Elsevier

Applied Surface Science

Volume 263, 15 December 2012, Pages 334-338
Applied Surface Science

Optical characterization of poly(methyl methacrylate) implanted with low energy ions

https://doi.org/10.1016/j.apsusc.2012.09.056Get rights and content

Abstract

The samples of poly(methyl methacrylate) (PMMA) were subjected to 100 keV N+ and Ar+ ion implantation up to a maximum fluence of 2 × 1016 ions/cm2. The effect of ion implantation on the optical energy gap and the refractive index has been studied through UV–visible spectroscopy. The results clearly indicate a decrease in the values of optical energy gap and an increase in the values of refractive index as an effect of ion implantation corresponding to both of the ions. It has also been observed that the changes induced by the implanted ions are more pronounced for N+ ions in comparison to Ar+ ions. This variation has been correlated with the calculated ranges of these ions in PMMA polymer using Stopping and Range of Ions in Matter (SRIM) code. Finally, an attempt has been made to correlate all the observed changes with the induced structural changes as revealed through Raman spectroscopy.

Highlights

► The study provides the optical behavior of ion-implanted poly(methyl methacrylate). ► Optical energy gap reduces from 3.13 to 0.8 and 2.8 eV for N and Ar implanted PMMA. ► Refractive index increases from 1.54 to 2.71 and 2.02 for N and Ar implanted PMMA. ► The changes after N and Ar implantation are justified by Raman spectroscopy. ► The implanted PMMA may find extensive applications in opto-electronic devices.

Introduction

In modern era, polymers have emerged as most promising materials for various scientific and technological applications. This has become possible because of their excellent inherent properties which can further be modified by various treatments including chemical doping, heat treatment, ion implantation, etc. [1], [2], [3]. It is well known that energetic ions, when bombarded on a polymeric surface, can drastically alter its various chemical and physical properties. These changes, in general, are incorporated by various elastic and inelastic collisions between the energetic incident ions and the target polymer. However, the extent of these changes produced depends on the structure of the polymer and the experimental parameters of the ion irradiation like ion energy, fluence, mass, charge, etc. [4], [5], [6], [7]. The improved properties of the polymers through proper tailoring make them promising materials in today's world.

Among the broad variety of available polymers, PMMA (monomer composition: C5H8O2) is one of the outstanding material most widely studied in the last decade [8], [9], [10]. Due to its excellent and promising chemico-physical properties, it finds wide applications in many technological and productive fields. It exhibits good mechanical strength, chemical inertness, thermal stability, weather resistance, moldability, etc. Apart from all these, it finds an extensive application in various optical and opto-electronic devices due to its excellent optical properties from near-UV to near-IR regions [11], [12]. Ion implantation studies in PMMA attract special attention because of its usability in the fabrication of optical waveguides, lithography, biomedical applications, etc. [12], [13], [14], [15], [16], [17]. Some studies on the effect of N+ and Ar+ ion implantation in PMMA are available in the literature, but from different point of view. Leontyev et al. [13] and Kulish et al. [14] have concentrated mainly on the refractive index behavior of PMMA under N+ ion implantation. He et al. [15] studied the biomedical applications of Ar+ ion-implanted PMMA. Koval [16] has studied the etching mechanism of Ar+ ion-implanted PMMA. Tsvetkova et al. [17] have quoted the enhanced photoluminescence after implantation to Si+ ions in PMMA at different energies.

In the present work, we have carried out a systematic study on the effect of 100 keV N+ and Ar+ ion implantation on the optical energy gap and refractive index of PMMA polymer and simultaneously correlated to the induced structural changes as revealed through Raman spectroscopy. Such studies will not only lead to the better understanding of the fundamental processes involved during the ion–polymer interaction responsible for the tuning of various properties of the polymers but will also enhance the industrial applications of polymers as materials with the reduced cost.

Section snippets

Materials and methods

The samples (1 cm × 1 cm) of PMMA (Goodfellow, UK) were cut from a flat sheet of thickness 500 μm and subjected to implantation of 100 keV N+ and Ar+ ions using Low Energy Ion Beam Facility (LEIBF) available at Inter University Accelerator Centre (IUAC), New Delhi, India. The irradiation of these samples was performed at room temperature at normal incidence to the surface under high vacuum (∼10−6 Torr) up to a maximum dose of 2 × 1016 ions/cm2. The beam current density was kept ∼0.6 μA/cm2 in order to

UV–visible studies

The optical behavior of the virgin- and ion-implanted samples has been analyzed by recording the UV–visible transmission (T) and reflection (R) spectra in the wavelength range 190–900 nm. Since the measured values of T involve the reflection from top and bottom air–sample interfaces, therefore, these values need to be corrected before incorporating them in the relevant equations. Taking into account these corrections, the transmission coefficient (t) for light for a single pass through the

Conclusion

From the observed behavior of PMMA under ion implantation, it may be concluded that it shows a drastic change in its optical parameters. The values of optical energy gap decreases while those for refractive index increases with the increasing fluence of implanted ion. It may also be inferred that the changes induced also depends upon the implanted ion and the depth of the ion to which it impinges in the host polymer matrix. All the observed changes have been correlated to the induced structural

Acknowledgements

The authors are thankful to Dr. D. Kanjilal, IUAC, New Delhi, for valuable discussions. Thanks are due to Dr. P. Kumar, IUAC for helping during irradiation. Raman spectroscopic measurements were performed at UGC-DAE Consortium for Scientific Research, Indore, India. Authors are grateful to Prof. Vasant Sathe and Mr. Manoj Kumar for their kind cooperation during the Raman experiments. One of the authors (PKG) is thankful to CSIR, New Delhi for financial assistance in form of SRF.

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