22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Analysis of energetic oxygen species effect on in vitro biological responses of RF plasma-treated polymer F. Rezaei1 and B. Shokri1,2 1 Laser & Plasma Research Institute, Shahid Beheshti University G.C., Evin, Tehran, 1983963113, Iran 2 Physics Department, Shahid Beheshti University G.C., Evin, Tehran, Iran Abstract: The low pressure RF (13.56 MHz) plasma generated from high purity oxygen gas was used to impart biological characteristics to Polymethylmethacrylate (PMMA). PMMA samples were modified in constant pressure and voltage. The plasma process was monitored using optical emission spectroscopy (OES) to study the oxygen species which were generated in the plasma. Water contact angle goniometry showed that the plasma process was followed by a decrease of contact angle. Samples were characterized for their cell viability and biocompatibility by MTT assay using MEF cells. Moreover, antibacterial activity of samples utilizing the method of plate counting against Escherichia Coli was evaluated. Based on the obtained results, cell viability and antibacterial performance of samples were statistically studied in terms of water contact angle and intensity of most predominant oxygen species. Keywords: oxygen species, OES, antibacterial activity, MEF cells, goniometry 1. Introduction Polymethylmethacrylate (PMMA), because of its desirable volume properties, is one of the most extensively used polymeric biomaterials in different biomedical applications. One of the disadvantages of polymeric biomaterials is the general lack of the desirable surface properties, such as biocompatibility and bioactivity, in the majority of cases [1, 2]. Surface properties of biomaterials, including wettability, morphology and chemistry are of great importance in determining their biological responses and long term performance. Therefore, the main goal in designing the biomaterials is to ensure that they exhibit appropriate surface properties as well as desired physical and mechanical characteristics [3]. Therefore, surface modification of polymers for biomedical applications is required. Plasma-based processing is one of the common methods for modifying surface characteristics without affecting bulky properties [4, 5]. It is thus possible to have desired volume properties of the biomaterial and at the same time also improve its surface properties to be able to function properly in the biological environment. Plasma can be used for regulation of cells and bacteria attachment processes as a source of biologically active agents, like reactive species, charged particles and ultraviolet light. It is quite important to understand how these agents affect the surface of biomaterials to optimize plasma parameters. It is also critical to identify plasma components which have different effects on cells and bacteria. In the present study, we investigated the effect of most predominant oxygen species intensities on the cellular and antibacterial responses of PMMA samples. It is stated P-II-11-8 that use of energetic oxygen species in plasma treatment of the polymer leads to enhancement of biocompatibility and antibacterial characteristic of PMMA films. 2. Experimental 2.1 Surface Modification Process In present study, PMMA films were used as samples. Samples were ultrasonically cleaned in deionized water and ethanol successively. Oxygen (99.99% purity) was used as carrier gas. PMMA samples were modified via low pressure RF frequency of 13.56 MHz plasma in a parallel plate capacitively coupled reactor, described elsewhere [5]. The pressure and RF power were kept constant at 40 mTorr and 60 W, respectively. Samples were treated for 2 min at various gas flow rates (10 - 120 sccm). To ensure the reproducibility of the results, each experiment was done at least three times. Therefore, the results obtained by taking the average of analysed data. 2.2 Optical Emission Spectroscopy (OES) OES was employed for monitoring the reactive oxygen plasma. OES measurements are very sensitive to change in the high-energy fraction of the electron distribution function (EDF), which is responsible for production of radicals and ions in reactive plasmas [6]. Coinciding with treatments the optical spectra were detected in the wavelength range from 200 to 1100 nm by an optical spectrometer (AvaSpec-3648). 2.3 Contact Angle Goniometry A simple technique to measure the reactive level of a surface is contact angle measurement. Contact angles were determined by goniometry with Sessile Drop 1 2.5 In Vitro Bacterial Adhesion Assay The antibacterial performance of plasma treated samples was assessed using a modified plate-counting method against Escherichia coli ATCC 25922 (Gram negative). This assay has been described in detail previously [5]. 2.6 Statistical Analysis The statistical analysis was performed using OriginPro 8 SR0 software (v8.0724, OriginLab Corporation, USA). One way analysis of variance (ANOVA) was used to compare mean values. 