Mitra Surjyasish, Hamada Natalie, Mitra Sushanta K
Department of Mechanical & Mechatronics Engineering, Waterloo Institute for Nanotechnology, University of Waterloo Waterloo Ontario N2L 3G1 Canada
Canadian Centre for Electron Microscopy, McMaster University 1280 Main St W Hamilton ON L8S 4L8 Canada
RSC Adv. 2024 Aug 12;14(35):25307-25315. doi: 10.1039/d4ra04893h.
The interaction of graphene with gold nanoparticles is investigated using transmission electron microscopy. We observe gold-nanoparticle-mediated etching of graphene flakes, often leading to hole formation. Further, using a combination of high-angle annular dark field imaging and electron energy loss spectroscopy, we highlight that the catalytic effects of gold nanoparticles on graphene lead to the formation of amorphous carbon layers. From the extracted diffractograms, we observe regions with diffraction halos as well as some regions with a weak tetrahedral motif. Using independently performed Raman measurements, we confirm the presence of tetrahedral amorphous carbon as well as mixed graphitic-amorphous regions. For the amorphous carbon regions with mixed sp-sp states, the Raman G peak is red-shifted to 1564 cm and an / ratio of 0.63 indicates less than 20% sp content. For the tetrahedral amorphous carbon regions, we observe that the Raman G peak is at 1580 cm, close to that of monolayer graphene. However, there is no Raman D peak, , / = 0, which indicates close to 100% sp content. The translation of the Raman G peak location and the / ratios is on par with the amorphization trajectory analysis of Ferrari and Robertson (, 2000, , 14095) and validates the conversion route of graphite to amorphous carbon to tetrahedral amorphous carbon. The presented method provides a promising pathway for creating defect-induced amorphous carbon at room temperature, which has a broader impact on the electronics and semiconductor industries.
利用透射电子显微镜研究了石墨烯与金纳米颗粒的相互作用。我们观察到金纳米颗粒介导的石墨烯薄片蚀刻,这通常会导致孔洞形成。此外,结合高角度环形暗场成像和电子能量损失谱,我们强调金纳米颗粒对石墨烯的催化作用会导致非晶碳层的形成。从提取的衍射图中,我们观察到有衍射晕的区域以及一些具有弱四面体图案的区域。通过独立进行的拉曼测量,我们证实了四面体非晶碳以及石墨 - 非晶混合区域的存在。对于具有混合sp - sp状态的非晶碳区域,拉曼G峰红移至1564 cm,且I / I 比率为0.63表明sp含量小于20%。对于四面体非晶碳区域,我们观察到拉曼G峰位于1580 cm,接近单层石墨烯的G峰位置。然而,没有拉曼D峰,I / I = 0,这表明sp含量接近100%。拉曼G峰位置和I / I 比率的变化与法拉利和罗伯逊(2000年,14095)的非晶化轨迹分析一致,并验证了石墨向非晶碳再向四面体非晶碳的转化途径。所提出的方法为在室温下创建缺陷诱导的非晶碳提供了一条有前景的途径,这对电子和半导体行业具有更广泛的影响。