written as
If all these atoms assemble into a rod of diameter D and length l 1 then the number of molecules in the rod can be written in terms of lengthl 1 as
However, not all the atoms in Eq. 5end up making the rod. The actual fraction that self-assembles into the rod is proportional to the Boltzmann’s fraction, which depends on the temperatureT of the ambient given as
E A is the activation energy of the atoms.
After the first layer has assembled into the rod of lengthl 1, the next layer in the sphere has a radius ofR 0 −Ω which forms the next segment of the rod of lengthl 2. The subsequent layers have radii ofR 0 − 2Ω,R 0 − 3Ω,R 0 − 4Ω,R 0 − 5Ω and so forth. Thei th layer will have a radius ofR 0 −(i− 1)Ω such that the number of atoms in thei th layer is
This corresponds to the number of atoms in the i th segment of the rod of length l i given as
The total length of the wire is a summation of all the segments of the wire emanating from each corresponding layer in the source sphere.
Parameter ζ is a function of temperature T and also depends on the geometry of the source of the atoms. The higher the annealing temperature, T, the higher the slope, ζ. This fact may mean that thinner nano-wires can be obtained at higher annealing temperatures. But there must be a lower limit to how thinner the nano-wires can get in the SVS mechanism since at much higher temperatures all solid-state starting material should evaporate away leaving nothing to form the nano-wires with. These limits are yet to be determined. The same question has been asked if there is a thermo-dynamical lower limit to the nano-wires growth by VLS . It can be seen that if the source is equally crystalline then the ratio of the densities in the source to the final structure is unity. By quick inspection, one can see that the geometry described by the summation in Eq. 11 is proportional to the total surface area of all atomic or molecular layers in the source. A plot of l versus 1/D 2 should be a positive straight line graph with a y-intercept of zero and a slope of ζ. Similarly a plot of aspect ratios l/D versus 1/D 3 is supposed to be a positive straight line going through the origin and having the slope, ζ.
In the VLS mechanism, given a constant flux of molecules in the source, a nano-wire that has a large diameter will grow much longer compared to when it starts out with a small diameter. In the SVS growth, the thinner the wire the longer it is and vice versa as shown in the plots of Fig. 7a. When aspect ratios, defined here as the ratio of length to diameter, is plotted against diameter, the same profile is obtained (Fig. 7b). When length and aspect ratio are plotted against 1/D 2 and 1/D 3, respectively, in accordance with Eq. 10, positive slopes are manifested (Fig. 8) almost equal to each other as expected from the above theory and of the order of ~ 10−20 m 3. This value is related to the order of magnitude of the average volume of the WO3 nano-wires. It should be noted that reverse growth from one-dimensional to spherical particles is also possible at suitable annealing conditions. For instance, nano-belts of Zn acetate were converted into aggregates of ZnO nano-particles as reported in this journal .
In summary, liquid atomization and subsequent laser pyrolysis were carried out using a CO2 laser tuned at its 10P20 line of wavelength 10.6 μm. SEM characterization of the as-produced WO3 samples showed that selective photochemical reactions by the laser have a part to play in initiating self assembly growth centres even without the need for a catalyst. Self assembly is only continued by further annealing. We have shown that oxygen carrier gas gives a higher yield of WO3 nano-wires by laser pyrolysis than acetylene. The latter also shows trace amounts of multi-walled carbon nano-tubes. The transmission electron microscopy reveals that the nano-wires are core-shell structures of a mixture of Au, Pd and C in the shell and WO3 at the core. The shell is due to the prior-to-SEM coating to improve imaging. The absence of catalysts in addition to the analysis of the nano-wire length-and-diameter data has validated a new growth mechanism, which we have called SVS growth as proposed earlier .
Cox PA: Transition Metal Oxides: An Introduction to Their Electronic Structure and Properties. Oxford University Press, Oxford; 1992.
Granqvist CG, Azens A, Hjelm A, Kullman L, Niklasson GA, Rönnow D, et al.: Sol. Energy. 1998, 63: 199. COI number [1:CAS:528:DyaK1cXotV2gsb4%3D] 10.1016/S0038-092X(98)00074-7
Granqvist CG, Avendano E, Azens A: Thin Solid Films. 2003, 442: 201. COI number [1:CAS:528:DC%2BD3sXnsVaju7k%3D] 10.1016/S0040-6090(03)00983-0
Hoel A, Reyes LF, Heszler P, Lantto V, Granqvist CG: Curr. Appl. Phys.. 2004, 4: 547. 10.1016/j.cap.2004.01.016
Bendahan M, Boulmani R, Seguin JL, Aguir K: Sens. Actuators. 2004, 100: 320. 10.1016/j.snb.2004.01.023
R.F. Mo, G.Q. Jin, X.Y. Guo, Mater. Lett. doi:10.1016/j.matlet.2006.12.061
Shigaya Y, Nakayama T, Aono M: Sci. Technol. Adv. Mater.. 2004, 5: 647. 10.1016/j.stam.2004.02.021
Gillet M, Aguir K, Bendahan M, Mennini P: Thin Solid Films. 2005, 484: 358. COI number [1:CAS:528:DC%2BD2MXltVGrtLs%3D] 10.1016/j.tsf.2005.02.035
Bittencourt C, Landes R, Llobert E, Molas G, Correig X, Silva MAP, et al.: J. Electrochem. Soc.. 2002, 149: H81. COI number [1:CAS:528:DC%2BD38XitlWht74%3D] 10.1149/1.1448821
Ivanov P, Hubalek J, Malysz K, Prasek J, Vilanova X, Llobert E, et al.: Sens. Actuators B. 2004, 100: 293. 10.1016/j.snb.2003.12.065
Dai CL, Liu MC, Chen FS, Wu CC, Chang MW: Sens. Actuators B Chem.. 2006.
