Plasma etching of DLC films for microfluidic channels
Introduction
The development of nano- and micro-technologies has made important impacts in many areas, such as in the electronic, medical, automotive, avionic and aerospace industries promoting significant improvements of the microelectronic systems and on the products for civil use. Certainly these processes are related to the new materials and techniques that have been intensively studied in this period.
Diamond-like carbon (DLC) films are classified among these materials, because of their attractive mechanical, optical, electrical and chemical properties. They are widely used as protection films of magnetic recording disk due to its hardness, chemical inertness and low friction coefficient [1], [2]. One more advantage associated with DLC is that its properties can be easily tailored by the ratio of the tetrahedral bonding population to the trigonal bonding population (sp3/sp2 ratio).
When these films are conveniently lithographed and plasma etched, it could be possible to produce microfluid channels to be used in the so-called lab-on-a-chip technology. Silicon and glasses are the usual materials for these channels. To evaluate the applicability of DLC for this technology it is necessary to study the effects of plasma etching on the morphology of this film. In this article etching rate and surface roughness are the main parameters that we measured considering various operational conditions for RIE of DLC.
Section snippets
Experimental
DLC films were deposited by a 150 W dc magnetron sputtering of a graphite target with the discharge produced in a gas mixture of 10% CH4 and 90% argon. The films exhibit high hardness of the order of 10 GPa, and friction coefficient as slow as 0.15. Fig. 1 shows a typical DLC Raman spectrum containing a mixed structure of microcrystalline diamond and graphite as well as a disordered structure.
The spectrum has a well-pronounced single peak centered on 1565 cm−1 with shoulder at around 1400 cm−1.
Results and discussions
Fig. 2 shows the behavior of the etching rate and the rms roughness as a function of the rf power. These etches were performed at a pressure of 6.6 Pa and using pure oxygen, at a flow rate kept at 5 sccm. In this figure, an increase in the etching rate up to 220 nm/min was observed when the rf power is increased. Roughness increases gradually from 0.3 up to 0.8 nm with the power. The roughness of the films etched at power higher than 80 W could not be determined by AFM because their values were
Conclusions
RIE etching of DLC films has been carried out and the qualities of the processed surfaces were investigated by AFM. The etching rate and surface roughness were measured as function of the rf power supplied to the discharge and with respect to the oxygen content in the oxygen/argon gas mixture. The main conclusions of this work are:
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Increasing the rf power an increase in the etching rate and in the rms roughness was observed. Working at power higher than 80 W high values of etching rate, about 200
Acknowledgements
The authors would like to acknowledge the ‘Laboratrio de Filmes Finos do IFUSP’, Brazil, for the SPM facility and to technician Alexandre Marques Camponutti for the technical support in SEM analyses. The financial support of FAPESP, CAPES, CNPq and FINEP is also acknowledged.
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