22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Stable amine-rich layers prepared by cyclopropylamine plasma polymerization A. Manakhov1, E. Makhneva1,2, J. Polčak3, D. Nečas1,2 and L. Zajíčková1,2 1 Plasma Technologies, CEITEC Central European Institute of Technology, Masaryk University, Brno, Czech Republic 2 Department of Physical Electronics, Faculty of Science, Masaryk University, Brno, Czech Republic 3 CEITEC - Central European Institute of Technology, Brno University of Technology, Brno, Czech Republic Abstract: The preparation stable and amine-rich plasma polymers is still challenging due to high thickness loss of amine-rich coatings in water, preventing their bio-applications. In this work, the amine films exhibiting 9 at.% of NH x environment and thickness loss of only 2% were prepared by low pressure cyclopropylamine plasma polymerization. The influence of plasma power and duty cycle on layer chemistry and stability is reported. Keywords: amines, plasma polymerization, cyclopropylamine, XPS, AFM 1. Introduction Amine surface functionalization is a hot topic for material processing, because such functional groups are enhancing cell adhesion and proliferation and also can also be used for the immobilisation of biomolecules [1]. Although plasma polymerization of amine containing precursors has been studied for more than 50 years the preparation of stable amine films with high concentration of primary amines is still challenging [2]. In general, the stability of amine plasma polymers can be enhanced at the expense of the density of amine groups [3]. Moreover, the majority of the monomers employed for the amine plasma polymerization (ammonia, allylamine) are highly toxic compounds. Therefore, new monomers for the deposition of amine plasma polymers are required. Recently we have shown that amine plasma polymerization of non-toxic cyclopropylamine (CPA) led to deposition of amine films containing around 9 at.% of NH x environment and exhibiting thickness loss of 20% after 48 hours in water. In this work, the amine-rich plasma polymer (NH x > 7 at.%) were deposited on Si wafers by CPA RF CCP polymerization in a vertically oriented stainless steel plasma reactor. In this configuration, the bottom electrode bearing the substrates was direct-current (DC) negatively self-biased due to an asymmetric coupling but ion bombardment was significantly reduced by a relatively high process pressure of 50 Pa. The deposited coatings exhibited thickness loss below 2%, which is sufficiently low to employ these amine plasma polymers for biomedical applications. 2. Experimental The CPA plasma polymers were prepared in a stainless steel parallel plate reactor [4]. The bottom electrode, 420 mm in diameter, was capacitively coupled to a radio frequency (RF) generator working at the frequency of 13.56 MHz. The gases were fed into the chamber through a grounded upper showerhead electrode, 380 mm in diameter. The distance between the electrodes was 55 mm. The bottom electrode with substrates was negatively DC self-biased due to an asymmetric coupling. P-III-6-34 The reactor was pumped down to 10-4 Pa by a turbomolecular pump with a backing rotary pump. The deposition was carried out with the rotary pump only. The leak rate including wall desorption was below 0.1 sccm for all the experiments. The CPA was polymerized in squared pulsed CPA/Ar plasma at a power of 30 - 250 W and pressure of 50 Pa in pulsed or continuous mode. The pulse duty cycle and repetition frequency were 33% and 500 Hz, respectively. The flow rate of Ar was set to 28 sccm and regulated by an electronic flow controller Hastings, whereas the flow rate of CPA vapors was set to 2 sccm by a needle valve. The deposition time was adjusted to obtain film thickness around 200 nm. The substrates were sputter-cleaned by pulsed Ar plasma for 10 minutes prior to the deposition. The chemistry of the deposited films was characterized by Fourier Transform Infrared and X-ray Photoelectron Spectroscopy, whereas layer morphology was analyzed by Scanning Electron Microscopy and Atomic Force Microscopy. 3. Results The deposited amine films exhibited adhesion to substrate and were homogenous and smooth, as shown in Fig. 1a. However, some single nanoparticles with the diameter in the range from 100 to 300 nm were observed both by SEM and AFM imaging. The density of nanoparticles was dependent on plasma power and duty cycle. Both extremely low and high power led to suppression of nanoparticles densities and size. Regarding the CPA plasma layer chemistry, FT-IR revealed the bands of hydrocarbon (CH 3 at, CH 2 and CH) and amine groups (N-H stretching at and NH 2 scissoring at). The intensities of amine bands were decreasing with the P av , while the hydrocarbon peaks were gaining the intensity with the average power P av (plasma power multiplied by duty cycle). XPS analyses revealed that all layers were composed of carbon, oxygen and nitrogen (hydrogen cannot be detected by XPS). The C.O:N ration was dependent on P av and the main trend was that carbon and oxygen concentrations were increasing with P av at 1 large expenses of nitrogen. The highest nitrogen concentration equal to 18 at.