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从分子到氢化纳米金刚石的红外振动光谱的尺寸变化:密度泛函理论研究。

Size variation of infrared vibrational spectra from molecules to hydrogenated diamond nanocrystals: a density functional theory study.

机构信息

Ministry of Science and Technology, Baghdad, Iraq; Tel. +964-7901335231.

出版信息

Beilstein J Nanotechnol. 2013 Apr 15;4:262-8. doi: 10.3762/bjnano.4.28. Print 2013.

DOI:10.3762/bjnano.4.28
PMID:23766948
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3678429/
Abstract

Infrared spectra of hydrogenated diamond nanocrystals of one nanometer length are calculated by ab initio methods. Positions of atoms are optimized via density functional theory at the level of the generalized gradient approximation of Perdew, Burke and Ernzerhof (PBE) using 3-21G basis states. The frequencies in the vibrational spectrum are analyzed against reduced masses, force constants and intensities of vibration. The spectrum can be divided into two regions depending on the properties of the vibrations or the gap separating them. In the first region, results show good matching to several experimentally obtained lines. The 500 cm(-1) broad-peak acoustical branch region is characterized by pure C-C vibrations. The optical branch is centered at 1185 cm(-1). Calculations show that several C-C vibrations are mixed with some C-H vibrations in the first region. In the second region the matching also extends to C-H vibration frequencies that include different modes such as symmetric, asymmetric, wagging, scissor, rocking and twisting modes. In order to complete the picture of the size dependence of the vibrational spectra, we analyzed the spectra of ethane and adamantane. The present analysis shows that acoustical and optical branches in diamond nanocrystals approach each other and collapse at 963 cm(-1) in ethane. Variation of the highest reduced-mass-mode C-C vibrations from 1332 cm(-1) of bulk diamond to 963 cm(-1) for ethane (red shift) is shown. The analysis also shows the variation of the radial breathing mode from 0 cm(-1) of bulk diamond to 963 cm(-1) for ethane (blue shift). These variations compare well with experiment. Experimentally, the above-mentioned modes appear shifted from their exact positions due to overlap with neighboring modes.

摘要

利用从头算方法计算了一纳米长的氢化金刚石纳米晶的红外光谱。通过密度泛函理论,在 Perdew、Burke 和 Ernzerhof(PBE)广义梯度近似水平上,使用 3-21G 基态对原子位置进行了优化。在振动光谱中,根据折合质量、力常数和振动强度对频率进行了分析。该光谱可根据振动的性质或分隔它们的间隙分为两个区域。在第一区域,结果与几个实验获得的谱线吻合较好。500 cm(-1)宽的声学支区域的特征是纯 C-C 振动。光学支位于 1185 cm(-1)。计算表明,在第一区域中,几个 C-C 振动与一些 C-H 振动混合。在第二区域中,匹配也扩展到了包括不同模式的 C-H 振动频率,例如对称、不对称、摇摆、剪刀、摇滚和扭曲模式。为了完成振动光谱尺寸依赖性的全貌,我们分析了乙烷和金刚烷的光谱。目前的分析表明,金刚石纳米晶中的声学和光学支彼此接近,并在乙烷中在 963 cm(-1)处坍塌。从体相金刚石的 1332 cm(-1)到乙烷的 963 cm(-1)(红移),最高折合质量模式 C-C 振动的变化显示出来。分析还表明,从体相金刚石的 0 cm(-1)到乙烷的 963 cm(-1)(蓝移),径向呼吸模式的变化。这些变化与实验吻合较好。实验上,由于与相邻模式的重叠,上述模式出现了从其精确位置的位移。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/aa494c001205/Beilstein_J_Nanotechnol-04-262-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/3d605731f5cf/Beilstein_J_Nanotechnol-04-262-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/87580db01094/Beilstein_J_Nanotechnol-04-262-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/9c4ff43cf3dd/Beilstein_J_Nanotechnol-04-262-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/bf5ccd494193/Beilstein_J_Nanotechnol-04-262-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/aa494c001205/Beilstein_J_Nanotechnol-04-262-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/3d605731f5cf/Beilstein_J_Nanotechnol-04-262-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/87580db01094/Beilstein_J_Nanotechnol-04-262-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/9c4ff43cf3dd/Beilstein_J_Nanotechnol-04-262-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/bf5ccd494193/Beilstein_J_Nanotechnol-04-262-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/53a0/3678429/aa494c001205/Beilstein_J_Nanotechnol-04-262-g006.jpg

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