Synthesis and characterization of of a-cyclodextrins with thiolated 4-arm PEG using a
毕业论文外文翻译-壳聚糖-茶多酚纳米颗粒的合成和性质及细胞毒性的研究
毕业论文外文翻译-壳聚糖-茶多酚纳米颗粒的合成和性质及细胞毒性的研究Synthesis and Characterization of Chitosan-Tea Polyphenol Nanoparticles and Their Cytotoxicity StudyAbstractIn this study, chitosan-tea polyphenol nanoparticles were synthesized using a simple and green method. The physical and chemical properties of the nanoparticles were characterized by various techniques including dynamic light scattering, Fourier transform infrared spectroscopy, and transmission electron microscopy. The cytotoxicity of the nanoparticles was evaluated using MTT assay and cell morphological observation. The results showed that the synthesized nanoparticles had a diameter of 183.6 nm, a positive surface charge of 27.54 mV, and a polydispersity index of 0.22. The nanoparticles exhibited good biocompatibility with cells and low cytotoxicity, indicating their potential application in drug delivery.Keywords: chitosan, tea polyphenol, nanoparticles, cytotoxicity, drug deliveryIntroductionNanoparticles have been extensively studied in the field of drug delivery due to their unique properties such as high surface area, high reactivity, and enhanced permeation and retention effect. Among various materials, chitosan has attracted great attention as a drug delivery carrier due to its biocompatibility, biodegradability, and low toxicity (1). However, chitosan nanoparticles often suffer from low stability and poor solubility, which limit their application in drug delivery. To overcome these limitations, various methods have been developed to improve the stability and solubility of chitosan nanoparticles, such as crosslinking, coating, and blending with other materials (2).Tea polyphenols are natural plant extracts with various biological activities such as antioxidation, anticancer, and anti-inflammatory effects (3). Therefore, tea polyphenols have been widely used as functional food ingredients and nutraceuticals. In addition, tea polyphenols have also been investigated as potential anticancer agents due to their ability to induce apoptosis and inhibit cell proliferation (4). However, tea polyphenols suffer from low bioavailability and poor stability, which limit their therapeutic efficacy (5).To improve the stability and solubility of chitosan nanoparticles and enhance the therapeutic efficacy of tea polyphenols, we synthesized chitosan-tea polyphenol nanoparticles using a simple and green method. The physical and chemical properties of the nanoparticles were characterized, and the cytotoxicity of the nanoparticles was evaluated.Materials and MethodsMaterialsChitosan (degree of deacetylation > 85%, molecular weight 300,000-400,000 g/mol) was purchased from Sigma-Aldrich (USA). Tea polyphenols were extracted from green tea leaves and purified using ethanol precipitation according to a previous method (6). Dulbecco's modified eagle medium (DMEM), fetal bovine serum (FBS), and penicillin/streptomycin solution were obtained from Gibco (USA). 3-(4,5-Dimethylthiazol-2-yl)-2,5-diphenyltetrazolium bromide (MTT) and dimethyl sulfoxide (DMSO) were purchased from Sigma-Aldrich (USA). All reagents were of analytical grade and used without further purification.Synthesis of Chitosan-Tea Polyphenol NanoparticlesChitosan-tea polyphenol nanoparticles were prepared using a simple and green method. Briefly, chitosan (50 mg) was dissolved in 5 ml of acetic acid (1%, v/v), and tea polyphenol (5 mg) was dissolved in 5 ml of distilled water. The tea polyphenol solution was added dropwise into the chitosan solution under magnetic stirring at room temperature. The mixture was stirred for another 30 min to obtain a homogeneous solution. The solution was then added dropwise to 20 ml of 0.1 M sodium hydroxide solution under magnetic stirring to induce nanoparticle formation. The mixture was stirred for 60 min and then centrifuged at 10,000 rpm for 10 min to remove unreacted materials. The nanoparticles were washed three times with distilled water and freeze-dried for further use.Characterization of Chitosan-Tea Polyphenol NanoparticlesThe physical and chemical properties of chitosan-tea polyphenol nanoparticles were characterized by various techniques. The nanoparticle size and zeta potential were measured using a dynamic light scattering instrument (Malvern, UK). The particle morphology was observed using a transmission electron microscope (TEM, JEOL, Japan) after negative staining with uranyl acetate. The chemical structure of the nanoparticles was analyzed by Fourier transform infrared spectroscopy (FTIR, PerkinElmer, USA) using KBr pellets.Cytotoxicity StudyThe cytotoxicity of chitosan-tea polyphenol nanoparticles was evaluated using MTT assay and cell morphological observation. Human gastric cancer cells (SGC-7901) were seeded in a 96-well plate at a density of 5 × 103 cells per well in DMEM supplemented with 10% FBS and 1% penicillin/streptomycin solution. After 24 h, the cells were treated with different concentrations of chitosan-tea polyphenol nanoparticles (0, 12.5, 25, 50, 100, and 200 μg/ml) for 24 h. Then, the MTT solution (5 mg/ml) was added to each well and incubated for another 4 h. The supernatant was discarded, and DMSO was added to dissolve the formazan crystals. The absorbance was measured at 490 nm using a microplate reader (BioTek, USA). Cell viability was calculated as a percentage of the control group.For cell morphological observation, the cells were treated with chitosan-tea polyphenol nanoparticles (50 μg/ml) for 24 h and then observed under an inverted microscope (Olympus, Japan).Results and DiscussionsCharacterization of Chitosan-Tea Polyphenol NanoparticlesChitosan-tea polyphenol nanoparticles were synthesized using a simple and green method, and the physical and chemical properties of the nanoparticles were characterized by various techniques. As shown in Figure 1A and B, the nanoparticles had a diameter of 183.6 nm and a positive surface charge of 27.54 mV, indicating good stability and low aggregation. The nanoparticles exhibited a narrow size distribution with a polydispersity index of 0.22, indicating good homogeneity. The TEM image of the nanoparticles showed a spherical shape with a smooth surface, and the size observed by TEM was consistent with the DLS measurement (Figure 1C). FTIR spectroscopy was used to investigate the chemical structure of the nanoparticles. The characteristic absorption peaks of chitosan at 1658 cm-1 (amide I) and 1569 cm-1 (amide II) were observed in the spectrum of chitosan-tea polyphenol nanoparticles, indicating the successful formation of nanoparticles (Figure 1D).Cytotoxicity StudyThe cytotoxicity of chitosan-tea polyphenol nanoparticles was evaluated using MTT assay and cell morphological observation. As shown in Figure 2A, the cell viability of SGC-7901 cells treated with chitosan-tea polyphenol nanoparticles wasabove 90% at concentrations up to 200 μg/ml, indicating good biocompatibility with cells and low cytotoxicity. The morphological observation of cells treated with chitosan-tea polyphenol nanoparticles (50 μg/ml) showed no obvious changes compared with the control group (Figure 2B).ConclusionIn this study, we successfully synthesized chitosan-tea polyphenol nanoparticles using a simple and green method. The nanoparticles had a diameter of 183.6 nm, a positive surface charge of 27.54 mV, and a polydispersity index of 0.22, indicating good stability and low aggregation. The nanoparticles exhibited good biocompatibility with cells and low cytotoxicity, indicating their potential application in drug delivery. Further studies are needed to investigate the in vivo efficacy and safety of these nanoparticles.Figure 1 Characterization of chitosan-tea polyphenol nanoparticles. (A) Size distribution of nanoparticles measured by dynamic light scattering; (B) Zeta potential of nanoparticles; (C) Transmission electron microscopy image of nanoparticles; (D) Fourier transform infrared spectroscopy spectra of chitosan and chitosan-tea polyphenol nanoparticles.Figure 2 Cytotoxicity evaluation of chitosan-tea polyphenol nanoparticles. (A) MTT assay of SGC-7901 cells treated with different concentrations of nanoparticles (n = 3, *p < 0.05 compared with control); (B) Morphological observation of SGC-7901 cells treated with chitosan-tea polyphenol nanoparticles (50 μg/ml) and control group.AcknowledgmentsThis work was supported by the National Natural Science Foundation of China (No. 81673508).References1. Qi L, Xu Z, Jiang X, Hu C, Zou X, Preparation and antibacterial activity of chitosan nanoparticles. Carbohydr Res. 2004;339:2693-2700.2. Chen M-C, Mi F-L, Liao Z-X, Hsiao C-W, Sonaje K, Chung M-F, et al., Recent advances in chitosan-based nanoparticles for oral delivery of macromolecules.Adv Drug Deliv Rev. 2013;65:865-879.3. Wang D, Wang H, Guo Y, Ning W, Katirai F, Zhou Q, et al., Antioxidant properties and neuroprotective capacity of naturally occurring polyphenols in Parkinson's disease.Antioxidants (Basel). 2019;8:420.4. Siddiqui IA, Adhami VM, Ahmad N, Mukhtar H, Nanochemoprevention: sustained release of bioactive food components for cancer prevention.Nutr Cancer. 2010;62:883-890.5. Floegel A, Kim D-O, Chung S-J, Koo SI, Chun O-K, Comparison ofABTS/DPPH assays to measure antioxidant capacity in popular antioxidant-rich US foods.J Food Compos Anal. 2011;24:1043-1048.6. Zhang L, Yang X, Lv Y, Wang P, Gao Y, Hu K, et al., Optimizing the ultrasonic-assisted extraction of tea polyphenols from green tea using response surface methodology.J Food Sci. 2012;77:C1205-C1210.。
Synthesis and characterization of novel systems fo
专利内容由知识产权出版社提供
专利名称:Synthesis and characterization of novel systems for guidance and vectorization of molecules of therapeutic interest towards target cells
发明人:Pascal Dumy,Marie-Christine Favrot,Didier Boturyn,Jean-Luc Coll
申请号:US10528320 申请日:20030919 公开号:US07531622B2 公开日:20090512
摘要:A method for preparing a grafted homodetic cyclopeptide forming a framework that defines a grafted upper face and grafted lower face, including synthesizing a linear peptide from modified or unmodified amino acids, some of which carry orthogonal protective groups; intramolecular cyclizing the resulting protetuting some or all of orthogonal protective groups with a protected precursor; and grafting at least one molecule of interest onto one and/or the other face of the framework via an oxime bond.
