22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium A ToF-SIMS study of the polyethylene chemical modification induced by an atmospheric Ar-D 2 O post-discharge V. Cristaudo1, S. Collette2, C. Poleunis1, F. Reniers2 and A. Delcorte1 1 Institut de la Matière Condensée et des Nanosciences (IMCN), Bio & Soft Matter (BSMA), Université catholique de Louvain (UCL), 1 Croix du Sud, BE-1348 Louvain-la-Neuve, Belgium 2 Chimie Analytique et Chimie des Interfaces (CHANI), Université Libre de Bruxelles (ULB), 2 Boulevard du Triomphe, BE-1050 Brussels, Belgium Abstract: In an original approach to trace water reactivity upon surface treatment by ambient “open air” plasma, the H-D exchange and the oxidation processes induced in polyethylene by an Ar-D 2 O post-discharge are investigated using time-of-flight secondary ion mass spectrometry (ToF-SIMS), both at the surface and along the sample depth. Keywords: atmospheric Ar-D 2 O post-discharges, ToF-SIMS, deuteration, oxidation 1. Introduction The use of atmospheric plasmas for surface modification of polymers has expanded tremendously since the last decade [1-3]. In addition to the many advantages offered by the more conventional low pressure plasma techniques, atmospheric plasmas allow us to avoid the constraints of the vacuum, thereby achieving surface treatments at lower costs. In order to upgrade these surface plasma treatments to industrial scale, the chemical and physical properties of the polymers modified in atmospheric discharges need to be better understood. However, this investigation is complicated by the interaction between the plasma and the environment. Indeed, oxygen, nitrogen and water are always present in the atmosphere, intervening inevitably in the plasmainduced processes. Often, the presence of water vapor in the plasma can be considered as problematic as water is known to destabilize it [4-6]. However, the water vapor can be deliberately mixed into the plasma to achieve a milder treatment or to generate radicals of interest [7]. It is known in the literature that the presence of water vapor in the plasma induces the grafting of -OH groups onto polymer surfaces, representing a promising functionalization route for industrial and medical applications [8]. However, tracing of the water reactivity in the polymer modification remains challenging. In order to investigate the reactions involving hydrogen, and thereby obtain a comprehensive view of the surface modification by water plasmas, one must be able not only to detect hydrogen, out of reach of the classical characterization techniques, such as X-ray photoelectron spectroscopy (XPS). However, it is also requested the separation of the diverse hydrogen contributions, deriving from the water vapors - plasma or atmospheric water and from the polymer itself. The present work reports an original approach to elucidate the reactions involving hydrogen, using a combination of deuterated water in the plasma and state-of-the-art SIMS analysis. For this purpose, D 2 O P-III-6-12 vapor was injected in the post-discharge of an atmospheric argon plasma torch for the treatment of LDPE (low density polyethylene) films. ToF-SIMS was chosen for the surface and in-depth analysis because it is the only surface technique possessing sufficient sensitivity and selectivity to the hydrogen isotopes as elements and in molecular fragments [9-11]. In addition, thanks to the recent advent of large Ar cluster ion beams (clusters constituted by hundreds to thousands of atoms) for sample sputtering, the modifications of the polymer molecular structure can be also followed along the sample depth [12-14]. Therefore in the following sections, a protocol for the quantification of the deuteration at the surface is first established by defining a deuteration ratio based on the SIMS intensities of the protonated repetitive units of LDPE differing in their H isotopes content. Based on this parameter, the torch-surface distance is optimized. In the second part of the work, the evolutions of the deuteration and the oxidation in a shallow region of the sample subsurface is followed using molecular depth profiling, demonstrating the usefulness of Ar cluster beams for this purpose. 2. Methods The LDPE film was treated by an atmospheric RF argon plasma torch (AtomfloTM 250D) from SurfX Technologies LLC. Deuterated water vapors were injected into the post-discharge region of the Ar plasma by means of a bubbler. In order to investigate the efficacy of the deuteration process as a function of the gap between the LDPE film and the plasma source, the experiments were performed during 5 minutes of treatment at three different distances of 5, 7 and 10 mm, respectively. Secondary ion mass spectra and molecular depthprofiling experiments were performed using an ION-TOF ToF-SIMS V (Münster, Germany) instrument equipped with both Bi-LMIG (liquid metal ion gun) and Ar-GCIB (gas cluster ion beam) primary ion sources mounted at 1 45° to the surface normal. The secondary ions were collected by a time of flight analyzer perpendicular to the sample surface. The mass spectra were obtained using a 30 keV Bi 5 + beam on a 200 x 200 µm2 sample area. Whereas, the depth-profiles were performed in dual ion beam mode. 10 keV Ar 5000 + ions were employed to sputter a 600 x 600 µm2 area, and 30 keV Bi 5 + ions for collecting the spectra from a 200 x 200 µm2 area concentric to the sputtered surface. zero. Only the C 2 DH 4 + intensity does not level off due to the interference of the 13CCH 5 + peak. Finally, the fluence