金属卟啉LB膜的气敏特性研究

采用Langmuir-Blodgett (LB)技术,在不同膜压条件下制备了四苯基卟啉锌(ZnTPP)和四苯基卟啉铜(CuTPP)LB膜,分析了两种金属卟啉LB膜分别对吡啶、乙酸乙酯和四氢呋喃气体的紫外-可见光吸收光谱变化,并通过LB膜对紫外-可见光吸收光谱响应的变化,系统研究了两种金属卟啉LB膜的气敏特性,初步建立适合有机气体传感器敏感探测单元使用的材料体系.实验结果表明,在23mN/m的膜压条件下,金属卟啉的成膜效果最好,金属卟啉LB膜的紫外-可见吸收光谱响应最敏感,且发现分别通入3种不同气体后,CuTPP LB膜和ZnTPP LB膜的吸收光谱呈现不同的响应.所以CuTPP LB膜和ZnTPP LB膜相配合可作为色谱阵列单元用于识别吡啶、四氢呋喃和乙酸乙酯气体.     

新型四苯基卟啉衍生物及其锌(Ⅱ)配合物的合成与性质研究

以四苯基卟啉(TPP)为原料,经过硝化、还原、酰胺化等反应合成了一种新型四苯基卟啉衍生物及其锌(Ⅱ)配合物,通过FAB-MS、IR、1 H-NMR和元素分析等方法鉴定了目标产物的结构,并对其发光性质进行了研究。结果表明,四苯基卟啉衍生物及其锌(Ⅱ)配合物的紫外-可见光谱和荧光光谱均发生了明显红移。     

非金属卟啉自组装超薄膜的制备及其微观结构研究

应用自组装法，在银岛膜基底上成功制备了5，10，15，20-四-（羧酸苯基）卟啉-巯基吡啶交替超薄膜，并利用紫外可见和表面增强拉曼光谱探索膜的微观结构和成膜驱动力。实验发现，交替膜的形成是通过羧基与吡啶环上的N之间形成氢键来实现的，膜中的卟啉以J聚集体的形式存在，环平面与基片法线之间的夹角在27°左右。     

含偶氮基卟啉大环衍生物的制备及表征

文章介绍了有光、热敏感性能的四（4-重氮基苯基）卟啉及含有偶氮基团的卟啉衍生物的合成,用红外光谱,紫外光谱,飞行质谱等进行了结构表征,并对其光、热稳定性进行了研究。     

聚3,4-乙烯二氧噻吩/聚苯乙烯磺酸复合LB膜在OLED器件上的应用

采用Langmuir-Blodgett(LB)膜静电诱导沉积法制备聚3,4-乙烯二氧噻吩(PEDOT)高度有序导电聚合物复合薄膜,研究了薄膜的导电性能并进一步研究薄膜在改善器件性能方面的作用.并将其应用于有机电致发光二极管(OLED)器件的空穴缓冲层,将聚3,4-乙烯二氧噻吩/聚苯乙烯磺酸(PEDOT/PSS)复合LB沉积于纳米铟锡金属氧化物(ITO)电极上,制备了以复合LB膜为空穴缓冲层的OLED器件.发现复合LB膜改善了器件性能(启动电压降低,最大亮度增加),但进一步的研究表明LB膜器件在一定时间后出现性能劣化.I-V特性和X射线反射率(XRR)分析表明,薄膜的结构发生一定程度的改变是导致器件性能变差的可能原因.     

含氟聚酰亚胺特种单体的合成及表征

以2,2-双-[4-(4-硝基苯氧基)苯基]六氟丙烷(BNHFP)为原料,在钯/炭(Pd/C)、水合肼的作用下,还原得到了2,2-双-[4-(4-氨基苯氧基)苯基]六氟丙烷(BAHFP)单体。利用元素分析方法傅立叶转换红外光谱(FTIR)、核磁共振(NMR)和液相色谱等对所获得的聚酰亚胺(PI)单体BAHFP进行分析表征。然后,将BAHFP分别与均苯四甲酸二酐(PMDA)、氧撑二苯酐(ODPA)、苯酮四甲酸二酐(BTDA)和双酚A二酐(BPADA)进行聚合,得到了高特性粘度(≥0.8dl/g)的聚酰胺酸溶液,并可进一步热亚胺化成PI薄膜。     