DiI (细胞膜红色荧光探针)说明书
DiI (细胞膜红色荧光探针)产品编号 产品名称包装 C1036DiI (细胞膜红色荧光探针)10mg产品简介:DiI 即DiIC 18(3),全称为1,1'-dioctadecyl-3,3,3',3'-tetramethylindocarbocyanine perchlorate ,是最常用的细胞膜荧光探针之一,呈现橙红色荧光。
DiI 是一种亲脂性膜染料,进入细胞膜后可以侧向扩散逐渐使整个细胞的细胞膜被染色。
DiI 在进入细胞膜之前荧光非常弱,仅当进入到细胞膜后才可以被激发出很强的荧光。
DiI 被激发后可以发出橙红色的荧光,DiI 和磷酯双层膜结合后的激发光谱和发射光谱参考下图。
其中,最大激发波长为549nm ,最大发射波长为565nm 。
DiI 的分子式为C 59H 97ClN 2O 4,分子量为933.88,CAS number 为41085-99-8。
DiI 可以溶解于无水乙醇、DMSO 和DMF ,其中在DMSO 中的溶解度大于10mg/ml 。
发现较难溶解时可以适当加热,并用超声处理以促进溶解。
DiI 被广泛用于正向或逆向的,活的或固定的神经等细胞或组织的示踪剂或长期示踪剂(long-term tracer)。
DiI 通常不会影响细胞的生存力(viability)。
被DiI 标记的神经细胞在体外培养的条件下可以存活长达4周,在体内可以长达一年。
DiI 在经过固定的神经元细胞膜上的迁移速率为0.2-0.6mm/day ,在活的神经元细胞膜上的的迁移速率为6mm/day 。
DiI 除了最简单的细胞膜荧光标记外,还可以用于检测细胞的融合和粘附,检测发育或移植过程中细胞迁移,通过FRAP(Fluorescence Recovery After Photobleaching)检测脂在细胞膜上的扩散,检测细胞毒性和标记脂蛋白等。
用于细胞膜荧光标记时,DiI 的常用浓度为1-25µM ,最常用的浓度为5-10µM 。
Synthesis and characterization of low cost magnetorheological (MR) fluids
SYNTHESIS AND CHARACTERIZATION OF LOW COSTMAGNETORHEOLOGICAL (MR) FLUIDSVK Sukhwani and H Hiraniv_sukhwani@iitb.ac.in , hirani@iitb.ac.inDepartment of Mechanical Engineering, Indian Institute of Technology BombayMumbai-40007, INDIAABSTRACTMagnetorheological fluids have great potential for engineering applications due to their variable rheological behavior. These fluids find applications in dampers, brakes, shock absorbers, and engine mounts [1].However their relatively high cost (approximately US$600 per liter) limits their wide usage. Most commonly used magnetic material “Carbonyl iron” cost more than 90% of the MR fluid cost [2]. Therefore for commercial viability of these fluids there is need of alternative economical magnetic material. In the present work synthesis of MR fluid has been attempted with objective to produce low cost MR fluid with high sedimentation stability and greater yield stress. In order to reduce the cost, economical electrolytic Iron powder (US$ 10 per Kg) has been used. Iron powder of relatively larger size (300 Mesh) has been ball milled to reduce their size to few microns (1 to 10 microns). Three different compositions have been prepared and compared for MR effect produced and stability. All have same base fluid (Synthetic oil) and same magnetic phase i.e. Iron particles but they have different additives. First preparation involves organic additives Polydimethylsiloxane (PDMS) and Stearic acid. Other two preparations involve use of two environmental friendly low-priced green additives guar gum (US$ 2 per Kg) and xanthan gum (US$ 12 per Kg) respectively.Magnetic properties of Iron particles have been measured by Vibrating Sample Magnetometer (VSM). Morphology of Iron particles and additives guar gum and xanthan gum has been examined by Scanning Electron Microscopy (SEM) and Particles Size Distribution (PSD) has been determined using Particle size analyzer. Microscopic images of particles, M-H plots and stability of synthesized MR fluids have been reported. The prepared low cost MR fluids showed promising performance and can be effectively used for engineering applications demanding controllability in operations Keywords: Smart fluids, MR fluid, Magnetorheology, Particle distribution, Guar gum, Xanthan gum, PDMS, Low cost.1.INTRODUCTIONMagnetorheological (MR) fluids are known for their ability to change their rheological behavior by several orders of magnitude within milliseconds under the influence of magnetic field and therefore have been regarded as controllable fluids for engineering applications. Typically these fluids are non colloidal suspensions of micron sized magnetic particles (generally Iron particles) in nonmagnetic carrier medium (mineral oil, synthetic oil or water). Under the influence of magnetic field, these particles polarize and forms columnar structure parallel to the applied field, thus increases the apparent viscosity of the fluid which develops the yield stress in the structure. This viscosity change is rapid and completely reversible. Therefore MR fluid can be converted from a free flowing liquid to a plastic like solid by applying magnetic field and vice versa and can be used in different applications to bring dynamic change in performance measures like damping resistance as in MR-dampers, braking torque in MR-brakes and minimum film thickness in MR-bearings [3].Performance of any MR fluid in any application depends upon the magnetic properties of the solid phase, volume fraction, size and distribution of the magnetic particles, and viscosity of the carrier fluid etc.The synthesis of MR fluid involves many challenges. Two critical factors are the problem of gravitational sedimentation and agglomeration of particles and relatively high cost of MR fluids (approximately US$ 600 per liter). The large density difference between magnetic particles (i.e., ρ =7.86 g/cm3) and carrier fluid (i.e. ρ =1 g/cm3) is responsible for sedimentation problem. The problem of sedimentation has been mainly solved by three approaches, by adding Behavior and Mechanics of Multifunctional and Composite Materials 2007, edited by Marcelo J. DapinoProc. of SPIE Vol. 6526, 65262R, (2007) · 0277-786X/07/$18 · doi: 10.1117/12.720870surfactants, by adding nano particles or using nano magnetizable particles and by coating magnetizable particles with polymers .The addition of nano particles or use of nano magnetizable particles improves sedimentation stability effectively but at the same time it also reduces the MR effect produced by MR fluids. [4]High cost of MR fluid is mainly due to the high cost of magnetic material. Most commonly used magnetic material is Carbonyl iron obtained by thermal decomposition of Iron penta carbonyl .This material costs more than 90 % of the MR fluid cost [2, 5] Therefore for commercial viability of these fluids there is need of alternative economical magnetic material. In addition, an important functional requirement to produce more MR effect is the high dynamic yield stress. Use of alternative materials to reduce the cost has been reported in literature. Foister et al [5] in their patent have described the synthesis of low cost MR fluid using low cost water atomized Iron powder, multi component organoclay and multi component additive. Also the use of green additives like guar gum as thixotropic agent to solve the problem of sedimentation and agglomeration of MR fluids has been reported in literature. Chen et al [4] and Wu Wei Ping et al [6] successfully employed guar gum for improving sedimentation stability of MR fluids but they used the expensive carbonyl iron powder for synthesis of MR fluid. Similarly use of xanthan gum for achieving sedimentation stability of particles in MR fluid has been described by JD Carlson and JC Jones Guion in their patent. [7]As per authors knowledge no one has attempted use of both the economical Iron powder and additives like guar gum or xanthan gum in a single MR fluid composition. This has been attempted in the present work. In the present work synthesis of MR fluids have been carried out with objective to produce low cost MR fluid with high sedimentation stability and large yield stress. Low cost electrolytic Iron powder as magnetic material and variety of additives has been used for the present synthesis.2. SELECTION OF MAGNETIC PARTICLESThe magnetic particles for MR fluids should have high saturation magnetization and low coercivity. Carbonyl iron powder [8, 9, 10, 11], Nickel Zink ferrite [12], Iron oxide coated polymer composite particles [13], and Iron Cobalt alloy [14, 15] go well with these requirements. Saturation magnetization of Nickel Zink ferrite, Iron powder and Iron Cobalt alloy are 0.4T, 2.1 T and 2.43 T respectively [12,15] i.e. Iron Cobalt alloy has highest saturation magnetization but its density (8.1 g/ cm3) is greater than Iron therefore it aggravates gravitational settling. All the above mentioned magnetic materials are costly and therefore don’t suit the present synthesis of low cost MR fluid. Therefore for present synthesis Iron powder produced by electrolytic process has been chosen as this process yields the Iron of very high purity at very economical price (US$ 10 per Kg).The electrolytic Iron (EI) powder of relatively larger size 300 mesh (SD Fine-Chem, India) has been ball milled by suitable stainless steel grinding media in stainless steel pot to reduce the size to the order of few microns (1 -10 micron). This milled Iron powder was used for synthesis of all three MR fluids..3. SELECTION OF CARRIER FLUIDThe function of carrier or base fluid is to provide liquid phase in which magnetically active phase can be suspended. The carrier fluid should be non magnetic, nontoxic, non corrosive and non reactive. As most of lubricant with their additives packages suits these requirements, the commercial lubricants can be used for synthesis of MR fluid. In the present synthesis work, PAO (Poly Alfa Olefin) based high temperature synthetic oil with density 0.87 gram /cm3 and viscosity 20 cSt (0.01 Pa s) at 40°C has been selected. This oil can withstand operating temperature up to 180°C.4. SELECTION OF ADDITIVESAs discussed earlier, many additives have been attempted by researchers for synthesis of MR fluid. Generally thixotropic agents are added to prevent particle sedimentation. In addition, anti wear, anti corrosion, friction modifier and antioxidant agent are also added. Following are some important additives used in the synthesis of MR fluids for different purposes as reported in the literature:•To overcome sedimentation,o Fumed Silica [11], Lithium stearate, Aluminum distearate, Thiophosphorus, Thiocarbomate, Phosphorus, Guar gum [4], Organoclay[16] Poly vinyl pyrolidone [17], Poly vinyl butyl [18]•To overcome agglomeration,o Fumed silica [11], Fibrous carbon [19], Stearic acid [20], Sodium dodecyl sulphate [15], Viscoplastic media[21] o To increase abrasion wear resistance,o ZDDP (Zink dialkyl dithio phosphate ) [22-23]•To reduce oxidation,o ZDDP [23]• To reduce friction resistance.o Organomolybydnums (Moly) [22]Most of the above additives are not only expensive they are harmful to environment also. Therefore two environmental friendly additives, guar gum and xanthan gum have been chosen to prevent sedimentation of particles in the present synthesis. However for comparison purpose one organic polymer Polydimethylsiloxane (PDMS) has also been used as additives in one MR fluid composition.Guar gum is a high molecular weight hydro colloidal polysaccharide. It is extracted from guar bean (Cyamopsistetra gonoloba). It consist of linear chains of (1→4) linked ß-D mannose residue with a-D-galactopyranosyl units attached by (1.6) linkages. There is no polar group on the main chain of the guar gum, and most of the hydroxyl group is located outside. Furthermore, the side chain of the a-D-galactopyranosyl units does not hide the active alcoholic hydroxyl group; therefore it has a very large area of hydrogen bond. These characteristics make it useful as a thickening agent, suspension agent and stabilizing agent [4]. Its main application is found in food industry, where it is used as thickener, suspending agent and binder agent of free water in sauces, Ice cream, salad dressings etc.Similarly xanthan gum is a biosynthetic gum similar to natural gum. Xanthan gum is a long chain polysaccharide. It is prepared by fermentation of corn sugar with a microbe called Xanthomonas campestris. Xanthan gum has a special molecular structure. Its most important property is its very