Synthesis of ZnO nanoparticle coatings on carbon nanotube cathodes for electrical discharge applications Martin Lennox, Sylvain Coulombe Department of Chemical Engineering, McGill University, Montréal, QC, Canada Abstract: The enhanced field emission of carbon nanotube and carbon-nanotubenanoparticle composite materials have the potential to significantly improve the voltage requirements and reduce cathode heating in plasma generation. An integrated dusty plasma process for the deposition of zinc nanoparticle films on carbon nanotube-coated metal electrodes is described and their performance as cathodes in DC glow discharges is evaluated. Keywords: zinc oxide, carbon nanotube, nanoparticle, dusty plasma, thin film 1. Introduction The lifetime of DC electrical discharge-based device is largely dependent upon the electron emission characteristics of the cathode material. Thermionic and thermo-field emission processes are effective modes of electron emission, but necessitate high temperatures and consequently significant thermal loads at the attachment point, which ultimately lead to erosion by vaporization and liquid volume ejection1. Nanostructured materials show great promise as cathode materials, since reports of their enhanced electron emission2 could mitigate the need for high temperature-sustained electron emission modes. The nanostructure plays the dual role of local electric field enhancer and host for work functionlowering materials. Carbon nanotubes in particular, are already in use as field electron emitters. Our recent work demonstrated that under the right conditions, carbon nanotubes can also be used to sustain low-power density DC electrical discharges3. It appeared that thermo-field emission at lowtemperature is possible due to the drastic lowering of the CNT work function due to the presence of contaminants in the plasma environment. On the other hand, pristine CNTs, being single walled or multi-walled, appear to not be capable of sustaining electrical discharge conditions. Uncoated and/or unfunctionalized CNTs have been documented as susceptible to erosion4 and suffer etching when exposed to oxidizing plasmas. There is thus an interest to protect the CNT surface for high temperature and/or reaction while maintaining their nanostructure. The present work reports our preliminary attempt to deposit ZnO nanocrystal coatings onto CNTs in an attempt to maintain or enhance their enhanced emission properties while protecting the CNTs. Research into the use of CNTs decorated with zinc oxide nanoparticles as potential electron emission sources has reported enhanced electron fieldemission current5 as well as an increase in the nanotube field emission lifetime6, although it appears that a different morphology of the ZnO coating can decrease the electron emission properties of such composite materials. Documented synthesis methods frequently rely on wet chemistry, organometallic precursors, or exposure of CNTs to high temperatures for zinc vapour deposition or annealing. Most often, these methods result in “decorated” CNTs, a term used in the literature to describe the sporadic deposition of nanoparticles on CNT substrates. In order to improve the deposition of ZnO coatings on CNTs for their eventual testing as cathode materials, a dusty plasma process was developed that makes use of an aerosol flow condensation (AFC) process for zinc nanoparticle synthesis. AFC is a process for the synthesis of micro- and ultra-fine metal powders previously described in the literature7. Collection of these particles has been noted as problematic, and has relied on the use of thermophoretic sampling methods. Previous success in our research group with regards to the collection of metal nanoparticles onto substrates covered in CNTs8 has led to the use of the surface charging experienced by the nanoparticles in a dusty plasma to enhance their deposition as coatings on CNTcoated metal cathodes. Given the potential for enhanced electron emission of CNTs and ZnO-CNT composites, it is of interest to investigate their utility in reducing the operating temperature requirements of cathode materials through improved electron emission, as well as their durability in such processes. 2. Zinc nanoparticle synthesis Zinc nanoparticles are synthesized by AFC from a heated crucible at 450-500 °C that contains pure zinc pellets. Argon gas is passed over the crucible through a 1 mm x 20 mm rectangular orifice in a water-cooled nozzle. Simultaneously, a sheath gas of argon is flowed over the interior diameter of the reactor from sixteen 1.6 mm diameter holes, spaced equally around the circumference of the nozzle. This stream of zinc nanoparticles flows through two consecutive glass electrical breaks, of which the isolated portion is used as the live electrode for the generation of a continuous RF (13.56 MHz) glow discharge. !" #$%&'()&* +%,-. K% 0,138()@* A&1B$%C /()&,%* 0$1($) 9:;<=* 0>? +$* 2,3445* 678,4.1 D$$'()@* H,1&%* I&.&%J$(% D%43(E'&* >&,1&%*!