Itoh K, Kudryashov I, Yamagata J, Nishizawa T, Fujii M, Osaka N
Department of Chemistry, School of Science and Engineering, Waseda University, Tokyo 169-8555, Japan.
J Phys Chem B. 2005 Jan 13;109(1):271-6. doi: 10.1021/jp0403644.
Confocal Raman microscopic measurements were performed at room temperature on the Langmuir-Blodgett (LB) monolayer of 10,12-pentacosadiynoic acid (DA) prepared on surface enhanced Raman scattering (SERS) active Ag island films, two-dimensional (2D) Raman images of which exhibit bright and dim spots on a dark background. The measurements performed by focusing the excitation laser light (488 nm) on the dark background indicate the prompt appearance of the Raman bands (1515 and 2115 cm(-1)) due to polydiacetylene (PDA) in the red phase and subsequent diminution of the Raman bands. On the other hand, the spectra observed by focusing the excitation laser spot on the dim and bright spots exhibit almost random fluctuations, giving rather narrow Raman bands in the 1620-1000 cm(-1) region, which appear and disappear temporarily with varying intensities under the continuous irradiation at 488 nm. Broad Raman bands appear around 1580 and 1360 cm(-1), which are ascribable to amorphous carbon, at a later stage of the observation, the intensities from the bright spot being more than 100 times stronger than those from the dim spot. The narrow bands are ascribed to a series of carbonaceous intermediates such as polyenes, graphite sheets with various sizes, and folded or reorganized forms of the sheets including carbon nanotubes and fullerenes, which are formed during the conversion of PDA to amorphous carbon. The random spectral fluctuation was interpreted by considering that the intermediates undergo thermally activated diffusion and get temporarily in contact with the SERS-active site, resulting in the enhancement of their Raman bands and the fluctuation.
在室温下,对制备在表面增强拉曼散射(SERS)活性银岛膜上的10,12-二十五碳二炔酸(DA)的朗缪尔-布洛杰特(LB)单分子层进行了共焦拉曼显微镜测量,其二维(2D)拉曼图像在暗背景上呈现出亮点和暗点。通过将激发激光(488 nm)聚焦在暗背景上进行的测量表明,由于红色相中的聚二乙炔(PDA),拉曼带(1515和2115 cm⁻¹)迅速出现,随后拉曼带减弱。另一方面,通过将激发激光光斑聚焦在暗点和亮点上观察到的光谱呈现出几乎随机的波动,在1620 - 1000 cm⁻¹区域给出相当窄的拉曼带,这些拉曼带在488 nm连续照射下强度变化时会暂时出现和消失。在观察后期,在1580和1360 cm⁻¹附近出现宽拉曼带,这归因于无定形碳,亮点的强度比暗点的强度强100倍以上。窄带归因于一系列含碳中间体,如多烯、各种尺寸的石墨片以及包括碳纳米管和富勒烯在内的片层的折叠或重组形式,这些中间体是在PDA向无定形碳转化过程中形成的。通过考虑中间体经历热激活扩散并暂时与SERS活性位点接触,从而导致其拉曼带增强和波动,对随机光谱波动进行了解释。