Optical and structural transformations in polyethylene terephthalate (PET) films subjected to Ag+-ion implantation and subsequent Au7+-ion irradiation

IF 2.8 3区 物理与天体物理 Q2 PHYSICS, CONDENSED MATTER Physica B-condensed Matter Pub Date : 2024-09-11 DOI:10.1016/j.physb.2024.416518
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Abstract

We report on the dual effects of ion implantation and swift heavy ion on the optical and structural characteristics of polyethylene terephthalate (PET) films using UV–Vis spectrophotometry, FTIR and X-ray diffraction measurements. Samples were first implanted with 150 keV Ag+-ions at different fluences of 1 ×1016, 5 ×1016, and 1 ×1017 ions/cm2, and thereafter irradiated with 30 MeV Au7+-ions at different fluences, while analysing elemental depth profile in situ on the Time of Flight Heavy Ions Elastic Recoil Detection (ToF-Hi-ERDA) instrument. The elemental depth profile measurements showed considerable atomic depletion of hydrogen from 36% down to below 6% and oxygen from 18% to about 5%. The proportion of carbon increased from 45% to over 87%. The optical bandgap decreased with increasing ion implantation fluence and reduced even further on irradiation with 30 MeV 197Au7+-ions. The most notable outcome of the implantation was the onset of the precipitation of gold nanoparticles (Au-NPs) in the PET matrix, marked by Localised Surface Plasmon Resonance effects, coincided with a relatively significant drop in the bandgap energy. This latter effect could only be best explained as the result of these Au-NPs in the PET. This suggests that optical bandgap tuning in polymer films, usually achievable through high fluence implantation at low energy (i.e., keV), could also be realized through low fluence irradiation with MeV energy ions. It is surmised that, for the noble metals, NP-induced bandgap modification in PET precludes the need for high fluence to achieve the same. This has the obvious advantage of bandgap alterations at much lower structural damage to the target polymer. As reported by FTIR results, one can observe structural changes with the formation of new chemical bonds on thin films. X-ray diffraction results exhibited one prominent peak corresponding to the (100) plane, which varies in intensity with increased implantation fluence, suggesting a change in the crystallinity of the PET. The decrease in (100) peak or crystallinity was well connected with the presence and decrease of 847, 970, and 1471 cm−1 peaks, which were assigned to the ethylene glycol molecular groups.

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聚对苯二甲酸乙二酯 (PET) 薄膜在经过 Ag+ 离子植入和随后的 Au7+ 离子辐照后发生的光学和结构变化
我们利用紫外可见分光光度法、傅立叶变换红外光谱法和 X 射线衍射测量法,报告了离子注入和快速重离子对聚对苯二甲酸乙二酯(PET)薄膜的光学和结构特性的双重影响。首先以 1 ×1016、5 ×1016 和 1 ×1017 离子/平方厘米的不同通量植入 150 keV Ag+ 离子,然后以不同通量辐照 30 MeV Au7+ 离子,同时在飞行时间重离子弹性反冲探测(ToF-Hi-ERDA)仪器上原位分析元素深度剖面。元素深度剖面测量结果表明,氢的原子消耗量相当大,从 36% 降至 6% 以下,氧从 18% 降至约 5%。碳的比例从 45% 增加到 87% 以上。光带隙随着离子注入通量的增加而减小,在 30 MeV 197Au7+ 离子的辐照下,光带隙进一步减小。离子注入最显著的结果是 PET 基质中开始析出金纳米粒子(Au-NPs),其特征是局部表面等离子共振效应,同时带隙能也相对显著下降。只有 PET 中的这些 Au-NPs 才能最好地解释后一种效应。这表明,聚合物薄膜的光学带隙调节通常可以通过低能量(即 keV)的高通量植入来实现,但也可以通过 MeV 能量离子的低通量辐照来实现。据推测,对于贵金属而言,NP 诱导的 PET 带隙改性无需高通量即可实现。这样做的明显好处是,带隙改变对目标聚合物的结构破坏更小。正如傅立叶变换红外光谱结果所报告的那样,我们可以观察到薄膜上形成新化学键后的结构变化。X 射线衍射结果显示了一个与 (100) 平面相对应的突出峰值,其强度随植入通量的增加而变化,这表明 PET 的结晶度发生了变化。(100)峰或结晶度的降低与 847、970 和 1471 cm-1 峰的出现和降低密切相关,这些峰被归属于乙二醇分子基团。
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来源期刊
Physica B-condensed Matter
Physica B-condensed Matter 物理-物理:凝聚态物理
CiteScore
4.90
自引率
7.10%
发文量
703
审稿时长
44 days
期刊介绍: Physica B: Condensed Matter comprises all condensed matter and material physics that involve theoretical, computational and experimental work. Papers should contain further developments and a proper discussion on the physics of experimental or theoretical results in one of the following areas: -Magnetism -Materials physics -Nanostructures and nanomaterials -Optics and optical materials -Quantum materials -Semiconductors -Strongly correlated systems -Superconductivity -Surfaces and interfaces
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