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The Fullerene C <sub> 60 </ Sub> Nano Preparation And Fluorescence Spectra Of Ultra-thin Films

Posted on:2010-12-03Degree:MasterType:Thesis
Country:ChinaCandidate:Y WangFull Text:PDF
GTID:2191360275965403Subject:Optics
Abstract/Summary:PDF Full Text Request
Since the discovery of the C60 molecule in 1985, it attracts much attention for its ideal symmetry, unique physical and chemical properties and potential applications. In 1990, Kratschmer and Huffman discovered an efficient preparation method for high pour C60, the properties of C60 have been extensively studied by scientists. Because of the photoelectricity characteristic of C60, the study of constructing planar ordered structure become hot.The Langmuir-Blodgett (LB) technique is one of the most powerful tools to form organic ultrathin films in molecular thickness. So it is an attractive idea to form C60 LB film, and to measure their PL. Usually film-forming molecules should be amphiphilic. C60 molecule is not a typical amphiphilic molecule. When C60 was spread on the air-water surface, the molecules of C60 always aggregated. So it is very difficult to fabricate homogeneous pure C60 LB film. And as a result very few works on PL of C60 LB films have been carried out. The reports of the PL spectra of C60 LB films are also very few.C60 is of great interest because of the numerous potential applications in physics and chemistry. Among the properties of C60, photoluminescence (PL) which has potential application in areas such as optics, electrics, materials science and biomedicine et al is of great importance. It is significant to investigate the emission mechanism to achieve high-quality PL of C60, especially at room temperature. In the last years many studies have been focused on the optical characterization of both C60 molecules and solid fullerite. In particular, PL measurements have been performed on dilute molecular solutions, films, polycrystalline powders and single crystals. The PL spectra of C60 film, which have been fabricated using many methods, such as powder sublimation, epitaxial growth, cast film and so on, have been measured on varies substrate. Many groups found that the PL spectra of C60 film depending on the temperature greatly and only under low temperature(≤10 K) can we get rich PL emission.In this paper, we prepara four glass of C60/SA/toluene solution. Then ablate them at different time. Using TEM,we observed different structures in different solution. Comparaing the four different solution, we discover that the solution which been ablated 30minutes is adapte to preparaing C60 LB film. The particle size of C60 in this solution is about several nanometers.Using the four different C60/SA/toluene solutions, we fabricate different C60 LB films. By analyzing, the film preparaed with the solution we ablated 30minutes is better than that preparaed with other three solution. The C60 cluster size is very small. The ablation time too long or too short will affect the charater of the film.Different surface topography and structure C60LB films were obtained by changing the ultrasonic time of the C60/SA/toluene mixed solutions. SEM images display that when the ultrasonic time is 30min, the film contain some little cluster, increasing the time to 90min, there are some bigger cluster and little rodlike structure. Along with the increasing of the ultrasonic time, some regular hollow prismatic structure appeared. The PL spectra of the film show that there are two PL spectral peaks at room temperature, as the changing of the temperature, a new peak appeared at about 768nm when decreasing the temperature to 120K.The conclusion above not only open a way for further systematic studies of C60 LB film, but also provide a novel application potential of fullerne LB film in photosensitive and luminescent material.
Keywords/Search Tags:C60 film, laser ablation, LB film, pressure-area isotherm(π-A curve) photoluminescence as the changing of temperature
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