high viscosity at low-shear and relatively low viscosity at high shear. High viscosity at low shear provides stability to colloidal suspensions and therefore it is used as thickener and stabilizer for emulsions and suspensions.In the present work guar gum with approximate particle size 300 mesh (Premcem Gums India) and xanthan gum (Sienokem USA) have been used as thixotropic additives in two different preparations. In another preparation organic additive Polydimethylsiloxane (PDMS) with viscosity 100 cSt and Stearic acid are used. In addition an additive pack consists of anti wear, anti rust, anti corrosion, friction modifier and anti oxidant agent has also been used in all three preparations.5. CHARACTERIZATIONThe solid phase of MR fluid i.e. magnetic material was characterized before it is used in synthesis. Typically characterization includes analysis of particle size and its distribution, morphology and magnetic characterization. Additives guar gum and xanthan gum were also checked for their morphology.5.1 Particle size distribution analysisParticle size distribution analysis is very important for synthesis of MR fluid as particle size and size distribution influence the important properties i.e. Sedimentation stability, yield stress and magnetic properties of MR fluids [24]. Ota and Miyamoto [25] using two particle sizes calculated the static yield stress for a theoretical ER fluid and concluded that “ER Fluid consist of only same particle size gives the higher yield stress”. Lemaire et al [26] reported the influence of particle size on MR effect “It is better to have monodisperse sample in order to optimize the MR effect”. This indicates that narrow size distribution leads to more MR effect. But Wereley et al [13] in their study concluded that use of bidisperse particles in MR fluid increases their sedimentation stability. They also suggested a favorable tradeoff of proportion of particle sizes to increase the yield stress of MR fluid. Often particle size ranging 0.1 micron to 10 micronsis preferred [27]. Particle lesser than 0.1 micron will be subjected to random Brownian forces which destroy the chain like structure leading to decrease in the yield stress. On the other hand particles larger than 10 microns create the sedimentation problem. Kordonski et al [24] reported that particle size growth results in quadratic decrease of stability. Magnetic particles were analyzed using a particle size analyzer (GALAI computerized inspection system CIS-1, Particle size analyzer, Israel). Particles were dispersed in de ionized water with few drops of polyelectrolyte stabilizer to prevent the agglomeration of particles. Sodium Hexa Meta Phosphate was used as a medium to disperse the particles in this case. Sonication was also done to disperse the particles thoroughly. Fig-1 and Fig-2 show the particle size distribution of magnetic Electrolytic Iron (EI) particles before and after milling.Fig 1 Probability Volume density Graph for Electrolytic Iron powder before millingFig 2 Probability Volume density Graph for Electrolytic Iron powder after millingResults show that magnetic particle have broad size distribution (3.94 -77.50 microns ) with mean size 39 micron before milling and narrow size distribution (1.11-9.50microns) with mean size 4.27 micron after milling. This size range is recommended size range (1-10 micron) and therefore they are suitable for synthesis of MR fluids. These particles will have relatively lesser tendency to settle down.5.2 Morphology of magnetic particles and gum powdersThe morphology of the particles was studied by scanning electron microscopy (SEM facility S-3400 N, Hitachi Science Systems Japan). The powder sample was prepared by placing very small amount of powder on double sided carbon tape and pressing with the tip of spatula. The tape was then placed on brass stub. Gold plating was done on the samples to make the samples conducive. High vacuum was used and SEM was operated at 6-10 KV.Fig 3 SEM Image of Electrolytic Iron Particles before millingThe SEM image of the electrolytic Iron particles is shown in fig-3 .It shows the characteristic morphology of the particles .The electrolytic iron particles are of dendrite shape with a size distribution. Also they are in well dispersed state. SEM was also done for additives guar gum and xanthan gum. Fig-4 shows the SEM images (×500) obtained.(a) Guar gum (b) Xanthan gumFig 4 SEM Images of Guar gum and Xanthan gum powder5.3 Magnetic properties of particlesMagnetic properties of Iron particles were measured using vibrating sample magnetometer (VSM) technique. The VSM facility used for this purpose is Lakeshore VSM (Model 7410) interfaced with Lakeshore Cryotronics, Inc.VSM software.The Iron powder weight was measured with the accuracy of 0.0001 g by electronic balance (Precisa, Switzerland). The powder sample is pressed in to a small pellet. Small part of pellet (10-100 mg) is weighed and wrapped tightly in a butter paper /Teflon tape to avoid the movement of powder inside the sample holder. The magnetic field up to 20 K Oe was applied and operating frequency was 82 Hz.VSM was also done for costly carbonyl Iron (CI) powder to compare the magnetic properties of economical electrolytic Iron (EI) with costly carbonyl Iron (CI). Figure-5 shows M-H curves of the EI powder and CI powder obtained at room temperature (210C). The VSM results show that saturation magnetization of the electrolytic Iron powder is quite high (204.54emu/g) and approximately is of the same order of saturation magnetization of costly carbonyl Iron powder which is mostly used in synthesis of MR fluids. The saturation magnetization of carbonyl Iron (CI) powder has been found 212.08 emu/g. Slightly lower value of saturation magnetization of electrolytic iron powder in comparison to carbonyl Iron may be due to the fact that the electrolytic Iron used has 95.0 % purity while examined carbonyl Iron has 97-98 % purity. Moreover electrolytic Iron powder has also been milled to reduce the particle size which may also induce some impurities in the powder. Therefore more saturation magnetization will be obtained if EI powder having more purity is used.Coercivity was also determined from VSM data. Measured coercivity for electrolytic Iron is 26 O e and for carbonyl Iron it is 22 Oe. This shows that coercivity of electrolytic iron is only a little higher than the coercivity of carbonyl Iron. Moreover its value is still lower than 50 Oe and therefore can be considered as soft magnetic materials [28]Fig 5 M-H curves for Electrolytic Iron and Carbonyl Iron6. SYNTHESIS ROUTEIn present work three MR fluids are prepared using same base fluid (PAO based synthetic oil) and same magnetic phase i.e. electrolytic Iron (EI) powder but with different additives. These MR fluids are:MR Fluid-1: It has thixotropic agent Polydimethylsiloxane (PDMS) which is silicon based organic polymer and is known for its anti caking properties, Stearic acid as stabilizer additives and an additive package consist of anti wear, anti corrosion, friction modifier and anti oxidant agent.MR Fluid-2: It has green additive guar gum as thixotropic agent and above additive package. MR Fluid-3: It has additive xanthan gum as thixotropic agent and above additive package.6.1Coating of guar gum/xanthan gum on Iron particlesAdditives guar gum /xanthan gum were coated on the milled EI powder. Wu Wei Ping et al [6] reported that additive guar gum will be more effective when it is coated over the iron particles rather than co ball milling it with the Iron powder therefore first approach has been used in this work. For coating guar gum /xanthan gum over Iron particles the measured quantity of guar gum /xanthan gum was added to some quantity of water and mixed by mechanical stirrer for 30 minutes at 500 rpm. Iron powder was then added and mixture was agitated for 30 minutes at 1000 rpm. Ethanol was then added gradually to the mixture which leads to guar gum or xanthan gum forming a coating on the Iron powder. Precipitate was washed with acetone and filtered and dried to remove the water and then milled. These coated particles were used for synthesis. The weight percentage of guar gum /xanthan gum in the MR fluids is 3 %.6.2 Preparation of MR fluidsTo prepare MR fluid, first the appropriate amount of additive package consist of anti wear, anti rust, anti corrosion, friction modifier and anti oxidant agent was added to the measured quantity of base oil and mixed appropriately for 15 minutes by mechanical stirrer. The Iron particles (uncoated in case of MR fluid-1 and coated in case of MR fluid-2 and MR fluid-3) were then directly dispersed with specified volume fraction (0.36) in the above mixture. This mixture was homogenized by agitation of a mechanical stirrer at 1000 RPM for twenty-four hours to make MR fluid homogeneous. Appropriate amounts of PDMS with viscosity100 cSt and Stearic acid were also added in addition to the above additive package to the base oil for synthesis of MR fluid MRF-1. Fig-6 shows the flow chart for synthesis route of Magnetorheological fluid. The compositions of different MR fluids synthesized are given in table-1.Fig 6 Flow chart for Synthesis route of MR fluidsTable -1, Compositions of synthesized MR Fluids7. RESULTS & DISCUSSIONSIn present study three MR fluids have been synthesized using synthetic oil as base fluid, economical electrolytic Iron (with purity > 95.0 %) particles as magnetic phase and different additives. The prepared MR fluids were checked for their magnetic properties, expected MR effect and stability against sedimentation. Results of the study are as follows:7.1 Magnetic properties of uncoated particlesAs discussed earlier, magnetic properties of uncoated EI particles has been determined by VSM. Results indicate that saturation magnetization which is most important factor for producing MR effect i.e. yield stress developed , of low cost electrolytic iron powder (204.54 emu/g) is slightly lower (3.5%) than that of costly Carbonyl iron powder (212.084 emu/g). Similarly measured coercivity of EI powder (26 Oe) is slightly greater than Coercivity of CI powder (24 Oe).Therefore electrolytic Iron (EI) can be used for synthesis of MR fluid to reduce the cost of MR fluid significantly without significant reduction in MR effect.MRF-1 MRF-2 MRF-3 Ingredients Weight % Approx.Vol % Weight % Approx.Volume % Weight % Approx.Volume %Syntheticoil 16 64 15.5 64 15.5 64 Iron Powder81 36 81 36 81 36PDMS 2 ------ ------ ------ ------ ------ Stearicacid0.5 ------ ------ ------ ------ ------Guar gum ---- ------ 3.0 ------ ------ ------ Xanthangum ---- ------ ------ ------ 3.0 ------ Additive package0.5 ------ 0.5 ------ 0.5 ------7.2 Magnetic properties of coated particlesTo observe the effect of the additives coating on the magnetic properties of iron particles the magnetic properties of guar gum and xanthan gum coated particles were also checked by VSM. M-H curves for guar gum and xanthan gum coated particles are shown in figure-7. M-H curves show that saturation magnetization of guar gum coated and xanthan gum coated Iron particles are 198.52 emu/g and 198.14 emu/g respectively. Theses values are slightly lower (3%) than magnetic saturation of uncoated iron particles (204.54 emu/g). Measured Coercivity of these guar gum coated and xanthan gum coated Iron particles are 26 Oe and 28 Oe respectively which are almost same as that of coercivity of uncoated EI particles (26 Oe). This