四苯基卟啉夹层石墨烯复合物的光电子特性研究

以四苯基卟啉和石墨烯为原料,用溶剂-非溶剂共沉淀法制备得到四苯基卟啉夹层石墨烯复合物,通过扫描电镜（SEM）、透射电镜（TEM）、荧光光谱和电化学循环伏安对所得复合物进行表征。分析结果表明,共沉淀过程使得四苯基卟啉成功包裹了石墨烯,它们之间存在电子转移,且四苯基卟啉在654nm和717nm处的荧光淬灭;四苯基卟啉-石墨烯复合物是一个很好的电子给体-受体体系,在新型显示器、光伏电池等方面有潜在的应用价值。     

修饰LB膜法制备聚3,4-乙烯二氧噻吩薄膜的光电性能

采用修饰LB膜法以二十烷酸(AA)LB膜为模板,通过3,4-乙烯二氧噻吩(EDOT)单体在LB膜亲水基团间聚合,制备了AA/PEDOT复合LB膜。UV-Vis、FT-IR和XPS分析表明EDOT在多层膜中有效聚合,生成了PEDOT导电聚合物;XRR和SIMS分析表明薄膜具有较好的层状有序结构,进一步研究发现EDOT在AA多层膜中的聚合破坏了原有LB膜的有序性,这可能与聚合过程对层状结构产生的破坏作用有关;采用四探针仪及半导体测试仪研究了薄膜导电性能,发现AA/PEDOT多层膜的电导率随处理时间的变化产生突变,这与多层膜中导电通道的"渝渗"有关,在有效导电网络连通后电导率发生了突变。测试结果还表明AA/PEDOT膜导电性明显优于PEDOT旋涂膜和ODA-SA/PEDOT-PSS复合膜,这是由于原位制备的PEDOT共轭度较高,且薄膜具有很好的层状有序结构。     

一种新型可溶喹吖啶酮衍生物LB膜的制备及其光谱特性

采用表面压-分子面积(π一A)等温曲线和紫外-可见吸收谱的方法研究了一种新型喹吖啶酮衍生物材料LB膜的制备及其光谱特性．实验表明,这种新型喹吖啶酮衍生物能够在水面上形成稳定的单分子膜,它与花生酸(AA)混合后不仅可以形成很好的单分子膜,而且可以较好地转移到固体基片上制备成LB膜多层膜．这种新型喹吖啶酮衍生物LB膜的紫外-可见吸收谱的吸收峰位较稀溶液发生了红移,这是由极性溶剂分子与其相互作用的结果．它在溶液和LB膜中都是以单体的形式存在．     

硒化锌量子点二维阵列的LB方法制备与表征

以去铁铁蛋白作为生物模板合成了硒化锌量子点,采用Langmuir-Blodgett技术在硅基质表面制备1:4的EA/SMA的LB薄膜并将硒化锌核铁蛋白吸附组装到EA/SMA薄膜上形成二维阵列。用紫外-可见吸收光谱(UV-Vis)、荧光光谱(PL)、傅里叶转换红外光谱(FTIR)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)进行表征,结果表明成功制备得到了硒化锌量子点核铁蛋白单分子层二维阵列。这种排列在固体表面的有序微观尺寸的纳米结构由于其独特的光学和生物学特性在生物传感、药物和诊断等领域具有潜在的应用前景。     

Characterization of a novel 1,3-bis(p-iminobenzoic acid)indane Langmuir-Blodgett film for organic vapor sensing

In the present paper we report about the Langmuir-Blodgett thin film characterization and organic vapor sensing properties of a novel 1,3-bis(p-iminobenzoic acid)indane (IBI) containing polar carboxylic acid groups. LB film properties of IBI material is characterized by UV-visible spectroscopy, atomic force microscopy, and quartz crystal microbalance. Our results show that high-quality and uniform LB films can be prepared with the transfer ratio of over 0.95. Organic vapor sensing properties are studied using quartz crystal microbalance measurement system. IBI film is found to be significantly more sensitive to benzene and the response of LB sample is fast, large, and reversible. The sensitivity of detection of toluene, ethyl alcohol, and isopropyl alcohol is much smaller than that of benzene. This newly synthesized IBI is a suitable molecule for the fabrication of an LB film and can be regarded as a promising sensing material in the development of a room temperature gas sensor for benzene vapor applications.     

