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同位素工程石墨烯体系的拉曼光谱和原位拉曼光谱电化学。

Raman spectroscopy and in situ Raman spectroelectrochemistry of isotopically engineered graphene systems.

机构信息

J. Heyrovský Institute of Physical Chemistry of the Academy of Sciences of the Czech Republic , v.v.i., Dolejškova 3, CZ-18223 Prague 8, Czech Republic.

出版信息

Acc Chem Res. 2015 Jan 20;48(1):111-8. doi: 10.1021/ar500384p. Epub 2015 Jan 8.

Abstract

CONSPECTUS

The special properties of graphene offer immense opportunities for applications to many scientific fields, as well as societal needs, beyond our present imagination. One of the important features of graphene is the relatively simple tunability of its electronic structure, an asset that extends the usability of graphene even further beyond present experience. A direct injection of charge carriers into the conduction or valence bands, that is, doping, represents a viable way of shifting the Fermi level. In particular, electrochemical doping should be the method of choice, when higher doping levels are desired and when a firm control of experimental conditions is needed. In this Account, we focus on the electrochemistry of graphene in combination with in situ Raman spectroscopy, that is, in situ Raman spectroelectrochemistry. Such a combination of methods is indeed very powerful, since Raman spectroscopy not only can readily monitor the changes in the doping level but also can give information on eventual stress or disorder in the material. However, when Raman spectroscopy is employed, one of its main strengths lies in the utilization of isotope engineering during the chemical vapor deposition (CVD) growth of the graphene samples. The in situ Raman spectroelectrochemical study of multilayered systems with smartly designed isotope compositions in individual layers can provide a plethora of knowledge about the mutual interactions (i) between the graphene layers themselves, (ii) between graphene layers and their directly adjacent environment (e.g., substrate or electrolyte), and (iii) between graphene layers and their extended environment, which is separated from the layer by a certain number of additional graphene layers. In this Account, we show a few examples of such studies, from monolayer to two-layer and three-layer specimens and considering both turbostratic and AB interlayer ordering. Furthermore, the concept and the method can be extended further beyond the three-layer systems, for example, to heterostructures containing other 2-D materials beyond graphene. Despite a great deal of important results being unraveled so far through the in situ spectroelectrochemistry of graphene based systems, many intriguing challenges still lie immediately ahead. For example, apart from the aforementioned 2-D heterostructures, a substantial effort should be put into a more detailed exploration of misoriented (twisted) bilayer or trilayer graphenes. Marching from the oriented, AB-stacked to AA-stacked, bilayers, every single angular increment of the twist between the layers creates a new system in terms of its electronic properties. Mapping those properties and interlayer interactions dependent on the twist angle represents a sizable task, yet the reward might be the path toward the realization of various types of advanced devices. And last but not least, understanding the electrochemistry of graphene paves the way toward a controlled and targeted functionalization of graphene through redox reactions, especially when equipped with the possibility of an instantaneous monitoring of the thus introduced changes to the electronic structure of the system.

摘要

概述

石墨烯的特殊性质为许多科学领域以及超出我们目前想象的社会需求提供了巨大的应用机会。石墨烯的一个重要特点是其电子结构相对简单的可调谐性,这一特性进一步扩展了石墨烯的可用性,超出了目前的经验。向导带或价带中直接注入电荷载流子,即掺杂,是一种可行的移动费米能级的方法。特别是,当需要更高的掺杂水平并且需要严格控制实验条件时,电化学掺杂应该是首选方法。在本报告中,我们专注于与原位拉曼光谱相结合的石墨烯电化学,即原位拉曼光谱电化学。这种方法的结合确实非常强大,因为拉曼光谱不仅可以很容易地监测掺杂水平的变化,还可以提供关于材料中最终的应变或无序的信息。然而,当使用拉曼光谱时,其主要优势之一在于在石墨烯样品的化学气相沉积(CVD)生长过程中利用同位素工程。通过在各个层中设计具有智能同位素组成的多层系统的原位拉曼光谱电化学研究,可以提供关于(i)石墨烯层本身之间、(ii)石墨烯层与其直接相邻环境(例如,基底或电解质)之间以及(iii)石墨烯层与其扩展环境之间的相互作用的大量知识,扩展环境通过若干个附加的石墨烯层与层分离。在本报告中,我们展示了一些此类研究的示例,从单层到双层和三层样品,并考虑了类石墨和 AB 层间有序。此外,该概念和方法可以进一步扩展到三层系统之外,例如,扩展到包含除石墨烯之外的其他二维材料的异质结构。尽管通过基于石墨烯的系统的原位光谱电化学已经揭示了大量重要结果,但仍然存在许多有趣的挑战。例如,除了上述二维异质结构之外,还应该投入大量精力更详细地探索错位(扭曲)双层或三层石墨烯。从取向的 AB 堆叠双层到 AA 堆叠双层,层之间的每一个扭转角度的增量都会在电子性质方面创造一个新的系统。根据扭转角度绘制这些性质和层间相互作用代表了一项相当大的任务,但回报可能是实现各种类型的先进设备的途径。最后但同样重要的是,对石墨烯电化学的理解为通过氧化还原反应对石墨烯进行可控和靶向功能化铺平了道路,尤其是当配备对系统电子结构的这种引入变化进行即时监测的可能性时。

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