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Raman spectra of graphite edge planes; edge planes of HOPG prepared by Ar ion cutting and Kish graphite formed on its crystal grain

机译:石墨边缘平面的拉曼光谱通过Ar离子切割制备的HOPG的端面和在其晶粒上形成的Kish石墨

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Only a few studies on Raman scattering from graphite edge planes have been conducted using HOPG edge planes, because of difficulty in preparation. Compagnini et al. found a feature at 1351 cm~(-1) for the virgin edge plane of their HOPG sample in addition to the G band at 1580 cm~(-1) using the 514.5 nm excitation. After irradiating with Ar ions, they obtained a doublet D band for the edge plane and an additional feature at 1360 cm~(-1) for the basal plane of HOPG (Compagnini et al. 1997). For the doublet D band, they determined the position of the lower energy peak (Dpline) at 1351 cm~(-1) and the higherenergy peak (D_2-line) at 1360 cm~(-1). They attributed also the D_1-line to the rupture of the space symmetry D_(6h)~4 and the D_2-line to the disorder induced line. Kawashima and Katagiri measured a singlet D band at 1355 cm~(-1) for the polished edge plane of HOPG (Kawashima and Katagiri 1999). They also measured a weak feature at 1621 cm~(-1) (D' band) and related it to disorder. However, Compagnini et al. did not mention the D' band. On the other hand, Tan et al. studied Raman scattering from natural graphite edge planes (Tan et al. 2004). They reported two features of Raman spectra showing clear doublets of D and D' bands for three different laser excitations. For the 514.5 nm excitation, the D band was found to consist of the D_1-line at 1352 cm~(-1) and the D_2-line at 1369 cm~(-1) while the D' band was comprised of the D'_1-line at 1620 cm~(-1) and the D'_2-line at 1624 cm~(-1).A method to prepare the edge plane of graphite crystal such as HOPG using Ar-ion polishing was developed in the present study. Measurement of the first order Raman spectrum was conducted in the present study on the edge plane of HOPG thus prepared to examine details of the D band and also the appearance of the D' band in relation to the D band. The measurements were also made for edge planes of Kish graphite crystals, for comparison.
机译:由于制备困难,仅使用HOPG边缘平面对石墨边缘平面的拉曼散射进行了一些研究。 Compagnini等。在514.5 nm激发下,除了在1580 cm〜(-1)处的G带外,他们还发现了HOPG样品原始边缘平面在1351 cm〜(-1)处的特征。用Ar离子辐照后,他们在边缘平面获得了一个双峰D带,在HOPG的基础平面上获得了1360 cm〜(-1)的附加特征(Compagnini等,1997)。对于双峰D带,他们确定了1351 cm〜(-1)处较低能量峰(Dpline)和1360 cm〜(-1)处较高能量峰(D_2-line)的位置。他们还将D_1线归因于空间对称性D_(6h)〜4的破裂,并将D_2线归因于无序诱导线。 Kawashima和Katagiri在HOPG的抛光边缘平面上在1355 cm〜(-1)处测量了一条单重态D带(Kawashima和Katagiri 1999)。他们还测量了1621 cm〜(-1)(D'波段)的弱点,并将其与无序相关。但是,Compagnini等。没有提到D'乐队。另一方面,谭等。研究了天然石墨边缘平面的拉曼散射(Tan等,2004)。他们报告了拉曼光谱的两个特征,显示了三种不同激光激发的D和D'波段清晰的二重峰。对于514.5 nm激发,发现D谱带由1352 cm〜(-1)的D_1线和1369 cm〜(-1)的D_2线组成,而D'谱带由D'谱线组成在1620 cm〜(-1)处的_1线和在1624 cm〜(-1)处的D'_2线。目前开发了一种使用Ar离子抛光制备石墨晶体如HOPG的边缘平面的方法研究。在本研究中对HOPG的边缘平面进行了一阶拉曼光谱的测量,由此准备检查D带的细节以及与D带相关的D'带的外观。为了比较,还对Kish石墨晶体的边缘平面进行了测量。

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