shows that coating of additives guar gum and xanthan gum on Iron particles has negligible effect on magnetic properties of Iron particles and therefore it can be concluded that MR effect produced by MR fluid will not reduce due to additive coating.Fig 7 M-H curves for Guar gum and Xanthan gum coated Electrolytic Iron7.3 MR effect expected (Yield stress developed)Magnetorheological (MR) effect produced by any MR fluid is the measure of its performance and is judged by maximum yield stress developed on application of magnetic field. For a MR fluid of known particle loading, particle size and known viscosity of base fluid the maximum yield stress depends upon the saturation magnetization of the magnetic material.The yield stress developed in MR fluid can be determined by performing magnetorheological measurement using a rheometer with an arrangement to produce magnetic field. Alternatively maximum yield stress developed in any MR fluid can be determined by measuring the saturation magnetization of the magnetic particles using VSM (Vibrating Sample Magnetometer). The relation between maximum obtainable yield stress and saturation magnetization of the magnetic particles has bee reported in the literature [29] as 20524()(3)()5yd s sat M τξφµ⎛⎞=⎜⎟⎝⎠(1)Where, yd τ is the yield stress, 0s M µ is saturation magnetization, φ is the particle volume fraction, 0µ is permeability of the free space and (3) 1.202ξ=(a constant)Table-2 shows the maximum yield stress expected to develop in three MR fluids obtained by using Eqn-1, based on their saturation magnetization values obtained by VSM .The values of yield stresses obtained for MRF-1, MRF-2 and MRF-3are quite high and are comparable to the value of yield stress (108 KPa) obtained for MR fluid using carbonyl Iron powder (2.09 T).Table 2- Expected Yield Stress for synthesized MR FluidsMR Fluid Saturation Magnetization Yield stress (KPa)MRF-1 204.54 emu/g (2.01 T) 99.59MRF-2 198.52 emu/g (1.96 T) 94.70MRF-3 198.14 emu/g (1.95 T) 93.737.4 Sedimentation stabilityPrepared MR fluids were put in graduated cylindrical flasks and observed over period of time for their sedimentation behavior i.e. settling of particles due to gravity. It was found that all three MR fluids remain in a well dispersed and stable state without significant settling of particles for quite long time. This is due to use of different thixotropic additives in MR fluids which reduces the sedimentation by forming weakly bonded structure in the fluid .These three dimensional structures have high apparent viscosity at low shear which prevents particle settling in the suspension. These structures collapse under shear leading to significant reduction in viscosity but reform again on removal of shear. Though all three MR fluids show very good stability against sedimentation but the MR fluids prepared by using additives guar gum and xanthan gum (MR fluid-2 and MR fluid-3) have better stability in comparison to MR fluid prepared using PDMS and Stearic acid (MR fluid-1). Sedimentation stability obtained are in the decreasing order from MRF-3 to MRF-1 i.e. lowest sedimentation tendency among three fluids was observed for MR fluid with xanthan gum and the highest sedimentation tendency was observed for MR fluid with PDMS. The result shows that the coating of guar gum and xanthan gum on iron particles gives better results in comparison to adding PDMS to the base fluid. This shows the utility of low-cost environmental friendly additives guar gum and xanthan gum in synthesis of MR fluids.8. CONCLUSIONS(01) Economical Iron powder produced by electrolytic process has very good magnetic properties, almost as good as costly carbonyl Iron powder which is most commonly used magnetic material for synthesis and therefore electrolytic Iron can be used as magnetic material to reduce the cost of MR fluid considerably without any significant reduction of MR effect produced.(02) Environmental friendly additives like guar gum and xanthan gum have been found more useful in comparison to organic polymer PDMS for preventing sedimentation of the particles in the MR suspension. Lowest sedimentation tendency has been observed for MR fluid with xanthan gum and the highest sedimentation tendency has been observed for MR fluid with PDMS.(03) The effect of coating of additives guar gum and xanthan gum on saturation magnetization and coercivity of Iron particles has almost been negligible. Therefore these additives can be used to improve the sedimentation stability without reducing MR effect produced by the MR fluids.(04) All three synthesized low cost MR fluids show very good stability against sedimentation and large yield stress therefore can be used in different commercial applications for achieving controllability in operation at relatively low cost..ACKNOWLEDGEMENTAuthors would like to thank their institute IIT Bombay for providing all the necessary facilities required for this workREFERENCES[1] Li W H, Du H and Guo NQ , “Finite Element Analysis and Simulation Evaluation of a Magnetorheological Valve”, Int. Journal of Advance Manufacturing Technology, Vol. 21, pp.438–445, 2003[2] Goncalves F D, Koo, J H, and Ahmadin M, “A review of the state of art in magnetorheological fluid technology – Part 1: MR Fluid and MR fluid models”, Shock and Vibration Digest, Vol.38, pp. 203-219, 2006,[3] Sukhwani VK and Hirani H, “Synthesis of a Magnetorheological lubricant” 5th International conference on Industrial tribology, ICIT-06, IISc Bangalore, Nov.30 –Dec. 02, 2006.[4] Fang Chen, Zhao Bin Yuan, Chen Le Sheng, Wu Qing, Liu Nan and Hu Ke Ao , “The effect of the green additive guar gum on the properties of magnetorheological fluid” , Smart materials structure, Vol.14, pp. N1-N5,2005.[5] Foister, Robet T, Iyanger, Vardarajan R, Yurgelvic and Sally M “Low cost MR fluid” US Patent No 6787058 , 2004[6] Wu Wei Ping , Zhao Bin Yuan , Wu Qing , Chen Le sheng and Hu Ke Ao, “The strengthening effect of guar gum on the yield stress of magnetorheological fluid” , Smart materials structure,Vol.15, pp. N94-N98,2006.[7] Carlson J D and Jones Guion J C, “Aqueous magnetorheological materials” U S Patent No 5670077, 1997.[8] Rabinow J, US Patent No 2575360, 1951.[9] Rabinow J, “The magnetic fluid clutch”, AIEE Trans, Vol. 67, pp.1308, 1948[10] Park J H, B yung Doo Chin and Ook Park , “Rheological properties and stabilization of magnetorheological fluid ina water in oil emulsion”, Journal of Colloid and Interface science, Vol. 240, pp 349-354 ,2001.[11] Lim S T, Cho M S, Jang I B and Choi H J, “Magnetrheological characterization of carbonyl iron suspension stabilized by fumed silica”, Journal of magnetism and magnetic materials, Vol. 282, pp .170-173, 2004.[12] Phule P P and Ginder J M “Synthesis and properties of novel magnetorheological fluids having improved stability and redispersibility”, 6th International conference on ER Fluids , MR suspensions and their applications, Yonezawa, Japan, World scientific, pp 445-453,1997.[13] Werely N M, Chaudhuri A , Yoo J H , John S, Kotha S, Suggs A , Radhakrishnan R, Love B J and Sudarshan T S, “Bidisperse magnetorheological fluids using Fe particles at nanometer and micron scale” ,Journal of Intelligent Materials, Systems and Structures, Vol. 17, pp. 393-401,2006.[14] Margida A J , Wiess K D and Carlson J D , “Magnetorheological materials based on Iron alloy particles”, Int. Journal of Modern Phys B, Vol.10, pp. 3335-3341,1996.[15] Phule P P and Jatkar A D, “Synthesis and processing magnetic iron cobalt alloy particles for high strength magnetorheological fluids”, 6th International conference on ER Fluids, MR suspensions and their applications, Yonezawa, Japan, World scientific, pp. 503-510,1997.[16] Foister R.T. Iyanger V R and Yugelevic S M, “Stabilization of magnetorheological fluid suspension using a mixture of organoclays”, US Patent No 6,592,772, 2003.[17] Phule P. “Magnetorheological fluid”, US Patent No 5,985,168, 1999[18] Jang I. B., Kim H B, Lee J Y ,You J L, Choi H J and John M S , “Role of organic coating on carbonyl Iron suspended particles in magnetorheological fluids”, Journal of Applied Phys, Vol.97, pp. 1-3, 2005。
Synthesis and characterization of Y_2O_2SEu~3+,Mg~2+,Ti~4+ nanorods via a solvothermal routine
JOURNAL OF RARE EARTHS,Vol.27,No.6,Dec.2009,p.895Fou ndation it em:Project s upported by the National Natural Science Foundation of China (20671042,50872045)and the Natural Science Foundations of Guang-dong Province (0520055,7005918)Cor respondin g aut hor:LI Wenyu (E-mail:liwenyu_jnn@;Tel.:+86-20-85221813)DOI 6S ()635Synthesis and char acter ization of Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods via a solvothermal routineLI Wenyu (李文宇),LIU Yingliang (刘应亮),AI Pengfei (艾鹏飞),CHEN Xiaobo (陈小博)(Department of Chemistry,Jinan University,Guangzhou 510632,Chi na)Received 24December 2008;revised 27April 2009Abstract:Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods were prepared by a solvothermal procedure.Rod-like Y(OH)3was firstly synthesized by hydro-thermal method to serve as the precursor.Y 2O 2S:Eu 3+,Mg 2+,Ti 4+powders were obtained by calcinating the precursor at CS 2atmosphere.The Y 2O 2S:Eu 3+,Mg 2+,Ti 4+phosphor with diameters of 30–50nm and lengths up to 200–400nm inherited the rod-like shape from the pre-cursor after calcined at CS 2atmosphere.The Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods showed hexagonal pure phase,good dispersion and exhibited bright red luminescence.After irradiation by 265or 325nm for 5min,the phosphor emitted red long-lasting phosphorescence,and the phos-phorescence could be seen with the naked eyes in the dark clearly for more than 1h after the irradiation source was removed.It was consid-ered that the long-lasting phosphorescence was due to the persistent energy transfer from the traps to the Ti 4+and Mg 2+ions to generate the red-emitting long-lasting phosphorescence.Keywords:yttrium oxysulfide;rod-like structure;nanomaterials;luminescence;rare earthsDuring the recent half-century there have been consider-able interests in the long-lasting phosphors because of their potential applications in safety indicators,fluorescent lamps,urgent illumination system,and cathode ray tubes,etc.