Department of Physics, The M. S. University of Baroda, Gujarat, 390002, India.
Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai, 400 085, India.
J Fluoresc. 2019 Jul;29(4):1007-1012. doi: 10.1007/s10895-019-02414-z. Epub 2019 Jul 10.
Polystyrene polymer (PS)/AlO nanocomposite films were synthesized from PS:AlO (1-x):x mixtures (x = 3 wt%) via solution casting method. These nanocomposite films were exposed to 5 MeV proton beam of different fluences. The proton beam induced changes in optical and luminescence properties of PS and PS:AlO films have been investigated using FTIR, UV-visible, Photoluminescence and thermoluminescence studies. FTIR studies concede reduction in the peak intensity due to doping of AlO and proton irradiation. The UV-visible spectra show shifting of absorption edge with increasing fluence. This can be attributed to creation of conjugated system of bonds. The band gap of PS and 3 wt% AlO doped PS is observed to be 4.38 eV and 4.34 eV, respectively, whereas the band gaps of proton irradiated 3 wt% AlO doped PS films are found to be 4.28 eV and 4.23 eV at the fluences of 1 × 10 ions/cm and 1 × 10 ions/cm respectively. The photoluminescence emission spectra show three peaks, wavelength at 411 nm, 435 nm and 462 nm corresponding to the PS in violet-blue region when excited with near UV wavelength of 380 nm. The intensity of emission peaks was found to increase with increasing fluence. The thermoluminescence curves of PS/AlO were analysed using glow curve deconvolution method (GCD). The increase in TL peak intensity of the glow curve was observed as fluence increase.
聚苯乙烯聚合物(PS)/AlO 纳米复合材料薄膜是通过溶液浇铸法从 PS:AlO(1-x):x 混合物(x=3wt%)合成的。这些纳米复合材料薄膜暴露于不同注量的 5MeV 质子束下。使用傅里叶变换红外光谱(FTIR)、紫外-可见光谱、光致发光和热致发光研究研究了质子束诱导 PS 和 PS:AlO 薄膜光学和发光性质的变化。FTIR 研究表明,由于掺杂 AlO 和质子辐照,峰强度降低。紫外-可见光谱显示随着注量的增加吸收边缘发生移动。这可以归因于键的共轭体系的形成。PS 和 3wt%AlO 掺杂 PS 的能带隙分别观察到为 4.38eV 和 4.34eV,而质子辐照 3wt%AlO 掺杂 PS 薄膜的能带隙在注量为 1×10 离子/cm 和 1×10 离子/cm 时分别为 4.28eV 和 4.23eV。光致发光发射光谱在激发近紫外波长 380nm 时显示三个峰值,波长分别为 411nm、435nm 和 462nm,对应于 PS 的紫蓝色区域。随着注量的增加,发射峰的强度增加。使用发光曲线解卷积方法(GCD)分析 PS/AlO 的热致发光曲线。随着注量的增加,观察到热致发光曲线的 TL 峰强度增加。