3. Results and Discussion The samples were exposed to oxygen plasma at different gas flow rates between 10 to 120 sccm. The optical spectra were measured continuously during the plasma treatment, as explained earlier. A typical optical spectrum of oxygen plasma is shown in Fig. 1. Table 1. Predominant transition lines observed in optical emission spectra. Oxygen species π π π2+ π2+ Gas flow: 60 sccm O (777 nm) Intensity (a.u.) 30000 20000 10000 O2+ (559 nm) O2+ (525 nm) O (844 nm) 5000 0 200 300 400 500 600 700 800 900 1000 1100 Wavelength (nm) Fig. 1. Typical optical spectrum of oxygen plasma. 2 559 525 - 9800 15600 O2+(559 nm) O(844 nm) 15500 9700 15400 9600 15300 9500 15200 9400 15100 9300 15000 9200 14900 9100 14800 9000 14700 15 30 45 60 75 90 105 120 Gas flow rate (sccm) Fig. 2. Variation of emission intensities of the oxygen species in function of gas flow rate. 25000 15000 Transition line 3π5 π β 3π 5 π 3π3 π β 3π 3 π According to Fig. 2, it is generally accepted that the intensity of both atomic oxygen (844 nm) and oxygen molecular ion (559 nm) decreases with increasing gas flow rate. This is more likely due to increasing of recombination of active species with increasing gas flow. Oxygen is an electronegative gas and so decreases the number of electrons by attachment under formation of negative πβ and π2β ions [8]. Therefore, by considering the mechanisms [1] and [2], less free electrons in plasma environment leads to less production of these oxygen species. 0 35000 Wavelength 777 844 Intensity at 844 nm (a.u.) 2.4 In Vitro MTT Cell Viability Assay Cell viability of samples was examined using MTT assay after 48 h the mouse embryonic fibroblast (MEF) cell seeding. The MTT method is based on the fact that living cells are capable of reducing less colored tetrazolium salts into intensely colored formazan derivatives. After 48 h, the culture medium was aspirated off and samples were rinsed twice with PBS to remove unattached cells. The remaining cells attached to samples were detached by trypsin-EDTA. Subsequently, MTT solution (0.5 mg/ml) was added to each well and cells were then incubated at 37 °C in a humidified 5% CO 2 atmosphere for 4 h, afterwards, the remaining solution was removed and DMSO was added to wells to dissolve the formazan crystals. Cell viability was evaluated by measuring absorbance (optical density) at 570 nm using a plate reader (ELISA Plate Reader). Obtained optical density (OD) for each well is proportional to the number of living cells [7]. The major spectral features are corresponding to oxygen atom lines at 777 and 844 nm and the π2+ ion lines at 559 and 525 nm. These transition lines are given in Table 1. Intensity variations of the 844 and 559 nm emission bands as a function of gas flow rate were studied and are presented in Fig. 2. Intensity at 559 nm (a.u.) technique. The measurements were performed using 3.0 ππ distilled water in triplicate. Results of contact angle goniometry are listed in Table 2. The decrease in contact angle with reducing gas flow rate indicates that the surface is becoming hydrophilic. This can be explained by the formation of more atomic π (844 nm) and π2+ ion (559 nm) as a result of plasma treatment and their dispersion on the surface [9], which is in complete compliance with Fig. 2. The effect of intensity of these two emission lines on cell viability of samples is evaluated. Viability of MEF cells that were exposed to samples was calculated using P-II-11-8 Table 2. Variation of droplet contact angle as a function of gas flow rate. Contact angle (°) 22.6±0.1° 17.0±0.8° 36.2±1.2° 41.5±0.5° 46.1±0.6° 50.7±0.6° With reference to Fig. 3, it is revealed that two stages of cell viability changes are identified. Firstly, the cell viability increases with a rapid rising of π2+ ion (559 nm) and atomic π (844 nm) intensities. In the second stage, the viability continues to increase with a more slightly increasing of the π2+ and π intensities. 9800 15600 9600 15400 9500 15300 9400 15200 9300 9200 15100 559 nm: R2=0.650 844 nm: R2=0.866 15000 9100 9000 50 52 54 56 58 60 62 64 66 68 70 Viability (%) Fig. 3. Viability variations of PMMA samples via emission intensity of O at 844 nm and O+ 2 at 559 nm. Statistical analysis showed that the relationship between cell viability (π) and intensity of these oxygen species (πΌ) can be expressed by exponential model. For the π2+ at 559 nm and the atomic π at 844 nm equations [4] and [5] were obtained, respectively. Presence of the reactive oxygen species may improve the reactive level of the surface [10]. When the highly reactive species reach the sample surface, they break weak bonds stabilized with radicals, promoting the formation of polar and oxygen-containing groups at the surface and opening up the chemical sites to future bonding [11]. Oxygen-containing functional groups like hydroxyl and carboxylic groups help to