[1–4]From the point of practical application,red is one of the three fundamental colors,and a red or orange afterglow phosphor is most suitable as illuminating light sources and appropriate for various displays.Therefore,red long-lasting phosphors with high luminescence and good chemical sta-bility are badly needed.Yttrium oxysulfide has been known for a long time as an excellent red phosphor host material.While doped with Eu,Mg,Ti,a red long-lasting phosphor with the afterglow time of above 3h has been synthesized [5].But until now,the progress on the systemic research of Y 2O 2S:Eu 3+,Mg 2+,Ti 4+is very slow and the luminescent mechanism is not well disclosed.The research of the long-lasting phosphors is mainly fo-cused on the bulk materials.However,one-dimensional rare-earth nanocrystals have recently attracted great attention because of their wide applications in fabrication of optical,electronic,biochemical and medical devices [6–9].If the rare earth compounds were fabricated in the form of one-dimen-sional nanostructures,they would have some new properties as a result of both their marked shape-specific and quan-tum-confinement effects.For luminescent materials,the phosphorescent properties are greatly affected by grain size,and many new properties can be obtained when the grain size reaches nanoscale.There are some methods for the prepara-tion of fine powders in nanosize,including sol-gel method,chemical precipitation,hydrothermal synthesis,and so on.The solvothermal method which exhibits some advantages of low processing temperature,high homogeneity and purity of the products has become a promising method for the prepara-tion of well-crystallized nanomaterials.Recently,some rare earth hydroxides with controlled morphology have been re-ported [10–13].As for lanthanide oxysulfides,only La 2O 2S,Gd 2O 2S and Eu 2O 2S are known as nanorods [14–16],La 2O 2Sand Nd 2O 2S as nanowires [17]and Y 2O 2S as nanotubes [11].There is still great difficulty in developing an effective route to synthesis high-quality (single-crystalline,well-shaped and phase-pure)nanocrystals.Until now the way to produce Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods hasrarely been reported yet.In this paper,we reported that,for the first time to our knowledge,Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods have been prepared by solvothermal method followed by a calcination process in CS 2atmosphere,and their photoluminescent properties were characterized at room temperature.Such Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods showed persistent red:10.101/1002-07210808-0896J OURNAL OF RARE EARTHS,Vol.27,No.6,Dec.2009emission after UV illumination,exhibiting potential in photoluminescent application.1Experimental Firstly,0.091mol Y 2O 3was dissolved in concentrated HNO 3.Then appropriate amount of ammonium aqueous so-lution was added dropwise.The co-precipitated powders were centrifugally separated,washed with distilled water and butanol three times,and then mixed with 40ml butonal.The solution was transferred to a teflon-lined stainless auto-clave and maintained at 260C for 5h and then cooled down to room temperature.The desired white hydroxide nanorods were filtered,washed with distilled water and ace-tone three times,and finally dried at 80C for 6h.In the second place,sulfur powder was put in a sealed graphite cru-cible,and heated to 800C for 4h.Then the dried precursor together with the mixture of 0.005mol Eu 2O 3,0.001mol Mg(OH)2.4MgCO 3.6H 2O,and 0.001mol TiO 2were placed into the graphite crucible and calcined at 1100C for 4h.Both the as-prepared Y(OH)3precursor and the final Y 2O 2S:Eu 3+,Mg 2+,Ti 4+phosphorescent products were characterized.The structures of the products were determined by powder X-ray diffraction (Bruker D8Focus).The morphologies of the powders were observed by employing scanning electron mi-croscopy (SEM,Philips XL-30),transmission electron mi-croscopy (TEM,Philips TECNAI 10)and high resolution transmission electron microscopy (HRTEM,Fei TECNAI G2F20).The photoluminescence spectra and intensity weremeasured on a fluorophotometer (Hitachi F-4500).All meas-urements were carried out at room temperature.2Results and discussion2.1Crystal structure of the product sFig.1shows pure phases of Y(OH)3precursor generated by a solvothermal process and Y 2O 2S after calcined in CS 2environment.It can be seen from the XRD patterns that both Y(OH)3and Y 2O 2S possess hexagonal structures.No impu-rity peaks are observed.As for Y 2O 2S,lattice parameters are as a=0.375nm,c=0.656nm by calculation,which are very close to the standard lattice parameters provided by the powder diffraction file,PDF #24-1424.Co-doped Eu 3+,Mg 2+and Ti 4+occupy the lattice sites in Y 2O 2S structure to form a uniform solid solution,with a nominal chemical composition of Y 2O 2S:Eu 3+,Mg 2+,Ti 4+.2.2Morphology of the Y(OH)3pr ecursorAs shown in Fig.2,Y(OH)3nanorods with uniform size and good distribution are obtained by the solvothermal method,showing the advantage of this method in preparing the particles with uniform size.A TEM micrograph is pre-sented in Fig.2(c),indicating obviously that the surface of the nanorods is smooth.2.3Morphology of the Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorods The calcination of the Y(OH)3in CS 2atmosphere leads toFig.1XRD patterns of the obtained Y(OH)3and Y 2O 2S:Eu 3+,Mg 2+,Ti 4+nanorodsFig.2Morphology of Y(OH)3precursor ()S M ;()()T M a E image b and c E micrographsLI Wenyu et al.,Synthesis and characterization of Y2O2S:Eu3+,Mg2+,Ti4+nanorods via a solvothermal routine897the formation of Y2O2S.As shown in Fig.3,all the crystals are of rod-like shape with the width diameters of30–50nm and the lengths ranging from200to400nm.For oxysulfide products,their1D linear morphology and diameters are nearly identical to those of the initial Y(OH)3nanorods,im-plying that the rod-like shape is kept after the high tempera-ture calcination.Although the exact mechanism is not clear now,it should be mentioned that the atmosphere in which the precursor is calcined plays an important part in keeping the rod-like shape.In our previous experiments[18],when the mixture was calcined in a flowing N2,air or H2S environ-ment,only Y2O2S:Eu3+,Mg2+,Ti4+particles were obtained. In this solid-gas reaction under such high temperature,we believe that the atmosphere is a key factor of a close mor-phological retention between the starting Y(OH)3and the final products.The detailed research of the mechanism is under way.2.4HRTEM examination of the Y2O2S:Eu3+,Mg2+,Ti4+nanorodsThe Y2O2S:Eu3+,Mg2+,Ti4+nanorods were also examined by using high resolution transmission electron microscopy. From Fig.4(a)we can see individual nanorods with the di-ameter of about50nm.A HRTEM micrograph of the nano-rod is shown in Fig.4(b),from which the single crystalline nature of the nanorod is confirmed.The spacing between the two adjacent lattice planes is0.365nm,which is just in good agreement with the interplanar crystal spacing of(101)of hexagonal phase Y2O2S:Eu3+,Mg2+,Ti4+.As is revealed in Fig.4(c),the corresponding selected area electron diffrac-tion pattern obtained is quite consistent with the target Y2O2S phase.These results further confirm that the final products are pure phased and single crystalline nanorods.2.5Luminescence property of the synthesized red phosphor For the sample calcined in CS2atmosphere under1100C, the excitation spectrum,shown in Fig.5(a),consists mainly of a wide band with two peaks at about260and325nm corresponding to Eu–O CTB(charge transfer band)and Eu–S CTB.While some weak and narrow peaks are attrib-uted to the f-f transition of Eu3+ions.The emission spectrum (Fig.5(b))excited by325nm indicates typical emission of Eu3+ion.The strong red-emission lines at615and625nm are due to transition from5D0to7F2level of Eu3+ion.Either Ti4+or Mg2+ion does not change the shape of excitation and emission spectra dramatically.2.6Afterglow decay curves of the phosphor sFrom the decay curve in Fig.6,it can be seen that doping both Mg2+and Ti4+ions can result in a long afterglow oftheFig.3Morphology of Y2O2S:Eu3+,Mg2+,Ti4+(a)SEM image;(b)and(c)TEMmicrographsFig.4TEM observation of Y2O2S:Eu3+,Mg2+,Ti4+nanorod(a)TEM micrograph for a single nanorod;(b)HRTEM image of the nanorod,showing single crystalline nature;()S Dc Corresponding AE pattern898J OURNAL OF RARE EARTHS,Vol.27,No.6,Dec.2009Fig.5Excitation and emission spectra of the Y2O2S:Eu3+,Mg2+,Ti4+phosphor(a)Excitation spectrum monitored at625nm;(b)Emission spectrum excited by325nmFig.6Afterglow decay curves of the phosphors(1)Y2O2S:Eu3+nanorods;(2)Y2O2S:Eu3+,Mg2+,Ti4+nanorods Y2O2S:Eu3+phosphor.The single Eu3+doped Y2O2S:Eu3+ phosphor shows very weak afterglow while red afterglow color can be clearly seen in the dark room for codoped Y2O2S:Eu3+,Mg2+,Ti4+.Moreover,the afterglow time of Y2O2S:Eu3+,Mg2+,Ti4+nanorods can last up to1h.We pro-pose that introduction of the Mg2+and Ti4+ions to the Y2O2S compound causes the formation of new electronic donating and accepting levels between the host lattice band gap.One of the two kinds of ions absorbs energy and ther-mally transfers the excited electrons to the other kind of ions which serves as trap centers.The trapping of excited elec-trons and thermally released processes results in the after-glow.3ConclusionsSingle crystalline Y2O2S:Eu3+,Mg2+,Ti4+nanorods were prepared by solvothermal method.Results showed that the final nanorods with uniform size and smooth surface inher-ited the rod-like shape from the precursor even after calcined S W with Mg2+and Ti4+ions,the phosphorescence lasted for1h in the light perception of the naked human eye.The intro-duction of Mg2+and Ti4+ions produced the complex hole and electron traps and resulted in long-lasting phenomenon. References:[1]Lin Y H,Tang Z L,Zhang Z T,Nan C W.Anomalous lumi-nescence in Sr4Al14O25:Eu,Dy phosphors.A pplied Physics Letter,2002,81:996.[2]Jia D,Wang X,Jia W,Yen W M.Persistent energy transfer inCaAl2O4:Tb3+,Ce3+.Journal of A pplied Physics,2003,93: 148.[3]Kamada M,Murakami J,Ohno N.Excitation spectra of a long-persistent phosphor SrAl2O4:Eu,Dy in vacuum ultraviolet region.Journal of Luminescence,2000,87-89:1042.[4]Wang X X,Zhang Z T,Tang Z L,Lin Y H.Characterizationand properties of a red and orange Y2O2S-based long afterglow phosphor.Materials Chemistry and Physics,2003, 80:1.[5]Wang Y H,Wang Z L.Characterization of Y2O2S:Eu3+,Mg2+,Ti4+long-lasting phosphor synthesized by flux method.Jour-nal ofRare Earths,2006,24(1):25.[6]Wang X,Zhang J,Peng Q,Li Y D.A general strategy fornanocrystal synthesis.Nature,2005,437:121.[7]Xia Y N,Yang P D.Chemistry and Physics of Nanowires.A dvanced Materials,2003,15:351.[8]Bockrath M,Liang W J,Bozovic D,Hafner J H,Lieber C M,Tinkham M,Park H K.Resonant electron scattering by de-fects in single-walled carbon nanotube.Science,2001,291: 283.[9]Hu J T,Odom T W,Lieber C M.Chemistry and physics inone dimension:synthesis and properties of nanowires and nanotubes.A ccounts of Chemical Research,1999,32:435. [10]Wang X,Li Y D.Synthesis and characterization of lanthanidehydroxide single-crystal nanowires.A ngew andte Chemie In-ternational Edition,2002,41:4790.[11]Wang X,Sun M,Yu D P.Rare earth compound nanotubes.at C2atmosphere at high temperatures.hile co-dopedLI Wenyu et al.,Synthesis and characterization of Y2O2S:Eu3+,Mg2+,Ti4+nanorods via a solvothermal routine899Advanced Materials,2003,15:1442.[12]Yang X F,Ning G L,Lin Y.Preparation of Eu(OH)3andEu2O3Nanorods through a Simple Method.Chemistry Letters, 2007,36:468.[13]Mao Y B,Huang J Y,Ostroumov R,Wang K L,Chang J P.Synthesis and luminescence properties of erbium-doped Y2O3 nanotubes.Journal of Physical Chemistry C,2008,112:2278.[14]Jiang Y,Wu Y,Xie Y,Qian Y T.Synthesis and characteriza-tion of nanocrystalline lanthanide oxysulfide via a La(OH)3 gel solvothermal route.Journal of the A merican Ceramic So-ciety,2000,83:2628.[15]Mao S P,Liu Q,Gu M,Mao D L,Chang C K.Long lastingphosphorescence of Gd2O2S:Eu,Ti,Mg nanorods via a hydro-thermal routine.Journal ofAlloys and Compounds,2008,468: 367.[16]Zhao F,Yuan M,Zhang W,Gao S.Monodisperse lanthanideoxysulfide nanocrystals.Journal of A merican Society,2006, 128:11758.[17]Huang Y Z,Chen L,Wu L M.Crystalline nanowires of Ln2O2S,Ln2O2S2,LnS2(Ln=La,Nd),and La2O2S:Eu3+conversions via the boron-sulfur method that preserve shape.Crystal Growth &Design,2008,8:739.[18]Li W Y,Liu Y L,Ai P F.Synthesis of nanocrystalline Y2O2S:Eu3+,Mg,Ti long-lasting phosphorescent materials by hydro-thermal-microwave method.Chinese Journal of Inorganic Chemistry,2008,24:772.。
Identification, isolation, synthesis and characterization of impurities
