光谱学与光谱分析, 2010, 30 (12): 3244, 网络出版: 2011-01-26  

3.3′二乙基硫醛三碳菁化碘拉曼光谱研究

Raman Spectrum Study of 3.3′-Diethylthiatri Carbocyanine Iodide
作者单位
1 长春理工大学纳米光子学与生物光子学国际联合研究中心, 吉林 长春130022
2 纽约州立大学布法罗分校激光、 光子学与生物光子学研究所, 美国 纽约14260-4200
3 长春理工大学计算机科学与技术学院, 吉林 长春130022
4 吉林大学数学学院, 吉林 长春130012
摘要
给出了3.3′二乙基硫醛三碳菁化碘(DTTC)分子的自然拉曼光谱、 表面增强拉曼光谱(SERS)、 以及理论计算拉曼光谱. SERS谱的增强基底是直径60 nm的金球和50 nm长的金棒, 外包附一层硫基聚乙二醇(thiol-polyethylene glycol, 简称Mpeg-SH)做为稳定层. 同时, 采用密度泛函(DFT)方法计算了DTTC分子的拉曼光谱, 计算基于B3LYP/6-31G基组. 经过仔细对比, 计算光谱和两种实测光谱特征峰位有很好的一致性. 对于不一致的部分, 分析原因可能是由于金纳米粒子表面等离子体波对于不同的峰位, 其增强程度不同所引起的. 这项工作将有利于基于DTTC分子的红外波段拉曼光谱技术在生化领域的应用.
Abstract
3.3′-diethylthiatricarbocyanine iodide (DTTC) dye is an important infrared Raman probe molecule, and has received great attention in the past decades due to their potential applications in Raman imaging, single cell detection, and tumor marker. In the present work, ordinary Raman, surface enhanced Raman scattering (SERS), and theoretical Raman spectra were given to estimate the Raman spectrum of DTTC suspension. More specifically, the original gold nanospheres (60-nm diameter) and gold nanorods (NRs) were encoded with DTTC and stabilized with a layer of thiol-polyethylene glycol (PEG) as Raman reporter, and SERS data were obtained from the samples. Density functional theory (DFT) calculation was applied to calculate the optimized Raman spectra of DTTC water solvent on a B3LYP/6-31G level. Subsequently, the obtained experimental spectra from the DTTC were carefully compared with the theoretically calculated spectra. From the spectra comparation, good agreements were obtained between the theoretical and experimental results. This work will facilitate the development of ultrasensitive SERS probes for advanced biomedical applications.

蔡红星, 张宇, Ken-Tye Yong, 邵桢, 李源珣, 张喜和. 3.3′二乙基硫醛三碳菁化碘拉曼光谱研究[J]. 光谱学与光谱分析, 2010, 30(12): 3244. CAI Hong-xing, ZHANG Yu, Ken-Tye Yong, SHAO Zhen, LI Yuan-xun, ZHANG Xi-he. Raman Spectrum Study of 3.3′-Diethylthiatri Carbocyanine Iodide[J]. Spectroscopy and Spectral Analysis, 2010, 30(12): 3244.

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