A study of Langmuir-Blodgett thin film for organic vapor detection

In this work, arachidic acid was deposited onto a quartz crystal using a standard Langmuir-Blodgett (LB) thin film deposition procedure. Quartz Crystal Microbalance (QCM) technique was used to monitor the reproducibility of the LB film monolayer and was employed to study the organic vapor sensing properties of chloroform, toluene, benzene, ethyl alcohol and isopropyl alcohol. QCM results show that arachidic acid monolayer was successfully organised and deposited from the water surface onto a quartz crystal substrate. This LB film is found to be highly sensitive and selective to chloroform vapor than other vapors. The response of the sample against chloroform is fast, large and reversible.     

Chemical vapor phase polymerization deposition of layer-ordered conducting polymer nanostructure for hole injection layer

Layer-ordered and ultrathin films of conducting polymer poly(3,4-ethylene dioxythiophene) (PEDOT) was prepared through a chemical vapor phase polymerization method. The chemical polymerization of 3, 4-ethylenedioxythiophene monomer was initiated in as-prepared oxidant LB films,and PEDOT nanofilms with layer-ordered structure was constructed. UV-Vis absorption spectrum and Fourier transform infrared spectroscopy was used to confirm an interface polymerization of PEDOT in as-prepared LB films. The results of X-ray diffraction and secondary ion mass spectrometry revealed that conductive PEDOT ultrathin layers were well located at different planes of LB films. The film deposition surface pressure and chemical polymerization time of PEDOT monomer in as-prepared LB films showed distinct influence on surface morphology and conductive performance of the polymerized PEDOT LB films. This layer-ordered conducting polymer ultrathin films was deposited on ITO surface as hole injection layer for organic light-emitting diodes, and the luminescence performance of devices was improved as well.     

Langmuir-Blodgett films of Cu(II)-tetrakis (3,3-dimethylbutoxycarbonyl) phthalocyanine: a spectrophotometric and TEM analysis of their structure and morphology

Langmuir-Blodgett (LB) films of copper(II)-tetrakis (3,3-dimethylbutoxycarbonyl) phthalocyanine [Cu(dmbc)Pc] have been prepared from toluene solutions; multilayers (up to 80 layers) were deposited onto hydrophobic quartz substrates. The refractive index n and extinction coefficient κ at normal incidence have been determined from both transmission and reflection measurements carried out in the 400–800 nm spectral range. The optical absorption spectrum as a function of the incident photon energy was also registered in order to determine the optical transition type in Cu(dmbc)Pc LB films by using a band model approach. Linearly polarised light absorbance measurements were performed at room temperature in the same spectral range. The average orientation of the phthalocyanine molecular rings in the LB film, with respect to the normal to the substrate and the dipping direction, has been evaluated. We have found that such orientation differs from that determined for LB films deposited from ethyl acetate solutions.

Structural and morphological analysis were also carried out by transmission electron microscopy techniques. Small ordered domains in a low range order matrix were observed by high resolution images. The structure of the material in the substrate plane has been determined by electron diffraction performed on single ordered domains.     

Preparation and properties of multilayer poly(3,4-ethylenedioxythiophene) Langmuir-Blodgett film

Multilayer ultrathin film of poly(3,4-ethylene dioxythiophene) (PEDOT) was fabricated using a modified Langmuir-Blodgett (LB) method. The chemical polymerization of PEDOT occurred in the multilayer nanometer space of an as-prepared LB film by exposing the film to 3,4-ethylene dioxythiophene vapor. UV-Vis-near infrared absorption spectrum and Fourier-transform infrared spectrum techniques were applied to confirm the formation of the PEDOT ultrathin film. The results of atomic force microscopy investigation for the PEDOT LB film showed that the film surface consisted of small clusters having diameters ranging from 50 to 200 nm. X-ray photoelectron spectroscopy and secondary-ion mass spectrometry were employed to analyze the atomic composition of the PEDOT LB film and the location of the formed PEDOT. It was found that the atomic composition of the composite film was almost consistent with the theoretical value, and the PEDOT clusters were well located in different planes of the multilayer structure. The PEDOT LB film exhibited higher conductivity than conventional films and better doping/dedoping characteristics of conductivity. The sensitivity of the PEDOT LB film to NH₃ and HCl gases was also discussed.     