Aurobindo Pharma Ltd.Research Centre1,Bachupally,J.N.T.University2,Kukatpally,Hyderabad,India Identification,isolation,synthesis and characterization of impuritiesof quetiapine fumarateCh.Bharathi1,K.J.Prabahar1,Ch.S.Prasad1,M.Srinivasa Rao1,G.N.Trinadhachary1,V.K.Handa1,R.Dandala1, A.Naidu2Received May28,2007,accepted June18,2007Ramesh Dandala,Senior Vice-President,A.P.L.Research centre,313,Bachupally,Hyderabad500072,India rdandala@Pharmazie63:14–19(2008)doi:10.1691/ph.2008.7174In the process for the preparation of quetiapine fumarate(1),six unknown impurities and one known impurity(intermediate)were identified ranging from0.05–0.15%by reverse-phase HPLC.These impu-rities were isolated from crude samples using reverse-phase preparative HPLC.Based on the spectral data,the impurities were characterized as2-[4-dibenzo[b,f][1,4]thiazepine-11-yl-1-piperazinyl]1-2-etha-nol(impurity I,desethanol quetiapine),11-[(N-formyl)-1-piperazinyl]-dibenzo[b,f][1,4]thiazepine(impur-ity II,N-formyl piperazinyl thiazepine),2-(2-hydroxy ethoxy)ethyl-2-[2-[4-dibenzo[b,f][1,4]thiazepine-11-piperazinyl-1-carboxylate(impurity III,quetiapine carboxylate),11-[4-ethyl-1-piperazinyl]dibenzo[b,f][1,4] thiazepine(impurity IV,ethylpiperazinyl thiazepine),2-[2-(4-dibenzo[b,f][1,4]thiazepin-11-yl-1-piperazi-nyl)ethoxy]1-ethyl ethanol[impurity V,ethyl quetiapine),1,4-bis[dibenzo[b,f][1,4]thiazepine-11-yl]piper-azine[impurity VI,bis(dibenzo)piperazine].The known impurity was an intermediate,11-piperazinyl-dibenzo[b,f][1,4]thiazepine(piperazinyl thiazepine).The structures were established unambiguously by independent synthesis and co-injection in HPLC to confirm the retention times.To the best of our knowledge,these impurities have not been reported before.Structural elucidation of all impurities by spectral data(1H NMR,13C NMR,MS and IR),synthesis and formation of these impurities are dis-cussed in detail.1.IntroductionQuetiapine fumarate(1)is an antipsychotic drug belonging to the chemical class of dibenzothiazepine derivatives.It is used as a hemifumarate salt.Its IUPAC name is2-[2-(4-dibenzo[b,f][1,4]thiazepin-11-yl-1-piperazinyl)ethoxy etha-nol,(E)-2-butenedioate(2:1)salt.A literature survey re-vealed various methods for the synthesis of quetiapine(War-awa et al.2001).We synthesized the compound according to the Scheme(Warawa and Migler1989)with modifications to make it simpler and commercially viable.Its molecular formula is(C21H25N3O2S)2ÁC4H4O4and molecular weight is883amu as fumarate salt and383amu as base.HPLC methods(Saracino et al.2006;Mandrioli et al.2002) and a HPLC-electrospray ionization mass spectrometric method(Zhou et al.2004)were reported for the determi-nation of quetiapine in human plasma.During the preparation of1in the laboratory,six unknown impurities were detected in HPLC along with one known impurity.A comprehensive study was undertaken to iso-late,synthesize and characterize these impurities by spec-troscopic techniques.An impurity profile study is neces-sary for any final product to identify and characterize all the unknown impurities that are present in level of>0.1%. (ICH guideline,2005).The present study describes the isolation,synthesis and characterization of related impuri-ties of1.2.Investigations,results and discussion2.1.Detection and identificationQuetiapine fumarate was analysed by HPLC under the ana-lytical conditions described below.The chromatogram dis-played seven peaks at relative retention times compared to quetiapine at0.80,0.94,1.08,1.17,1.65,1.67and2.28. The LC-MS analysis showed six peaks having m/z values 339,323,427,323,411and504.They were isolated from crude samples of quetiapine by preparative HPLC.All the compounds were co-injected with quetiapine fumarate sam-ple in HPLC to confirm the retention times.HPLC chroma-togram of quetiapine fumarate spiked with all impurities is shown in the Fig.Synthesis and structural elucidation of these impurities are discussed in the following sections. Quetiapine fumarate was synthesized as shown in the Scheme,impurities I–VI were synthesized as described in the Experimental section and characterized.2.2.Characterization and origin of impurities2.2.1.Impurity IThe ESI mass spectrum of impurity I displayed the proto-nated molecular ion at m/z340.Therefore the molecular weight of this impurity was considered as339which was less by44amu than quetiapine.The odd molecular weightindicated the presence of odd number of nitrogens which in turn indicated the intactness of dibenzo[b ,f ][1,4]thia-zepine piperazinyl ring in this impurity structure.Pre-sence of broad signals at 3.70ppm (4H)and 4.34ppm (4H)in 1H NMR spectrum was attributed to piperazinyl ring.Two triplets were observed in impurity spectrum at 3.39ppm and 3.89ppm corresponding to 2ÂCH 2sig-nals instead of 4ÂCH 2groups present in the side chain of quetiapine.In 13C NMR two CH 2signals were ob-served at 61.1ppm and 73.1ppm instead of four CH 2signals.Based on the above spectral data observations,the structure of impurity I was characterized as 2-[4-di-benzo[b ,f ][1,4]thiazepine-11-yl-1-piperazinyl]l-2-ethanol (desethanol quetiapine).2-[2-Chloroethoxy]ethanol is a raw material for the pre-paration of quetiapine.2-Chloroethanol may be present as an impurity in this raw material.During the alkylation step in the preparation of quetiapine,alkylation of piper-azinyl thiazepine with the impurity,2-chloro ethanol leads to the formation of impurity I (desethanol quetiapine).2.2.2.Impurity IIESI mass spectrum of impurity II exhibited a protonated molecular ion peak at m/z 324,indicating the molecular weight as 323.The molecular weight of impurity II was 28amu more than that of the intermediate,4-piperazinyl di-benzo[b ,f ][1,4]thiazepine (2),m/z 295.MS fragmentation peaks were observed at m/z 296and 251.1H NMR spec-trum of this impurity showed signals similar to those of 2and in addition one new signal was observed at 8.13ppm integrated to one proton which was not exchangeable.This data suggested the attachment of a ––CHO group on piper-azine NH.Based on the spectral data,the structure of im-purity II was characterized as 11-[(N -formyl)-1-piperazi-nyl]-dibenzo[b ,f ][1,4]thiazepine (N -formyl piperazinylSNOHi.Piperazine /Toluene SNN N H i.2-(2-C hloroethoxy)ethanol ii.Na 2CO 3/NaI /NMP /TolueneSNNNO.2HClPiperazinyl thiazepine (2)SNNNOOHCOOHHOOC.Fumaric acid /Ethanol212345678910111213141516171819202122232223Quetiapine fumarate (1)SchemeSN NNOH34567891011121314151618192021Impurity I (Desethanol quetiapine)SN NNCHO56789101112131415161819202122Impurity II (N-Formyl piperazinyl thiazepine)221234N SNNOOOHO567891011121314151618192021Impurity III (Quetiapine carboxylate)3456789101112131415161718192021SN NNCH 3Impurity IV (N-Ethylpiperazinyl thiazepine)56789101112131415161718192021SNN NSN 9'10'11'12'13'14'15'16'18'19'20'21'Impurity VI (Bis (dibenzo)piperazine)N SNNOOCH 2CH 312345678910111213141516181920212223Impurity V (Ethyl quetiapine)thiazepine).This impurity arises when the alkylation of pi-perazinyl thiazepine with2-chloroethoxyethanol is carried out in N,N-dimethyl formamide.2.2.3.Impurity IIIESI mass spectrum of impurity III displayed a protonated molecular ion peak at m/z428,indicating the molecular weight of the compound as427which is44amu more than quetiapine.MS fragmentation peaks were observed at m/z,384,340and324.After thorough study of1H NMR and13C NMR spectra of this impurity,it was found to be as carboxy group attachment.It was observed from the1H NMR spectrum that there was no change in the number of protons compared to quetiapine and the signal correspond-ing to methylene protons attached to piperazine ring has shifted downfield from3.50ppm to4.14ppm.An addi-tional signal was observed at161.5ppm in the13C NMR spectrum and it was confirmed as quaternary carbon from DEPT experiment.From the above spectral data,the struc-ture of impurity III was characterized as2-(2-hydroxy ethoxy)ethyl-2-[2-[4-dibenzo[b,f][1,4]thiazepine-11-piper-azinyl-1-carboxylate(quetiapine carboxylate).This impurity arises when the alkylation of piperazinyl thiazepine is car-ried out in the presence of sodium carbonate(quetiapine carboxylate).2.2.4.Impurity IVESI mass spectrum of this impurity exhibited a protonated molecular ion peak at m/z324indicated the molecular weight of this impurity as323.Molecular weight of this impurity is28amu more than that of11-piperazinyl thi-azepine(intermediate).This odd molecular weight indicated the presence of odd number of nitrogen atoms which in turn indicated the intactness of piperazinyl thiazepine ring. MS fragmentation peaks were observed at296and253 amu.The signals corresponding to––O––CH2––CH2––OH group of quetiapine molecule were absent in impurity IV. Additionally,1H NMR spectrum of this impurity showed aFig.:LC-Chromatogram of Quetiapine fumarate samplespiked with impuritiesTable1:Comparative1H NMR assignments for quetiapine fumarate and its impuritiesPosition a Quetiapine fumarated(ppm),multiplicity Impurity-I d(ppm),multiplicityImpurity-II d(ppm),multiplicityImpurity-III d(ppm),multiplicityImpurity-IV d(ppm),multiplicityImpurity-V d(ppm),multiplicityImpurity-VI d(ppm),multiplicity1 3.43(t,2H)–––– 3.45(t,2H)–– 3.44(m,2H)––2 3.49(t,2H)–––– 3.47(t,2H)–– 3.52(m,2H)––3 3.55(t,2H) 3.82(t,2H)–– 3.61(t,2H) 1.29(t,3H) 3.56(t,2H)––4 2.52(t,2H) 3.27(t,2H)–– 4.14(t,2H) 3.18(t,2H) 3.40(t,2H)––5 6 7 82.50–2.54(brm,4H)and3.43–3.48(brm,4H)3.48and3.76(2brs,8H)3.42–3.73(m,8H)3.42and3.48(2brs,8H)3.20–3.75(brm,8H)3.20–3.75(brm,8H)3.03.65(brm,8H)9––––––––––––––10––––––––––––––117.55(m,1H)7.68(m,1H)7.55(d,1H)7.55(d,1H)7.68(m,1H)7.69(m,1H)7.56(m,2H)12 137.40(m,2H)7.60(m,2H)7.34–7.36(m,2H)7.44(m,2H)7.52–7.60(m,2H)7.52–7.60(m,2H)7.44–7.48(m,4H)147.45(m,1H)7.62(m,1H)7.42(d,1H)7.47(m,1H)7.62(m,1H)7.62(m,1H)7.46(m,2H) 15––––––––––––––16––––––––––––––177.37(dd,1H)7.54(dd,1H)7.40(dd,1H)7.38(dd,1H)7.54(dd,1H)7.54(dd,1H)7.38(dd,2H) 187.18(ddd,1H)7.35(brm,1H)7.23(ddd,1H)7.18(ddd,1H)7.35(brm,1H)7.35(brm,1H)7.20(ddd,2H)19 6.88(ddd,1H)7.15(ddd,1H) 6.95(ddd,1H) 6.91(ddd,1H)7.16(brd,1H)7.16(brd,1H) 6.90(ddd,2H)20 6.99(dd,1H)7.35(brm,1H)7.10(dd,1H)7.01(dd,1H)7.35(brm,1H)7.35(brm,1H)7.01(dd,2H) 21––––––––––––––22 6.62(s,2H)––8.13(s,1H)–––– 3.89(brm,2H)––23–––––––––– 1.08(t,3H)––s,singlet;d,doublet;dd,doublet of a doublet;ddd,doublet of a double doublet;m,multiplet;brs,broad singlet;brm,broad multiplet;q,quartet;t,tripleta Refor Scheme for numbering of quetiapine fumarateORIGINAL ARTICLEST a b l e 2:C o m p a r a t i v e13C N M R a n dDE P T a s s i g n m e n t s f o r q u e t i a p i n e f u m a r a t e a n d i t s i m p u r i t i e sP o s i t i o n a Q u e t i a p i n e f u m a r a t eI m p u r i t y -II m p u r i t y -I II m p u r i t y -I I II m p u r i t y -I VI m p u r i t y -VI m p u r i t y -V I13C d (p p m )DE P T13C d (p p m )DE P T13C d (p p m )DE P T13C d (p p m )DE P T13C d (p p m )DE P T13C d (p p m )DE P T13C d (p p m )DE P T161.1C H 2––––––––61.1C H 2––––66.4C H 2––––273.1C H 2––––––––73.1C H 2––––70.4C H 2––––368.7C H 258.6C H 2––––68.8C H 29.6C H 369.7C H 2––––457.8C H 256.1C H 2––––66.0C H 251.3C H 255.6C H 2––––567846.7a n d 53.44ÂC H 246.0,51.3a n d 51.64ÂC H 246.3,51.0a n d 51.64ÂC H 244.04ÂC H 246.4,50.0a n d 50.34ÂC H 245.751.4a n d 51.84ÂC H 245.5,47.6a n d 50.54ÂC H 29160.9––162.1––162.0––161.0––162.3––161.8––163.1a n d163.2––10139.6––136.5––140.0––139.6––140.6––140.3––137.8a n d137.9––11132.8C H 134.0C H134.0C H 132.8C H 134.1C H 133.5C H133.6a n d134.02ÂC H12129.8C H 130.2C H130.3C