Nanocomposite silver/poly(ethylene oxide)-like plasma polymers prepared by plasma-assisted vacuum evaporation and magnetron sputtering Dmitry Arzhakov1, Ivan Gordeev1, Andrei Choukourov1, Anna Artemenko1, Ondřej Kylián1, Jaroslav Kousal1, Oleksandr Polonskyi1, Josef Pešička2, Danka Slavínská1 , Hynek Biederman1 1 Charles University in Prague, Faculty of Mathematics and Physics, Department of Macromolecular Physics, V Holešovičkách 2, 180 00 Prague, Czech Republic 2 Charles University in Prague, Faculty of Mathematics and Physics, Department of Physics of Materials, Ke Karlovu 5, 121 16 Prague, Czech Republic Abstract: Nanocomposite Ag/poly(ethylene oxide)-like plasma polymers were prepared by simultaneous vacuum thermal degradation of poly(ethylene oxide) (PEO) and RF magnetron sputtering of silver. At constant discharge power, nanocomposites with different silver content were fabricated by varying the evaporation rate of PEO. Chemical composition, structure, optical and bioadhesive properties of Ag/PEO-like nanocomposites were studied by XPS, FTIR, UV-Vis, QCM and TEM techniques. Obtained filling factors ranged from 0.8 % to 28.0 % whereas relative fraction of ether groups in polymeric phase varied between 79% and 54%. In general, the increase of silver content led to reduced retention of the PEO structure and as a consequence to the loss of nonfouling properties. Structural changes were also studied upon the contact of the nanocomposites with water. Nanoparticles of silver were found to diffuse within the polymeric matrix with following coalescence and formation of larger metallic structures. Keywords: Poly(ethylene oxide), plasma polymer, nanocomposite, magnetron sputtering 1. Introduction Nowadays, there is a growing interest in plasmadeposited thin films which show biocompatibility and are able to prevent microbial adhesion. Different approaches to inhibit bacteria growth have been proposed [1]. PEO is one of the most well-known biocompatible materials [2]. Several methods have been used to obtain the non-fouling films from PEO. Recently, glow discharge-based methods have been given a thorough consideration for fabrication of PEO-like plasma polymers [3-7]. On the other hand, silver is one of conventional antibacterial reagents. It is believed that Ag can prevent bacterial enzyme activity [8, 9] Several research groups have focused their attention on plasma deposition of nanocomposite Ag/PEOlike plasma polymers [10-14] with motivation to combine the non-fouling properties of PEO with the anti-bacterial properties of silver. For maintaining the non-fouling nature of plasma-deposited PEO-like films it is necessary to reach the highest retention of the C-O-C groups in plasma polymer. It is usually achieved when small discharge power of several watts is used. For magnetron sputtering, however, higher powers are favourable to ensure sufficient supply of silver. On the other hand, the higher power may deteriorate the retention of the C-O-C groups. This work presents a method of obtaining Ag/PEOlike plasma polymers by simultaneous magnetron sputtering of Ag and vacuum evaporation of conventional PEO. The possibility to fabricate the films with different filling factors of silver, yet with high retention of the PEO structure is discussed. measurements by using pre-defined values of deposition rates of pure silver and PEO plasma polymers. The deposition parameters are summarized in Table 1. 