$B&%* F4--'G Figure 1. Schematic of nanoparticle deposition apparatus. The total argon flow rate through the system is typically 1-2 SLPM, with a maximum possible total flow rate of 7.5 SLPM. The pressure inside the reactor during deposition is 2 Torr and the input power to the plasma is 20 W. 3. Results Using a total system flow rate of 2 SLPM Ar, exposure of the CNT-SS304 samples to the dusty plasma stream for 1 min resulted in the deposition of approximately 5 nm diameter particles, in addition to larger particles in the range of 20 – 50 nm, as shown in Figure 2. At the maximum argon flow rate, nanoparticles in the 5 nm range were deposited, as shown in Figure 3. The composite materials for testing are formed by exposing 9/16” diameter stainless steel 304 (SS304) mesh rounds that are coated with multi-walled carbon nanotubes (MWCNTs) by a previously described process9 to the stream issuing from the dusty plasma. The deposition is performed for the desired length of time by making use of a linear motion feed-through, upon which the deposition substrates are mounted. Oxidation of the zinc nanoparticles is accomplished by trace amounts of oxygen in the argon flow, as well as subsequent exposure of the composite materials to atmospheric conditions. A schematic diagram of the experimental apparatus is shown in Figure 1. Figure 2. TEM image of the CNT coating synthesized at 2 SLPM Ar (total flow rate) and 1 min deposition time. To generate nanocomposite structures to be evaluated as the cathodes of DC electrical discharges, a series of CNT-SS304 substrates were exposed to the outlet of the dusty plasma for 5 min to ensure complete coverage of the nanostructured surface. In this instance, the nanoparticle coating resulted in a drastic increase of the effective diameter of the nanostructured surface; untreated, the diameter of the MWCNTs growing from the surface of the SS304 mesh were between 30 – 50 nm, whereas the diameter of the coated MWCNTs was approximately 500 nm, as can be seen in Figure 4. '%#$ '"#$ '!#$ !"#$%&'()!*( Figure 3. STEM image of the CNT coating synthesized at 7.5 SLPM Ar (total flow rate) and 1 min deposition time. The performance of the synthesized composite materials was tested in a linear DC glow discharge operating at 3.5 Torr and 4 mA current. The nanocomposite cathodes were mounted in a custom boron nitride ceramic enclosure that ensured only the material for testing was exposed to the plasma. To mitigate the effects of cathode heating, argon was flowed through the system at a rate of 2 SLPM. The voltage across the generated glow discharge was monitored as a function of time, for cathodes composed of the base SS304 mesh and the ZnOCNT nanocomposite. The results of this are shown in Figure 5, with error bars showing the 95% confidence interval. '(#$ !&#$ !%#$ !"#$ #$ (#$ )#$ !#$ '#$ "#$ *#$ %#$ +#$ +,-'()-,.*( ,,!#'$ -./012$034536789$ Figure 5. Performance of tested cathode materials. There appears to be no significant difference between the tested SS304 base substrate and the ZnO-CNT composite material. In fact, the general trend of Figure 5 indicates that the composites formed by 5 min of deposition perform more poorly than the untreated SS304. This may be explained by the thickness of the ZnO coating, which may have acted as a barrier to electron emission. Moreover, composite material may no longer contain sufficient nanostructured surfaces to meaningfully enhance the electron emission, as reported in the literature. Figure 4. CNTs coated by the dusty plasma, 2 SLPM Ar (total flow rate), 5 min deposition time. The large variance observed in the voltage measurements of Figure 5 has been attributed to instability in the flow of argon across the cathode surface and thus fluctuations in the cooling rate of the cathode. The supplied voltage varied accordingly to maintain the set current of the discharge, which resulted in the observed variations voltage across the discharge. Consequently, tests are in progress to evaluate the performance of the nanostructured composites produced for shorter deposition times under more stable cooling conditions for the cathode. The results of the ongoing investigations will be reported at the conference. References [1] S. Coulombe and J.-L. Meunier, J. Phys. D: Appl. Phys. 30, 776 (1997). [2] V. Semet, Vu Thien Binh, P. Vincent, et al., Appl. Phys. Lett. 81, 343 (2002). [2] L. Rao, R. J. Munz and J.-L. Meunier, J. Phys. D: Appl. Phys. 40, 4192 (2007). [3] M. Dionne, S. Coulombe and J.-L. Meunier, The Science and Technology of Light Sources 12th International Symposium. Eindhoven, The Netherlands, July 11-16 (2010). [4] Y. Qin and M. Hu. Applied Surface Science. 254, 1757 (2008) [5] J. M. Green, L. Dong, T. Gutu, et al., J. Appl. Phys. 99, 094308 (2006). [6] Y.-S. Min, E. J. Bae, J. B. Park, et al., Appl. Phys. Lett. 90, 263104 (2007). [7] V. Haas, R. Birringer, H. Gleiter and S. E. Pratsinis. J. Aerosol. 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