首页> 外文期刊>Vibrational Spectroscopy: An International Journal devoted to Applications of Infrared and Raman Spectroscopy >Calculated dependence of vibrational band frequencies of single-walled and double-walled carbon nanotubes on diameter
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Calculated dependence of vibrational band frequencies of single-walled and double-walled carbon nanotubes on diameter

机译:计算单壁和双壁碳纳米管振动带频率直径的依赖性

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摘要

We have used density functional theory (DFT) at the B3LYP/6-31G level to calculate Raman and 1R spectra of zigzag (n,0) single-walled carbon nanotubes (SWNTs) and (n,0) and (2n,0) double-walled carbon nanotubes (DWNTs), for n ranging from 6 to 19 and 6 to 8, respectively. In the low frequency RBM region, calculated Raman spectra of SWNTs indicate that there are three vibrational modes, with symmetries A_(1g), E_(1g) and E_(2g), whose frequencies depend strongly on nanotube diameter. The E_(2g) mode is not only diameter dependent, but also depends on whether the number of hexagons formed in the circumference direction of the CNT is even or odd. Two IR spectral modes (of A_(2u) and E_(1u) symmetries) are found in calculated IR spectra that show strong diameter dependence. Also, three Raman bands with E_(1g), A_(1g) and E_(2g) symmetries found are to exist in the G-band region. For this latter case, computed spectra indicate that while Raman bands with A_(1g) symmetry essentially remain constant for even number of hexagons formed in the circumference direction, (e.g., (0,2n)-type CNTs with band position 1526 ± 0.5 cm~(-1)), bands corresponding to odd number of hexagons, i.e., (0,2n +1 )-type CNTs, are diameter dependent. The frequencies of the E_(1g) and E_(2g) modes (in the G-band region) are not only strongly diameter dependent, but also converge towards one another with increasing tube diameter. This latter type of behavior can lead to erroneous classification of nanotubes as metallic or semiconducting, since partially overlapping bands in the G-band region might result in bands that appear to have diffuse shoulders, a characteristic of metallic SWNTs. The RBMs for DWNTs are also strongly diameter dependent and are blue-shifted relative to their corresponding RBMs in the spectra of SWNTs. The relative distance between RBMs vibrational modes in the spectrum of a selected DWNT is larger than that for the corresponding SWNTs. The electron density for small-sized DWNT, e.g., (6,0)&( 12,0), indicates an intratube (inner-outer tube) cr-bonding in the excited state.
机译:我们在B3LYP / 6-31G级别使用密度泛函理论(DFT)以计算Z字形(N,0)单壁碳纳米管(SWNT)和(N,0)和(2N,0)的拉曼和1R光谱双壁碳纳米管(DWNT),用于分别为6至19和6至8。在低频RBM区域中,SWNT的计算拉曼光谱表明存在三种振动模式,具有对称A_(1G),E_(1G)和E_(2G),其频率在纳米管直径上强烈地取决于纳米管直径。 E_(2g)模式不仅直径依赖性,而且还取决于在CNT的圆周方向上形成的六边形的数量是偶数还是奇数。在计算的IR光谱中发现了两个IR光谱模式(A_(2U)和E_(1U)对称),其显示出强直径依赖性的IR光谱。此外,在G波段区域中找到了具有E_(1G),A_(1G)和E_(2G)对称性的三个拉曼频带。对于这种后一种情况,计算光谱表明,当具有A_(1G)对称的拉曼带基本上保持恒定,偶数在圆周方向上形成的六边形数量,(例如,具有带位置的带位置1526±0.5cm的(0.2n)型Cnts 〜(-1)),对应于奇数六边形的频带,即(0,2n +1)-type cnts是直径的。 E_(1G)和E_(2G)模式(在G带区域中)的频率不仅具有强烈的直径,而且还通过增加管直径朝向彼此收敛。后一种行为可以导致纳米管的错误分类为金属或半导体,因为G波段区域中的部分重叠带可能导致似乎具有漫射肩部的条带,所以金属SWNT的特征。对于DWNT的RBMS也是强烈的直径依赖性,并且在SWNT的光谱中相对于它们的相应RBMS是蓝移位。所选DWNT的频谱中的RBMS振动模式之间的相对距离大于相应SWNT的频谱。小尺寸DWNT,例如(6,0)&(12,0)的电子密度表示激发状态下的钻子子(内外管)Cr键合。

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