improve the surface biocompatibility and cellular response, and also hydroxyl groups contribute to cell colonization [12]. Moreover, carboxylic functions contribute to bond proteins to the surface, so the cells do not perceive the surface as a P-II-11-8 9800 15540 9700 15480 9600 15420 9500 15360 9400 15300 9300 15240 9200 559 nm: R2=0.574 844 nm: R2=0.924 15180 15120 9100 9000 60 63 66 69 72 75 78 81 84 Antibacterial activity (%) Intensity at 844 nm (a.u.) Intensity at 559 nm (a.u.) 9700 15500 15600 Intensity at 844 nm (a.u.) Gas flow rate (sccm) 10 20 30 60 90 120 foreign material, which is corresponding to the enhancement of biocompatibility [13]. Therefore, with increasing the intensity of the energetic oxygen species, biocompatibility and cellular attachment enhances. Variation of antibacterial behaviour of samples in term of the emission intensities of these energetic oxygen species is presented in Fig. 4. Antibacterial activity of the modified samples was calculated using equation [6], where π and πΆ are mean number of bacteria on the modified and control samples, respectively. Intensity at 559 nm (a.u.) equation [3], where πππ and πππ are the average optical density of sample group and control group, respectively. The results are plotted in Fig. 3. Fig. 4. Antibacterial activity of PMMA as a function of emission intensity of O at 844 nm and O+ 2 at 559 nm. As can be seen, with increasing both intensities, samples show more appropriate antibacterial behaviour. Statistical analysis indicated that antibacterial activity (π΅) of samples varies linearly in term of the intensity of the oxygen species (πΌ). Equations [7] and [8] were obtained for the π2+ at 559 nm and the atomic π at 844 nm, respectively. It is well accepted that cell walls of most bacterial strains are negatively charged [14]. As mentioned earlier, energetic oxygen species are responsible for surface activation and formation more oxygen-containing functional groups at the surface. Some of these groups are negatively charged like carboxylic group. With increasing concentration of these groups, the surface becomes more hydrophilic and negatively charged. Thereupon because of the strong repulsive forces, increasing the intensities of the oxygen species enhances the antibacterial efficiency. Also, in this work changes in cell viability and antibacterial activity of PMMA samples as a function of contact angle values is studied (Fig. 5.). As expected, according to the earlier discussion in this paper, it is clearly observed that higher polymer surface hydrophilicity (corresponding to lower contact angles) is positively affecting the biological responses of PMMA samples and enhances cell adhesion and antibacterial efficiency. 3 70 84 68 78 Viability (%) 64 75 62 72 60 69 58 66 56 63 54 Viability (%) Bactericidal activity (%) 52 Antibacterial activity (%) 81 66 60 50 57 15 20 25 30 35 40 45 50 55 o Contact angle ( ) Fig. 5. Changes in cell viability and antibacterial activity via contact angles. 4. Conclusion In this paper, the role of atomic oxygen (844 nm) and π2+ ion (559 nm) intensities in cellular viability and antibacterial activity of PMMA surface using reactive oxygen plasma was investigated. The plasma was characterized by optical emission spectroscopy. Obtained results demonstrated that presence of the energetic oxygen species leads to significant enhancement of MEF cells adhesion to the surface of PMMA samples and also better antibacterial performance of the surface after the plasma treatment. Oxygen-containing functional groups, which were introduced to the surface via low pressure RF plasma treatment, play important role in determining final biological efficiency and responses of the surface. Statistical study revealed that cell viability varies exponentially in terms of both atomic oxygen and oxygen molecular ion intensities, while antibacterial activity varies linearly. Moreover, water contact angle goniometry demonstrated that enhancing the surface hydrophilicity cause an increase in both cellular attachment and antibacterial activity. 4 Equations [1] π + π2 β π + πβ + π [2] π + π2 β 2π + π2+ ππ [3] πππππππππ (%) = 1 β οΏ½οΏ½1 β π οΏ½ × 100οΏ½ πππ [4] πΌ559 = 15459.5 οΏ½1 β ππποΏ½β0.8(π β 47.9)οΏ½οΏ½ [5] πΌ844 = 9681.3 β 2.4 exp(β0.3π) π [6] π΄π΄π΄π΄π΄π΄π΄π΄π΄π΄π΄π΄π΄ ππππππππ (%) = 1 β οΏ½ × 100οΏ½ πΆ [7] πΌ559 = 14415.4 + 13.2 π΅ [8] πΌ844 = 7488.2 + 27 π΅ 5. References [1] T. Bouet. J. Biomed. Mat. Res., 24, 11 (1990) [2] S. Itoh. J. Biomed. Mat. Res., 63, 5 (2002) [3] A.M. Gallardo-Moreno. Acta Biomaterialia, 5, 1 (2009) [4] P.K. Chu. J. Surf. Coating Technol., 201 (2007) [5] F. Rezaei. J. Phys. D: Appl. Phys., 47, 8 (2014) [6] J. Pavlik. J. Superficies y Vacio, 9 (1999) [7] J.K. Wilson. J. Cancer, 62, 2 (1990) [8] N. Krstulovic. J. Phys. D: Appl. Phys., 39, 17 (2006) [9] B. Lopes. J. Appl. Adhes. Sci., 2, 17 (2014) [10] T. Murakami. J. 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