H 129.9C H 130.3C H 130.6C H130.2a n d130.44ÂC H13129.9C H 130.7C H 130.7C H 130.0C H 130.8C H131.3C H131.0C H14132.1C H 133.3C H 133.3C H 132.3C H 133.4C H 133.3C H 132.8C H 15128.1––128.0––––––128.1––127.7––127.5––129.0––16134.3––134.2––––––134.3––135.8––131.7––135.4––17132.9C H 135.1C H134.0C H 133.9C H 135.3C H 133.9C H134.7a n d134.92ÂC H18130.1C H 131.9C H 132.1C H130.2C H 132.0C H131.7C H 132.22ÂC H 19123.5C H 126.1C H126.4C H 123.8C H126.2C H126.6C H126.9a n d127.12ÂC H20126.0C H 129.5C H130.3C H 125.8C H129.7C H130.4C H128.9a n d129.22ÂC H21149.4––142.0––143.0––149.4––140.6––143.5––140.8––22135.2––––––162.3C H 156.0––––––65.5C H 2––––23167.4––––––––––––––––––9.6C H 3––––aR e f e r S c h e m e f o r n u m b e r i n g o f q u e t i a p i n e f u m a r a t e––CH3triplet at1.29ppm and––CH2quartet at3.18ppmcorresponding to ethyl group.This was supported by thepresence of methyl and methylene signals at9.0ppm and53.0ppm in13C NMR spectrum.Based on the above spectral data,the structure of impurity IV was character-ized as11-[4-ethyl-1-piperazinyl]dibenzo[b,f][1,4]thiaze-pine(N-ethyl-11-piperazinyl thiazepine).Ethanolic hydro-chloride was used to isolate piperazinyl thiazepine asdihydrochloride salt.Ethanolic hydrochloride may containethyl chloride which may alkylate piperazinyl thiazepineto yield this impurity(N-ethyl piperazinyl thiazepine).2.2.5.Impurity VESI mass spectrum of this impurity displayed a protonatedmolecular ion peak at m/z412indicating the molecularweight of this impurity as411which was28amu higher than that of quetiapine.Molecular weight suggested thatthe impurity was formed due to the substitution of ethylgroup on quetiapine.MS fragmentation peak was observedat324amu.In1H NMR spectrum of this impurity all the signals corresponding to quetiapine structure were presentand in addition methyl signal was observed as triplet at1.08ppm and methylene signal as quartet at3.53ppm.In 13C NMR spectrum the corresponding signals were ob-served at9.6ppm and65.5ppm.Based on the abovespectral data,the structure of impurity V was determinedas2-[2-(4-dibenzo[b,f][1,4]thiazepin-11-yl-1-piperazinyl)ethoxy]1-ethyl ethanol(ethyl quetiapine).2-[2-Chloro-ethoxy]ethoxy ethane may be an impurity present in theraw material,2-[2-chloroethoxy]ethanol.This impurityarises during alkylation of piperazinyl thiazepine with2-[2-chloroethoxy]ethoxy ethane(ethyl quetiapine).2.2.6.Impurity VIESI mass spectrum impurity VI exhibited a protonatedmolecular ion peak at m/z505,indicating the molecularweight of impurity as504.The even molecular weight suggested that the even number of nitrogens are present in this impurity.The molecular weight of this impurity was 209amu higher than that of piperazinyl thiazepine(quetia-pine intermediate,m/z,295).The difference molecular weight209amu corresponding to the dibenzo[b,f][1,4] thiazepine group.These mass values suggested that an-other dibenzo[b,f][1,4]thiazepine group was attached to piperazinyl NH of the quetiapine intermediate2.Sixteen aryl protons were present in the1H NMR spectrum,corre-sponding to two dibenzothiazepine groups and eight pro-tons were observed at3.4ppm,corresponding to one pi-perazine group.In13C NMR spectrum,the number of carbon signals in aryl region were doubled,supported the pre-sence of two dibenzo thiazepine groups.Based on the above spectral data,the structure of impurity VI was character-ized as1,4-bis[dibenzo[b,f][1,4]thiazepine-11-yl]piper-azine(bis(dibenzo)piperazine).During the preparation of piperazinyl thiazepine intermediate from11-chloro-diben-zo[b,f][1,4]thiazepine and piperazine,alkylation of both the nitrogen atoms of piperazine leads to the formation of bis(dibenzo)thiazepine.2.2.7.Spectroscopic dataThe1H and13C NMR chemical shift values of quetiapine fumarate and all impurities are presented in Tables1and2 FT-IR spectral data are given in Table3.3.Experimental3.1.Synthesis of the impuritiesThe investigated samples of quetiapine bulk drug and crude samples were synthesized in APL Research Centre(a unit of Aurobindo Pharma Ltd., Hyderabad,India).All impurities were isolated from crude samples by pre-parative HPLC.All the reagents used for analysis were procured from Merck(India)limited.3.1.1.Synthesis of impurity I,desethanol quetiapine hydrochloride11-Piperazinylthiazepine dihydrochloride(5g,0.0136mol)reacted with 2-chloro ethanol(1.2g,0.0149mol)in the presence of sodium carbonate (8.7g,0.0821mol),1-methyl-2-pyrrolidine(8ml,0.0771mol)and a cata-lytic amount of sodium iodide(0.05g,0.0003mol)in toluene(40ml)at 95–100 C for about24h and the reaction was monitored by TLC.Upon completion of reaction the reaction mass was washed with water (2Â25ml).The organic layer was concentrated completely under reduced pressure at50–55 C.The residue was dissolved in ethanol(40ml)and pH of the reaction mass was adjusted to$2.0with ethanolic HCl(10ml, $20%w/w).The precipitated product was filtered,washed with isopropy-lether(15ml)and dried at55–60 C to yield4.7g of desethanol quetia-pine.3.1.2.Synthesis of impurity II,N-formyl piperazinyl thiazepine11-Piperazinyl thiazepine dihydrochloride(10g,0.027mol),sodium carbo-nate(17.25g,0.163mol),sodium iodide(0.1g,0.0006mol)and2-chloro-Table3:FT-IR spectral data for quetiapine fumarate and its impuritiespound IR(KBr)absorption bands,(cmÀ1)1Quetiapine fumarate3320(m)OH stretch,3074,3014(w)aryl CH stretch,2946,2929,2898,2870(m)aliphatic CHstretch,1600,1573(s)aryl C¼C stretch and C¼N stretch,1414(s)CH2bend,795,768(m)aryl CHout-of-plane bend.2Impurity-I3060,3004(w)aryl CH stretch,2951,2884(m)aliphatic CH stretch,1622,1572(s)aryl C¼C stretchand C¼N stretch,1443(s)CH2bend,779,767(m)aryl CH out-of-plane bend.3Impurity-II3070(w)aryl CH stretch,2950,2890(m)aliphatic CH stretch,1620,1570(s)aryl C¼C stretch andC¼N stretch,1440(s)CH2bend,770,765(m)aryl CH out-of-plane bend.4Impurity-III3065(w)aryl CH stretch,2975,2886(m)aliphatic CH stretch,1620,1572(s)aryl C¼C stretch andC¼N stretch,1446(s)CH2bend,780,755(m)aryl CH out-of-plane bend.5Impurity-IV3063(w)aryl CH stretch,2979,2895(m)aliphatic CH stretch,1627,1573(s)aryl C¼C stretch andC¼N stretch,1430(s)CH2bend,782,767(m)aryl CH out-of-plane bend.6Impurity-V3070(w)aryl CH stretch,2923,2855(m)aliphatic CH stretch,.1621,1574(s)aryl C¼C stretch andC¼N stretch,1455(s)CH2bend,772,751(m)aryl CH out-of-plane bend.7Impurity-VI3052(m)aryl CH stretch,2989,2978,2953,2844(w)aliphatic CH stretch,1602,1575(s)aryl C¼Cstretch and C¼N stretch,1397(s)CH2bend,1245(s)C-N strech,1005,759,738(s)aryl CHout-of-plane bend.w–weak,s–strong,m–mediumethoxy ethanol(3.8g,0.03mol)were added to N,N-dimethylformamide (25ml)at room temperature.The reaction mass was heated to$100 C and stirred for8h while monitoring the process by HPLC.There after,the reaction mass was cooled to room temperature and poured into water (200ml).The product was extracted with ethyl acetate(2Â75ml)and the organic extract was washed with water(2Â80ml).The organic layer was concentrated completely under the reduced pressure at50–55 C.The resi-due contains$5%of this impurity which was isolated by preparative HPLC.3.1.3.Impurity III,quetiapine carboxylateImpurity III was isolated from mother liquors obtained during the prepara-tion of compound1.3.1.4.Synthesis of impurity IV,N-ethyl-11-piperazinyl thiazepine11-Piperazinyl thiazepine dihydrochloride(5g,0.0136mol)reacted with ethyl bromide(2.4g,0.020mol)in the presence of sodium carbonate (8.7g,0.0821mol)and dimethylformamide(15ml)at room temperature for2h and the reaction was monitored by TLC.The reaction mass was poured into water(200ml)and extracted with ethylacetate(2Â80ml). The organic layer was washed with water(2Â50ml)and concentrated completely under reduced pressure at50–55 C.The resulting residue was dissolved in ethanol(40ml)and treated with ethanolic HCl(10ml,20% w/w)at pH2.0.Isopropylether(20ml)was added dropwise to isolate the product.The product was stirred at room temperature for1h.The product was filtered,washed with isopropylether(5.0ml)and dried at55–60 C to yield4.2g of title compound.3.1.5.Impurity V,synthesis of ethyl quetiapineEthyl bromide(5.3g,0.0486mol)was added dropwise to a mixture of quetiapine fumarate(10g)and sodium hydroxide(2.9g,0.073mol)in dimethylformamide(50ml)at15–17 C.The reaction mass was stirred at15–20 C for8h and the reaction mass was monitored by HPLC until completion.Water(250ml)was added to the reaction mass and extracted with methylene chloride(2Â100ml).The organic layer was washed with water(2Â50ml)and concentrated under reduced pressure.The re-sidue was dissolved in ethanol(50ml)and ethanolic HCl(20ml,$20% w/w)was added dropwise.The precipitated product was stirred for1h. The product was filtered,washed with ethanol(5ml)and dried at40–45 C to yield6g of product containing$91%of the desired product by HPLC.3.1.6.Impurity VI,synthesis of bis(dibenzo)thiazepine11-Chloro-dibenzo[b,f][1,4]thiazepine(20.5g,0.0835mol)was added in small portions to a stirred mixture of piperazine(14.4g,0.167mol)in to-luene(160ml)at$50 C.The reaction was heated to$100 C,stirred for 4h and the reaction was monitored by HPLC until disappearance of start-ing material.The reaction mass was cooled to$20 C and filtered the salts.The toluene filtrate was washed with water(4Â100ml).The organic layer was concentrated completely under reduced pressure at50–55 C. The residue contains$12%of bis(dibenzo)thiazepine impurity which was isolated by preparative HPLC.3.2.High performance liquid chromatographyA Waters Alliance2695separation module equipped with2996photodiode array detector with Empower pro data handling system[Waters corpora-tion,MILFORD,MA01757,USA]was used.The analysis was carried out on YMC Pack-C8,150mm long,4.6mm i.d.,5m m particle diameter column.Mobile phase A was a mixture of phosphate buffer and acetonitrile in the ratio of90:10v/v,adjusted to pH6.7Æ0.05with dilute orthopho-sphoric acid solution(phosphate buffer was prepared by dissolving0.77g of disodium hydrogen orthophosphate(anhydrous)and0.57g of potassium dihydrogen orthophosphate in1000ml of water).Mobile phaseB was acetonitrile.UV detection was carried out at225nm and flow rate was kept at1.5ml/min.Column oven temperature was set at45C and data acquired for45min.Pump mode was gradient and the program was as follows,Time(min)/A(v/v):B(v/v);T0.01/80:20,T15.0/70:30,T25.0/60:40, T30.0/35:65,T35.0/30:70,T45.0/25:75,T50.0/80:20,T60.0/80:20.3.3.Preparative liquid chromatographyA Shimadzu LC-8A preparative liquid chromatograph equipped with SPD-10A VP,UV-Vis detector[Shimadzu corporation,Analytical Instruments Division,Kyoto,Japan]was used.Hyperprep HS C18(250mm longÂ21.2mm i.d.)preparative column packed with10m m particle size was em-ployed for isolation of impurities.The mobile phase consisted of(A) 0.1M ammonium acetate solution and(B)acetonitrile.Flow rate was set at20ml/min and UV detection was carried out at225nm.The gradient program was as follows,time(min)/A(v/v):B(v/v);T0.01/98:2,T20.0/90:10, T35.0/80:20,T50.0/70:30,T60.0/60:40,T75.0/50:50,T90.0/25:75.3.4.LC-MS/MS analysisLC-MS/MS analysis was carried out using a Perkin Elmer triple quadru-pole mass spectrometer(API2000,PE SCIEX)coupled with a Shimadzu HPLC equipped with SPD10AT VP UV-VIS detector and LC10AT VP pumps.Analyst software was used for data acquisition and data processing. The turbo ion spray voltage was maintained at5.5kv and temperature was set at375 C.The auxillary gas and curtain gas used was high pure nitro-gen.Zero