Kepić Dejan, Milović Miloš, Sredojević Dušan, Stefanović Andjela, Gajić Brankica, Mead James L, Nardin Blaž, Likozar Blaž, Teržan Janvit, Yasir Muhammad, Saeed Warda, Jovanović Svetlana
Vinča Institute of Nuclear Sciences - National Institute of the Republic of Serbia, University of Belgrade, Mihajla Petrovića Alasa 12-14, Belgrade, 11351, Serbia.
Faculty of Chemistry, University of Belgrade, Studentski trg 12-16, Belgrade, 11158, Serbia.
Sci Rep. 2025 Jul 24;15(1):26924. doi: 10.1038/s41598-025-12655-7.
A low-dose gamma irradiation was used for the one-step synthesis of graphene oxide/platinum nanoparticle composites. Various spectroscopic and microscopic methods were employed to structurally and morphologically characterize the prepared composites, and the nature of the interactions between graphene oxide sheets and platinum clusters was investigated using density function theory (DFT). Gamma irradiation caused the reduction of hexachloroplatinic acid, resulting in the formation of Pt nanoparticles and the simultaneous partial reduction of graphene oxide (GO). Pt nanoparticles synthesized at doses of 10 and 20 kGy showed a homogeneous GO surface coverage with a high portion of particles with sizes of up to 10 nm. The DFT results indicate a difference in electrical conductivity between GO and PtNPs. This could cause charge redistribution across the contact area, creating a conductive network at the interface that should enhance the EMI shielding capabilities of the composite. The shielding efficiency of the composites measured at the X band showed a blockage of 77% of the incident electromagnetic wave at a center frequency of 10 GHz. The composite prepared at a 20 kGy dose exhibited a greater contribution from a mismatch loss component, attributed to the improved electrical conductivity induced by irradiation.
采用低剂量伽马射线辐照一步合成氧化石墨烯/铂纳米颗粒复合材料。运用多种光谱和显微镜方法对制备的复合材料进行结构和形态表征,并使用密度泛函理论(DFT)研究氧化石墨烯片层与铂簇之间相互作用的性质。伽马射线辐照导致六氯铂酸还原,从而形成铂纳米颗粒,同时氧化石墨烯(GO)也发生部分还原。在10和20 kGy剂量下合成的铂纳米颗粒在GO表面呈现均匀覆盖,且大部分颗粒尺寸达10 nm。DFT结果表明GO和PtNPs之间存在电导率差异。这可能导致电荷在接触区域重新分布,在界面处形成导电网络,进而增强复合材料的电磁干扰屏蔽能力。在X波段测量的复合材料屏蔽效率显示,在10 GHz中心频率下,入射电磁波的阻挡率为77%。在20 kGy剂量下制备的复合材料中,失配损耗分量的贡献更大,这归因于辐照诱导的电导率提高。