Molecular film technology for biosensors

Two different molecular film technologies have been developed for fabricating biosensors. Firstly, bovine serum albumin spread on the air-water interface was cross-linked and transferred onto the glass surface, on which various molecular assemblies were formed by the bioaffinity technique. Secondly, a protein monolayer was adsorbed from an aqueous phase on the potential-controlled electrode surface, which was followed by electrochemical polymerization and deposition of pyrrole between the protein molecules to make the adsorbed protein film conductive.

A unique optical biosensor for taste has been fabricated by depositing fluorophore-containing Langmuir-Blodgett (LB) films on the glass surface. Each layer of the LB films exhibits its characteristic fluorescence peak which is quenched or enhanced in contact with taste substances. The sensor consisted of three different LB films containing pyrene and anthracene and deposited on a glass plate. Novel performance was demonstrated with the response of the sensor to glutamate and nucleotide umami substances.     

C_(60)/花生酸混合LB膜Ⅲ.LB膜的酸、碱稳定性

LB膜的环境稳定性是它们实际应用中常见的问题。实验发现盐酸蒸汽和氨蒸汽对C60 /AA混合LB膜的周期结构都有影响 ,使衍射峰的强度逐步减弱和等同周期有所减小。酸碱处理甚至会在C60 /AA混合LB膜中造成C60 微晶的形成。     

Block copolymer assisted self-assembly of nanoparticles into Langmuir–Blodgett films: Effect of polymer concentration

We propose to use the self-assembly ability of a block copolymer to obtain CdSe quantum dots (QDs) structures of different morphology. The methodology proposed consist in transferring mixed Langmuir monolayers of QDs and the polymer poly (styrene-co-maleic anhydride) partial 2 buthoxy ethyl ester cumene terminated, PS-MA-BEE onto mica by the Langmuir–Blodgett (LB) methodology. The morphology of the LB films was analyzed by AFM and TEM measurements. Our results show that it is possible to modulate the self-assembly process by modifying the composition of the mixed Langmuir monolayer precursor of the LB film. The different morphologies are interpreted according to two different dewetting mechanisms, growth of holes and spinodal-like dewetting. The growth of holes dewetting process is driven by gravitatory effects and was observed for LB films obtained by transferring Langmuir monolayer of the smallest elasticity values in which the polymer is in brush conformation. The spinodal dewetting mechanism prevailed when the Langmuir monolayer presents the highest elasticity values.     

Anisotropic behaviour of the glass transition temperature in thin films of Langmuir-Blodgett deposited side chain polymers

Langmuir-Blodgett (LB) films of side chain polyamic acids were formed, deposited onto optical waveguides and imidized via heating to the corresponding polyimides on the optical waveguides. The LB film formation of the side chain polyamic acids, the imidization reaction and the glass transition behaviour of the polyimide thin films were investigated. Polarisation dependent waveguide mode spectroscopy was applied therefore. It was found that the glass transition temperature (Tg) of bulk and LB thin film samples of these polymers are identical and only depend on the spacer length between the side chain and backbone, not on film thickness. Our investigation shows that in the case of the ultrathin film geometry, the glass transition temperature exhibits an anisotropic behaviour. We find the classical kink in the temperature scan (a change in slope of the free volume vs. temperature plot) due to the thermal expansion change at Tg, in p-polarisation only, which is perpendicular to the main chain orientation. In the s-polarisation measurements (parallel to the main chains) no kink was found, only an offset in the vicinity of Tg. We attribute the anisotropic thermal behaviour to a transition, the freezing of segmental motion, in the side chains only.