reported in the x-axis of the profile was converted in depth. With the used experimental conditions, the total erosion depth was found to be ∼10 nm. The deuteration ratio, R D , applied to this depth-profile and reported in Figure 1.b, shows an evolution of the H-D exchange from an initial value of ∼30% to ∼4% over a depth of ∼10 nm. 3. Results and Discussion The first objective of the present work is to study the deuteration of the LDPE surface. To assess the extent of the deuteration, it is recommended to focus on molecular fragment ions. Therefore, the ions selected for this analysis were the protonated repetitive unit of the polyethylene, C 2 H 5 + at m/z = 29, and its progressive deuteration reaction products, C 2 DH 4 + (m/z = 30), C 2 D 2 H 3 + (m/z = 31), C 2 D 3 H 2 + (m/z = 32), C 2 D 4 H+ (m/z = 33) and C 2 D 5 + (m/z = 34). It is important to note that all these fragment ions, differing only by their H isotopic ratio, should possess the same ionization probability. This permits, to some extent, a quantitative analysis in SIMS. Once these methodological precautions and protocols are established, the influence of the sampletorch gap on the H-D exchange at the surface can be studied. Three different torch-surface distances were investigated - 5, 7 and 10 mm, respectively - keeping constant the treatment time (5 min). In order to obtain a synthetic view of the sample deuteration, it is useful to introduce an H-D exchange indicator or “deuteration ratio”, R D , which is defined as follows: 5 5 𝑥=1 𝑥=0 𝑅𝐷 = � 𝐶2 𝐻5−𝑥 𝐷𝑥+�� 𝐶2 𝐻5−𝑥 𝐷𝑥+ The results display that 5 mm gap gives a R D of 25 - 30% depending on the sample, which decreases strongly with the sample-torch distance, down to a value of ∼5% for a gap of 10 mm (not shown). The second objective of this work is to study the deuteration along the depth of the LDPE film functionalized in the optimized conditions of 5 min and 5 mm. The related depth-profile is shown in Fig. 1a, where the evolution of the ions C 2 D x H 5-x + (0 ≤ x ≤ 5) is now followed along the depth. There is a very strong decrease of the deuterated species intensities with the sample depth. The order of the curves follows the order of deuteration, C 2 D 5 + presenting the steepest decay. However, there is also a smaller decrease of the C 2 H 5 + intensity (30%), which might be the result of diverse causes such as, for instance, the presence of smaller chains on the surface, more branching of the molecules and/or oxidation. Furthermore, the C 2 H 5 + intensity stabilizes with increasing the sputtering fluence, whereas the decay of the species C 2 D x H 5-x + (2 ≤ x ≤ 5) goes to 2 Fig. 1. Depth-profile of the LDPE film treated for 5 min at 5 mm. a) Intensity of the C 2 D x H 5-x + fragments (0 ≤ x ≤ 5) as a function of the sputtering fluence. b) Evolution of the deuteration ratio (R D ) as a function of the Ar cluster fluence. The positive mass spectra of the plasma-deuterated LDPE also point out the presence of C x H y D z O n + fragment ions, containing oxygen and deuterium simultaneously. The plasma-treated LDPE depth-profile in Fig. 2 reports the molecular species C 2 H 5 O+, where only one O atom is linked to the repetitive unit of the polymer, and two other related fragment ions, which solely differ for their H isotopic ratio. The intensity evolution of these O-containing molecular ions reproduces that of the C 2 D x H 5-x + (2 ≤ x ≤ 5), going to zero for a 10 nm depth. In conclusion, the LDPE deuteration induced by an Ar-D 2 O post-discharge was successfully evidenced and quantified at the sample surface and along the depth using ToF-SIMS. Finally, the molecular depth-profiling by P-III-6-12 large Ar clusters shows that the H-D substitution is an extreme surface process involving only the top 10 nm, in the applied plasma treatment conditions. [10] J. Lub, F.C.B.M. van Vroonhoven, D. van Leyen and A. Benninghoven. J. Polymer Sci. B: Polymer Phys., 27, 2071 (1989) [11] R.H.G. Brinkhuis and W.J. van Ooij. Surf. Interface Anal., 11, 214 (1988) [12] J. Hubert, C. Poleunis, A. Delcorte, P. Laha, J. Bossert, S. Lambeets, A. Ozkan, P. Bertrand, H. Terryn and F. Reniers. Polymer, 54, 4085 (2013) [13] C.M. Mahoney. Mass Spectrom. Rev., 29, 247 (2009) [14] S. Ninomiya, K. Ichiki, H. Yamada, Y. Nakata, T. Seki, T. Aoki and J. Matsuo. Rapid Commun. Mass Spectrom., 23, 1601 (2009) Fig. 2. Depth-profile of the LDPE film treated for 5 min at 5 mm. Intensity of O-containing fragment ions as a function of the sputtering fluence. 4. Acknowledgements This work was carried out in the framework of the network on Physical Chemistry of Plasma-Surface Interactions - Interuniversity Attraction Poles, phase VII (PSI-IAP7), and supported by the Belgian Science Policy Office (BELSPO). Finally, the authors thank the Belgian ‘Fonds National de la Recherche Scientifique’ (FNRS) for financial support to purchase the ToF-SIMS instrument. A. Delcorte is a senior research associate of the FNRS. 5. References [1] D. Pappas, A. Bujanda, J. Orlicki and R. Jensen. Surf. Coatings Technol., 203, 830 (2008) [2] C. Liu, J. Wu, L. Ren, J. Tong, J. Li, N. Cui, B. Brown and B. Meenan. Mat. Chem. Phys., 85, 340 (2004) [3] B. Tompkins, J. Dennison and E. Fisher. J. Membrane Sci., 428, 576 (2013) [4] N. Srivastava and C. Wang. J. Appl. Phys., 110, 053304 (2011) [5] L. Magne, S. Pasquiers, K. Gadonna, P. Jeanney, N. Blin-Simiand, F. Jorand and C. Postel. J. Phys. D: Appl. Phys., 42, 165203 (2009) [6] I. Koo and W. Lee. Plasma Chem. 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