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Chemical vapor deposition of graphene: Synthesis, characterization, and applications.

机译:石墨烯的化学气相沉积:合成,表征和应用。

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Chapter 1 gives a brief introduction of graphene, the electrical properties of graphene, and chemical vapor deposition method of graphene synthesis.;Chapter 2 discusses a simple, scalable and cost-efficient method to prepare graphene using methane-based chemical vapor deposition on nickel films deposited over complete Si/SiO2 wafers. By using highly diluted methane, single- and few-layer graphene were obtained, as confirmed by micro Raman spectroscopy. In addition, a transfer technique has been applied to transfer the graphene film to target substrates via nickel etching. Field-effect transistors based on the graphene films transferred to Si/SiO2 substrates revealed a weak p-type gate dependence, while transferring of the graphene films to glass substrate allowed its characterization as transparent conductive films, exhibiting transmittance of 80% in the visible wavelength range.;In chapter 3, continuous, highly flexible, and transparent few-layer graphene films synthesized from Ni film were implemented as transparent conductive electrodes (TCE) in organic photovoltaic cells. Graphene films were synthesized by CVD, transferred to transparent substrates, and evaluated in organic solar cell heterojunctions (TCE/poly-3,4-ethylenedioxythiophene:poly styrenesulfonate (PEDOT:PSS)/copper phthalocyanine/fullerene/bathocuproine/aluminum). Key to our success is the continuous nature of the CVD graphene films, which led to minimal surface roughness (∼0.9 nm) and offered sheet resistance down to 230 Ω/sq (at 72% transparency), much lower than stacked graphene flakes at similar transparency.;In chapter 4, we discuss comparative study and Raman characterization on the formation of graphene on single crystal Ni (111) and polycrystalline Ni substrates using chemical vapor deposition. Preferential formation of monolayer/bilayer graphene on the single crystal surface is attributed to its atomically smooth surface and the absence of grain boundaries. In contrast, CVD graphene formed on polycrystalline Ni leads to higher percentage of multilayer graphene (≥3 layers), which is attributed to the presence of grain boundaries in Ni that can serve as nucleation sites for multilayer growth.;Chapter 5 discusses a vapor trapping method for the growth of large-grain, single-crystalline graphene flowers with grain size up to 100 µm. Controlled growth of graphene flowers with four lobes and six lobes has been achieved by varying the growth pressure and the methane to hydrogen ratio. Surprisingly, electron backscatter diffraction study revealed that the graphene morphology had little correlation with the crystalline orientation of underlying copper substrate.Our vapor trapping method provides a viable way for large-grain single-crystalline graphene synthesis for potential high-performance graphene-based electronics.;In chapter 6, a simple, clean, and highly anisotropic hydrogen etching method was developed for chemical vapor deposited graphene catalyzed by the copper substrate. By exposing CVD graphene on copper foil to hydrogen flow around 800 °C, we observed that the initially continuous graphene can be etched to have many hexagonal openings. In addition, we found that the etching is temperature dependent. Compared to other temperatures (700, 900, and 1000 °C), etching of graphene at 800 °C is most efficient and anisotropic. Of the angles of graphene edges after etching, 80% are 120°, indicating the etching is highly anisotropic. No increase of the D band along the etched edges indicates that the crystallographic orientation of etching is in the zigzag direction. Furthermore, we observed that copper played an important role in catalyzing the etching reaction, as no etching was observed for graphene transferred to Si/SiO2 under similar conditions. This highly anisotropic hydrogen etching technology may work as a simple and convenient way to determine graphene crystal orientation and grain size and may enable the etching of graphene into nanoribbons for electronic applications.
机译:第1章简要介绍了石墨烯,石墨烯的电学性质以及石墨烯合成的化学气相沉积方法。第2章讨论了一种简单,可扩展且经济高效的方法,该方法是在甲烷膜上使用甲烷基化学气相沉积法制备石墨烯。沉积在完整的Si / SiO2晶圆上。通过使用高稀释的甲烷,获得了单层和多层石墨烯,这已通过显微拉曼光谱法证实。另外,已经应用转移技术通过镍蚀刻将石墨烯膜转移到目标基板。基于转移到Si / SiO2衬底上的石墨烯膜的场效应晶体管显示出弱的p型栅极依赖性,而将石墨烯膜转移到玻璃衬底允许其表征为透明导电膜,在可见光波长下显示80%的透射率在第三章中,将由Ni膜合成的连续,高柔性和透明的多层石墨烯膜用作有机光伏电池中的透明导电电极(TCE)。石墨烯薄膜是通过CVD合成的,转移到透明基板上,并在有机太阳能电池异质结中进行评估(TCE /聚-3,4-乙撑二氧噻吩:聚苯乙烯磺酸盐(PEDOT:PSS)/铜酞菁/富勒烯/四苯甲嘌呤/铝)。我们成功的关键是CVD石墨烯薄膜的连续性,这导致最小的表面粗糙度(约0.9 nm),并且薄层电阻低至230Ω/ sq(在72%的透明度下),远低于类似条件下的堆叠石墨烯薄片在第四章中,我们讨论了使用化学气相沉积法在单晶Ni(111)和多晶Ni衬底上形成石墨烯的比较研究和拉曼表征。单晶/单层石墨烯在单晶表面上的优选形成归因于其原子上光滑的表面和不存在晶界。相比之下,在多晶镍上形成的CVD石墨烯导致多层石墨烯(≥3层)的百分比更高,这归因于Ni中存在可以用作多层生长成核位点的晶界。第5章讨论了气相捕集。种方法,用于生长粒径最大为100 µm的大晶粒单晶石墨烯花。通过改变生长压力和甲烷与氢的比例,实现了具有四个裂片和六个裂片的石墨烯花的受控生长。出乎意料的是,电子背散射衍射研究表明,石墨烯的形态与下层铜基板的晶体取向几乎没有相关性。我们的气相俘获方法为大尺寸单晶石墨烯的合成提供了可行的方法,以用于潜在的高性能石墨烯基电子产品。 ;在第6章中,开发了一种简单,清洁且高度各向异性的氢蚀刻方法,用于在铜基底的催化下化学气相沉积石墨烯。通过将铜箔上的CVD石墨烯暴露于约800°C的氢气流,我们观察到可以将最初连续的石墨烯蚀刻成许多六角形开口。此外,我们发现蚀刻与温度有关。与其他温度(700、900和1000°C)相比,在800°C下蚀刻石墨烯是最有效且各向异性的。蚀刻后的石墨烯边缘的角度中,有80%为120°,表明蚀刻是高度各向异性的。沿着蚀刻边缘的D带没有增加表明蚀刻的晶体学取向是在Z字形方向上。此外,我们观察到铜在催化蚀刻反应中起着重要作用,因为在相似条件下未观察到转移至Si / SiO2的石墨烯的蚀刻。这种高度各向异性的氢蚀刻技术可以作为确定石墨烯晶体取向和晶粒尺寸的简单便捷方式,并且可以将石墨烯蚀刻成纳米带,用于电子应用。

著录项

  • 作者

    Zhang, Yi.;

  • 作者单位

    University of Southern California.;

  • 授予单位 University of Southern California.;
  • 学科 Chemistry Inorganic.;Nanoscience.;Nanotechnology.
  • 学位 Ph.D.
  • 年度 2012
  • 页码 179 p.
  • 总页数 179
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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