% was determined for the layer deposited at 9.9 W (lowest power). fitting, the NH x environment is decreasing with P av from 13.0 down to 5.5 at.% , while CH x environment increases from 50 to 60 at.%. Intensity (counts) 6000 NHx 4000 2000 402 N-C=O C=N- 400 398 396 BE (eV) Fig. 3. N1s XPS curve fitting of CPA plasma polymer deposited at P av of 9.9 W. Fig. 1. The topography of CPA plasma polymer deposited at P av of 33 W: before (a) and after (b) immersion in the water for 216 hours. The XPS N1s and C1s curve fitting was employed to characterize the functional composition of the CPA plasma polymers. As shown in Fig. 2, the C1s signal was fitted with a sum of three components, namely corresponding to hydrocarbons (CH x ~ 285.0 eV), carbon bonded to nitrogen or oxygen (C-N/C-O ~ 286.3 ± 0.1 eV) and carbon double bonded to oxygen (N-C=O/-C=O ~ 288 eV). Intensity (counts) 10000 8000 CHx 6000 4000 N-C=O/C=O C-NHx C-O 2000 0 290 288 286 284 282 BE (eV) Fig.2. C1s XPS curve fitting of CPA plasma polymer deposited at P av of 9.9 W. The XPS N1s signal was also fitted with a sum three components corresponding to corresponding to the amine group (NH x=1,2 ~ 399.1 eV), amide group (N-C=O ~ 400.3 eV) and nitride / imine (-N=C ~ 398.3 eV) as depicted in Fig. 3. According to the N1s and C1s curve 2 Regarding the film stability in water, the thickness loss of the layers deposited at the P av of 9.9W was ~15% (immersion time 216 h) but it decreased to 2% when the P av was increased to 33 W. It should be noted that such layer also exhibited high retention of NH x environment (7 at.%) and no change of the layer morphology (Fig. 1b). The increase of P av above 100W led to increase of the thickness up to 10% and cracking of the layer after immersion in water for 216 h. Hence, the layers deposited at high power were swelled after immersion in water. Therefore, the deposition of the stable amine films from CPA does not require high power in order to achieve sufficient film stability. 4. Conclusions The stability, morphology and chemical composition of CPA plasma polymers was studied as a function of average power. The NH x was decreasing with P av from 13 to 5.5 at.%. The stability of the CPA plasma polymers was also dependent on the discharge parameters. Low power resulted in the thickness loss of 15%, while high power led to the layer swallowing. The optimum condition were as follow: plasma power of 100 W and duty cycle equal to 33%. In this condition the deposited layer exhibited 9 at.% of NHx environment, whereas the thickness loss was only 2%. Such low values of the thickness loss was rarely observed for functional plasma polymers. Hence, CPA plasma polymerization is a method of choice for the deposition of stable amine-rich films. 5. Acknoledgements This work was supported by the BioFibPlas project No. 3SGA5652 financed from the SoMoPro II Programme that has acquired a financial support from the People Programme (Marie Curie Action) of the Seventh P-III-6-34 Framework Programme of EU according to the REA Grant Agreement No. 291782 and was further co-financed by the South-Moravian Region. The research was also supported by the projects “CEITEC — Central European Institute of Technology” (CZ.1.05/1.1.00/02.0068) and “R&D center for low-cost plasma and nanotechnology surface modifications” (CZ.1.05/2.1.00/03.0086) from the European Regional Development Fund and by the Seventh Framework Programme of EU under the “Capacities” Specific Programme (Contract No. 286154—SYLICA). This publication reflects only the author's views and the Union is not liable for any use that may be made of the information contained therein. 6. References [1] K.S. Siow, L. Britcher, S. Kumar and H.J. Griesser. Plasma Process. Polym., 3, 392-418 (2006) [2] A. Manakhov, L. Zajíčková, M. Eliáš, J. Čechal, J. Polčák, J. Hnilica, et al. Plasma Process. Polym., 11, 532-544 (2014) [3] A. Abbas, C. Vivien, B. Bocquet, D. Guillochon and P. Supiot. Plasma Process. Polym., 6, 593-604 (2009) [4] A. Manakhov, D. Nečas, J. Čechal, D. Pavliňák, M. Eliáš and L. Zajíčková. Thin Solid Films. in press doi:10.1016/j.tsf.2014.09.015 (2014) P-III-6-34 3
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