2. Experimental setup 3. Results and Discussion The experimental arrangement was described in detail in [15-16]. Granules of conventional PEO were loaded into a copper crucible, which was heated by electric current. The crucible was placed 4 cm above a magnetron equipped with a silver target (figure 1). A radio frequency (Dressler Ceasar 13.56MHz) generator was used to deliver power to the magnetron. A quartz crystal microbalance (QCM) was placed in plane with the substrates 10 cm above the crucible to control the deposition rate. The vacuum chamber was brought to a base pressure of 2х10-3 Pa by rotary and diffusion pumps. The experiments were performed with argon used as a working gas. The pressure of 1 Pa and 5 cm3 (STP) min-1 flow rate were used. The discharge power was kept constant at 15 W. To obtain the films with different content of Ag, the deposition rate of PEO was varied by varying the temperature of the crucible. Volume fraction of silver, also called filling factor f, was determined from the QCM Table 1. Deposition parameters and filling factor of silver in the nanocomposite Ag/PEO-like plasma polymer films. Process Power W QCM, frequency shift Hz/min Deposition rate nm/min Ag 15 5 0.3 Ag PEO + QCM, filling factor vol. % 100.0 15 17 2.4 28.0 15 25 5.1 13.0 15 60 20.0 2.0 15 100 38.0 0.8 COC 54 % CC/CH 31 % Fill factor = 13,0 % COC 61 % CC/CH 25 % Fill factor = 2,0 % COC 75 % CC/CH 15 % Fill factor = 0.8 % COC 79 % CC/CH 14 % CPS Figure 1. Experimental setup: Q – quartz crystal microbalance, C– crucible with PEO; M – magnetron; T– silver target. Fill factor = 28,0 % 290 288 286 284 282 Binding Energy (eV) Figure 2. The C1s XP spectra of Ag/PEO-like nanocomposites prepared with different evaporation rate of PEO. Figure 2 shows the C1s peaks of the XPS spectra of the Ag/PEO-like plasma polymers with four different filling factors of Ag. The C 1s peak was fit by four components, namely C0 (C-H, C-C: BE=285.0 eV), C1 (C-O-C: BE=286.5 eV), C2 (C=O: BE=287.8 eV), C3 (O-C=O: BE=289.2 eV). The values of filling factors are also given for clarity. Obviously, the amount of Ag and the concentration of the C-O-C groups are related inversely. The relative fraction of the C-O-C species decreases from 79 to 54 % with increasing silver content from 0.8 % to 28.0 %. The films with high silver content (low evaporation rate of PEO) show the loss of the PEO character because of the increased specific power of the discharge, i. e. the power per mass unit of the precursor. Such behavior is analogous to that observed earlier in [10-14] Transmittance (%) 100 rate of PEO. Increase of the silver content leads to loss of non-fouling properties of coatings as measured by QCM in terms of fibrinogen adsorption. 0.8% 80 2% 60 13% 40 Pure Ag 28% 20 0 200 300 400 500 600 700 800 wavelength (nm) Figure 3. The UV–Vis transmittance of the nanocomposite Ag/PEO-like plasma polymers with different filling factors. The UV-Vis transmission spectra given in Figure 3 show that the nanocomposite Ag/PEO-like plasma polymer films are optically active in the visible area. The strong absorption peaks can be seen which are induced by the surface plasmon resonance (SPR) effect. This effect is characteristic for metal/dielectric nanocomposites when collective resonant oscillations of electronic gas in metals (plasmons) are excited upon interaction with electromagnetic field. The increase of silver content leads to intensification of the absorption. The main motivation for fabrication of the Ag/PEOlike plasma polymer films is their possible use in biomedical applications. Therefore, their behaviour in contact with water is of a great importance and it was also studied on example of the film with 13% of Ag. Figure 4a shows the distribution of the silver nanoparticles in plasma polymer matrix in a dry state as observed by TEM. It can be seen that silver nanoparticles tend to coalesce into bigger agglomerates which indicates their ability to diffuse in the bulk of the plasma polymer. Significant degree of flexibility of the PEO molecular segments can therefore be expected. The particles are of spherical shape and their size distribution is rather broad ranging from 2 nm to 45 nm. Immersion into water for two days has tremendous effect on the structure of the film (figure 4b). Silver undergoes crystallographic transformations and form larger monocrystalline structures of triangular shape. Figure 5 shows the adsorption kinetics of fibrinogen on the nanocomposite Ag/PEO-like plasma polymer films, which were