Rajeswari J, Kishore PS, Viswanathan B, Varadarajan TK: Nanoscale Res. Lett.. 2007, 2: 496. COI number [1:CAS:528:DC%2BD2sXhtl2rtrvM] 10.1007/s11671-007-9088-y
X.P. Wang, B.Q. Yang, H.X. Zhang, P.X. Feng, Nanoscale Res. Lett. 2, 405 (2007)
Bachmann HR, Noth H, Rinck R, Kompa KS: Chem. Phys. Lett.. 1974, 29: 627. COI number [1:CAS:528:DyaE2MXhtFyjtrY%3D] 10.1016/0009-2614(74)85107-9
Bowden CM, Stettler JD, Witriol NM: J. Phys. B Atom. Mol. Phys.. 1977, 10: 1789. COI number [1:CAS:528:DyaE1cXhsVahsA%3D%3D] 10.1088/0022-3700/10/9/028
B.W. Mwakikunga, A. Forbes, E. Sideras-Haddad, R.M. Erasmus, G. Katumba, B. Masina, Int. J. Laser Nanoparticles (2008)(in press)
Mwakikunga BW, Sideras-Haddad E, Forbes A, Arendse C: Phys. Status Solidi. 2008, 205: 150. COI number [1:CAS:528:DC%2BD1cXhvFeiu7w%3D] 10.1002/pssa.200776829
Seo JW, Hernadi K, Miko C, Forro L: Appl. Catal. Gen.. 2004, 260: 87. COI number [1:CAS:528:DC%2BD2cXhvFWktr8%3D] 10.1016/j.apcata.2003.10.003
Frank FC: Discuss Faraday Soc.. 1949, 5: 48. 10.1039/df9490500048
Wagner RS, Ellis WS: Appl. Phys. Lett.. 1964, 4: 89. COI number [1:CAS:528:DyaF2cXls1yhug%3D%3D] 10.1063/1.1753975
Givargizov EI: J. Cryst. Growth. 1975, 31: 20. COI number [1:CAS:528:DyaE28Xot1KmtQ%3D%3D] 10.1016/0022-0248(75)90105-0
Kikkawa J, Ohno Y, Takeda S: Appl. Phys. Lett.. 2005, 86: 123109–1. 10.1063/1.1888034
Kasuya K, Ooi T, Kojima Y, Nakao M: Appl. Phys. Express. 2008, 1: 034005. 10.1143/APEX.1.034005
Trenter TJ, et al.: Science. 1995, 270: 1791. 10.1126/science.270.5243.1791
Buhro W: Adv. Mater. Opt. Electron.. 1996, 6: 175. COI number [1:CAS:528:DyaK28Xlslyrurs%3D] 10.1002/(SICI)1099-0712(199607)6:4<175::AID-AMO236>3.0.CO;2-C
Holmes JD, et al.: Chem. Eur. J.. 2003, 9: 2144. COI number [1:CAS:528:DC%2BD3sXksFemtbc%3D] 10.1002/chem.200204521
Hanrath T, Korgel B: Adv. Mater.. 2003, 5: 15.
BW. Mwakikunga, E. Sideras-Haddad, C. Arendse, M.J. Witcomb, A. Forbes, J. Nanosci. Nanotechnol. (2008) (in press)
Elliot S: The Physics of Chemistry of Solids. Wiley, Chichester; 2000.
Hudson JB: Surface Science—An Introduction. Butterworth-Heinemann, Boston; 1992.
Tan TY, Li N, Gosele U: Appl. Phys. Lett.. 2003, 83: 1199. COI number [1:CAS:528:DC%2BD3sXmtFOks7Y%3D] 10.1063/1.1599984
Zhang Y, Zhu F, Zhang J, Xia L: Nanoscale Res. Lett.. 2008, 3: 201. COI number [1:CAS:528:DC%2BD1cXos1Sqsr4%3D] 10.1007/s11671-008-9136-2
Authors would like to thank Prof. Michael Witcomb, Mr. Mthokozisi Masuku, Mr. Henk van Wyk and Ms. Retha Rossouw. The South African Department of Science and Technology (DST) project for the African Laser Centre, the National Research Foundation (NRF), the DST/NRF Centre for Excellence in Strong Materials and the CSIR National Centre for Nano-Structured Materials are acknowledged.
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Mwakikunga, B., Forbes, A., Sideras-Haddad, E. et al. Optimization, Yield Studies and Morphology of WO3Nano-Wires Synthesized by Laser Pyrolysis in C2H2and O2Ambients—Validation of a New Growth Mechanism. Nanoscale Res Lett 3, 372 (2008). https://doi.org/10.1007/s11671-008-9169-6
- Laser pyrolysis
- Tungsten trioxide
- Growth mechanism