prepared at different evaporation Figure 4. TEM images of the Ag/PEO-like nanocomposite with 13% of Ag before wetting a) and after wetting b). In the case of high evaporation rate of PEO (0.8% of Ag), the frequency of QCM does not change with time. This proves that the surface possesses the nonfouling properties. It was shown previously that in the case of PEO-like plasma polymers about 70% retention of the C-O-C groups is required for the film to behave non-fouling [18]. Here, the film with 2% of Ag adsorbs the protein even though the concentration of the C-O-C groups in the plasma polymer is still at 75%. Apparently, silver reveals strong affinity to fibrinogen and introduction of as low as several percent of silver overrides the nonfouling properties of the plasma polymer. Strong adsorption of fibrinogen by the film with 28% of Ag is therefore given by both high content of silver and low content of the ether groups 79% COC 0.8 % Ag -20 -40 -60 75% COC 2 % Ag Protein Added Delta Frequency (Hz) 0 [4] D. Beyer, W. Knoll, H. Ringsdorf, J.H. Wang, R.B. Timmons, P. Sluka, J. Biomed. Mater. Res. 36 (1997), 181–189 54% COC 28 % Ag -80 -100 0 20 40 60 Time (min) Figure 5. Adsorption of fibrinogen on the Ag/PEO-like plasma polymer nanocomposites. 4. Conclusions Nanocomposite Ag/PEO-like plasma polymer films were prepared by simultaneous vacuum thermal degradation of polyethylene oxide and RF magnetron sputtering of silver. This method was shown to be good at obtaining nanocomposites with different filling factor of silver and with more than 75% retention of the C-O-C groups in polymeric phase. Nanoparticles of silver were found to be relatively mobile and able to form large monocrystal structures when in contact with water. Increasing silver content leads to loss of non-fouling properties of the nanocomposites. 5. Acknowledgements The work was supported by the grant SVV-2011263305 and by Academy of Science of the Czech Republic through the grant KAN 101120701. References [1] F. Furno, K.S. Morney, B. Wong, B.L. Sharp, P.L. Arnold, S.M. Howdle, R. Bayston, P.D. Brown, P.D. Winship, H. Reid, J. Antimicrob. Chemother, 54 (2004), 1019. [2] R.I. Mahato, Biomaterials for delivery and targeting of proteins and nucleic acids. Boca Raton London New York Washington, D.C. CRC Press.,(2005). [3] G.P. Lopez, B.D. Ratner, C.D. Tidwell, L.L. Haycox, R.J. Rapoza, T.A. Horbett, J. Biomed. Mater. Res. 26 (1992), 415–439 [5] E.E. Johnston, B.D. Ratner, J.D. Bryers, Polym. Mater. Sci. Eng. 77 (1997), 577 [6] E.E. Johnston, B.D. Ratner, Mater. Res. Soc. Abstracts, Fall Meeting, Boston, MA, 464, (1998). [7] A. Choukourov, O Polonskyi, J. Hanus, J. Kousal, A. Grinevich, D. Slavinska, H. Biederman, Plasma Process. Polym., 6 (2009), 21–24 [8] A. Oloffs, C. Grosse-Siestrup, S. Bisson , M. Rinck, T , R. Rudolph,U. Gross, Biomaterials, 15 (1994), 753 [9] J. M. Schierholz, L. J. Lucas, A. Rump, G. Pulverer, J. Hosp. Infection, 40 (1998), 257 [10] L. Yue, M. Zhou, Q. Chen, J. Weng, Y. Zhang, Vacuum 83 (2009), 1200-1203 [11] Q. Chen, M. Zhou, Y. Fu, J. Weng, Y. Zhang, L. Yue, F. Xie, C. Huo, Surf. Coat. Technol. 202, (2008), 5576-5578 [12] Q. Chen, L. Yue, F. Xie, M. Zhou, Y. Fu, Y. Zhang, J. Wend, J. Phys. Chem C ,112 (2008), 10004-10007 [13] P. Favia, M. Vulpio, R. Marino, R. d’Agostino, R. P. Mota, M. Catalano, Plasmas and Polymers, Vol 5 №1,2000 [14] E. Korner, P. Rupper, J.F. Lubben, A. Ritter, J. Ruhe, D. Hegemann, Surf. Coat. Technol. 205 (2011), 2978-2984 [15] A. Choukourov, I. Gordeev, D. Arzhakov, A. Artemenko, O. Kylián, J. Kousal, O. Polonskyi, J. Pešička, D. Slavínská and H. Biederma, Surf. Coat. Technol., 205 (2011), 2830-2837 [16] A. Choukourov, I. Gordeev, O. Polonskyi, A. Artemenko, L. Hanykova´, I. Krakovsky´, O. Kylia´n, D. Slavı´nska´, H. Biederman, Plasma Process. Polym., 7 (2010), 445–458 [17] E. Sardella, R. Gristina, G. S. Senesi, R. D’Agostino, P. Favia, Plasma Process. Polym. 1 (2004) 63.
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