air was used as nebulizer gas.LC-MS spectra were acquired from m/z100–1000in0.1amu steps with2.0s dwell time.The analysis was carried out using Hypersil BDS C18,150Â4.6mm column with5m m par-ticle dia.Mobile phase consisted of(A)0.01M ammonium acetate and(B) 1:1mixture of acetonitrile and methanol.UV detection was carried out at 225nm and flow rate was kept at1.5ml/min.Data acquisition time was 50min.The gradient program was as follows,Time(min)/A(v/v):B(v/v); T0.01/75:25,T5.0/75:25,T35.0/50:50,T40.0/15:85,T50.0/15:85.3.5.NMR SpectroscopyThe1H NMR,13C NMR(proton decoupled)and DEPT spectra were re-corded on Bruker300MHz spectrometer using DMSO-d6as solvent and tetramethylsilane(TMS)as internal standard.3.6.Mass spectrometryMass spectra were recorded on a Perkin Elmer PE SCIEX-API2000mass spectrometer equipped with a Turboionspray interface at375 C.Detection of ions was performed in electrospray ionisation,positive ion mode.3.7.FT-IR SpectroscopyFT-IR spectra were recorded as KBr pellet on a Perkin-Elmer instrument model––spectrum one.3.8.Isolation of impurities by preparative HPLCAll impurities were isolated by preparative HPLC from crude samples by using the conditions described above.Fractions collected were analyzed by analytical HPLC as per the conditions mentioned above.Fractions of >90%were pooled together,concentrated on Rotavapor to remove acetoni-trile.The concentrated fractions were passed through the preparative col-umn using water:acetonitrile(50:50)as mobile phase to remove the buf-fers used for isolation.Again the eluate was concentrated in a Rotavapor to remove acetonitrile.The aqueous solutions were lyophilized using freeze dryer(Virtis advantage2XL).Acknowledgements:The authors gratefully acknowledge the management of Aurobindo Pharma Limited,for allowing us to carry out the present work.The authors are also thankful to the colleagues of Analytical Re-search Department(ARD)and Chemical Research Department(CRD)for their co-operation.ReferencesICH Guideline Q3A(R2).Impurities in new drug substances,25October 2006.Mandrioli R,Fanali S,Ferranti A,Raggi MA(2002)HPLC analysis of the novel antipsychotic drug quetiapine in human plasma.J Pharm Biomed Anal30:969–977.Saracino MA,Mercolini L,Flotta G,Albers LJ,Merli R,Raggi MA (2006)Simulataneous determination of fluvoxamine isomers and que-tiapine in human plasma by means of HPLC.J Chromatogr843:227–233.Warawa EJ,Migler BM(1989)Novel dibenzothiazepine patent4,879,288.Warawa EJ,Migler BM,Ohnmacht CJ,Needles AL,Gatos GC,McLaren FM, Nelson CL,Kirkland KM(2001)Behavioral approach to nondyskinetic dopamine antagonists:identification of seroquel.J Med Chem44:372–389.Zhou Z,Li X,Li K,Xie Z,Cheng Z,Peng W,Wang F,Zhu R,Li H (2004)Simultaneous determination of clozapine,olanzapine,risperidone and quetiapine in plasma by HPLC-electrospray ionization mass spectro-metry.J Chromatogr802:257–262.。
有机化学实验报告模板
有机化学实验报告模板Title: Synthesis and Characterization of AspirinAbstract:Introduction:Materials and Methods:1. Salicylic acid (2.0 g)2. Acetic anhydride (5.0 mL)3. Concentrated sulfuric acid (2-3 drops)4. Ethanol (30 mL)5. Distilled water6. Melting point apparatus7. Thin-layer chromatography (TLC) plates8. TLC developing chamber9. UV lamp10. Infrared (IR) spectrometerThe procedure for synthesizing aspirin involved the following steps:1. Dissolving salicylic acid in acetic anhydride and addinga few drops of concentrated sulfuric acid.3. Allowing the reaction mixture to cool and then adding it to a mixture of ethanol and distilled water to precipitate the aspirin.4. Collecting the precipitated product by filtration and washing it with cold water.5. Drying the product and determining its melting point.The synthesized aspirin was characterized using thefollowing techniques:Results and Discussion:Conclusion:In conclusion, aspirin was successfully synthesized and characterized in this experiment. The physical properties of the synthesized aspirin, such as its melting point and appearance, were in agreement with the literature values. The TLC analysis indicated the purity of the synthesized aspirin, and the IR spectrum confirmed the presence of the functional groupsspecific to aspirin. Overall, this experiment provided valuable insight into the synthesis and characterization of aspirin using various techniques in organic chemistry.。
1997-JPC-(CdSe)ZnS Core-Shell Quantum Dots Synthesi_1`s and Characterization of a Size Series of
(CdSe)ZnS Core-Shell Quantum Dots:Synthesis and Characterization of a Size Series of Highly Luminescent NanocrystallitesB.O.Dabbousi,†J.Rodriguez-Viejo,‡F.V.Mikulec,†J.R.Heine,§H.Mattoussi,§R.Ober,⊥K.F.Jensen,‡,§and M.G.Bawendi*,†Departments of Chemistry,Chemical Engineering,and Materials Science and Engineering,Massachusetts Institute of Technology,77Massachusetts A V e.,Cambridge,Massachusetts02139,andLaboratoire de Physique de la Matie`re Condense´e,Colle`ge de France,11Place Marcellin Berthelot,75231Paris Cedex05,FranceRecei V ed:March27,1997;In Final Form:June26,1997XWe report a synthesis of highly luminescent(CdSe)ZnS composite quantum dots with CdSe cores ranging indiameter from23to55Å.The narrow photoluminescence(fwhm e40nm)from these composite dotsspans most of the visible spectrum from blue through red with quantum yields of30-50%at room temperature.We characterize these materials using a range of optical and structural techniques.Optical absorption andphotoluminescence spectroscopies probe the effect of ZnS passivation on the electronic structure of the dots.We use a combination of wavelength dispersive X-ray spectroscopy,X-ray photoelectron spectroscopy,smalland wide angle X-ray scattering,and transmission electron microscopy to analyze the composite dots anddetermine their chemical composition,average size,size distribution,shape,and internal ing asimple effective mass theory,we model the energy shift for the first excited state for(CdSe)ZnS and(CdSe)-CdS dots with varying shell thickness.Finally,we characterize the growth of ZnS on CdSe cores as locallyepitaxial and determine how the structure of the ZnS shell influences the photoluminescence properties.I.IntroductionSemiconductor nanocrystallites(quantum dots)whose radii are smaller than the bulk exciton Bohr radius constitute a class of materials intermediate between molecular and bulk forms of matter.1Quantum confinement of both the electron and hole in all three dimensions leads to an increase in the effective band gap of the material with decreasing crystallite size.Conse-quently,both the optical absorption and emission of quantum dots shift to the blue(higher energies)as the size of the dots gets smaller.Although nanocrystallites have not yet completed their evolution into bulk solids,structural studies indicate that they retain the bulk crystal structure and lattice parameter.2 Recent advances in the synthesis of highly monodisperse nanocrystallites3-5have paved the way for numerous spectro-scopic studies6-11assigning the quantum dot electronic states and mapping out their evolution as a function of size.Core-shell type composite quantum dots exhibit novel properties making them attractive from both an experimental and a practical point of view.12-19Overcoating nanocrystallites with higher band gap inorganic materials has been shown to improve the photoluminescence quantum yields by passivating surface nonradiative recombination sites.Particles passivated with inorganic shell structures are more robust than organically passivated dots and have greater tolerance to processing conditions necessary for incorporation into solid state structures. Some examples of core-shell quantum dot structures reported earlier include CdS on CdSe and CdSe on CdS,12ZnS grown on CdS,13ZnS on CdSe and the inverse structure,14CdS/HgS/ CdS quantum dot quantum wells,15ZnSe overcoated CdSe,16 and SiO2on Si.17,18Recently,Hines and Guyot-Sionnest reported making(CdSe)ZnS nanocrystallites whose room tem-perature fluorescence quantum yield was50%.19This paper describes the synthesis and characterization of a series of room-temperature high quantum yield(30%-50%) core-shell(CdSe)ZnS nanocrystallites with narrow band edge luminescence spanning most of the visible spectrum from470 to625nm.These particles are produced using a two-step synthesis that is a modification of the methods of Danek et al.16 and Hines et al.19ZnS overcoated dots are characterized spectroscopically and structurally using a variety of techniques. The optical absorption and photoluminescence spectra of the composite dots are measured,and the lowest energy optical transition is modeled using a simplified theoretical approach. Wavelength dispersive X-ray spectroscopy and X-ray photo-electron spectroscopy are used to determine the elemental and spatial composition of ZnS overcoated dots.Small-angle X-ray scattering in solution and in polymer films and high-resolution transmission electron microscopy measurements help to deter-mine the size,shape,and size distribution of the composite dots. Finally,the internal structure of the composite quantum dots and the lattice parameters of the core and shell are determined using wide-angle X-ray scattering.In addition to having higher efficiencies,ZnS overcoated particles are more robust than organically passivated dots and potentially more useful for optoelectronic device structures. Electroluminescent devices(LED’s)incorporating(CdSe)ZnS dots into heterostructure organic/semiconductor nanocrystallite light-emitting devices may show greater stability.20Thin films incorporating(CdSe)ZnS dots into a matrix of ZnS using electrospray organometallic chemical vapor deposition(ES-OMCVD)demonstrate more than2orders of magnitude improvement in the PL quantum yields(∼10%)relative to identical structures based on bare CdSe dots.21In addition,these structures exhibit cathodoluminescence21upon excitation with high-energy electrons and may potentially be useful in the*To whom correspondence should be addressed.†Department of Chemistry,MIT.‡Department of Chemical Engineering,MIT.§Department of Materials Science and Engineering,MIT.⊥Colle`ge de France.X Abstract published in Ad V ance ACS Abstracts,September1,1997.9463J.Phys.Chem.B1997,101,9463-9475S1089-5647(97)01091-2CCC:$14.00©1997American Chemical Societyproduction of alternating current thin film electroluminescent devices(ACTFELD).II.Experimental SectionMaterials.Trioctylphosphine oxide(TOPO,90%pure)and trioctylphosphine(TOP,95%pure)were obtained from Strem and Fluka,respectively.Dimethylcadmium(CdMe2)and di-ethylzinc(ZnEt2)were purchased from Alfa and Fluka,respec-tively,and both materials were filtered separately through a0.2µm filter in an inert atmosphere box.Trioctylphosphine selenide was prepared by dissolving0.1mol of Se shot in100mL of TOP,thus producing a1M solution of TOPSe.Hexamethyl-disilathiane((TMS)2S)was used as purchased from Aldrich. HPLC grade n-hexane,methanol,pyridine,and1-butanol were purchased from EM Sciences.Synthesis of Composite Quantum Dots.(CdSe)ZnS.Nearly monodisperse CdSe quantum dots ranging from23to55Åin diameter were synthesized via the pyrolysis of the organome-tallic precursors,dimethylcadmium and trioctylphosphine se-lenide,in a coordinating solvent,trioctylphosphine oxide (TOPO),as described previously.3The precursors were injected at temperatures ranging from340to360°C,and the initially formed small(d)23Å)dots were grown at temperatures between290and300°C.The dots were collected as powders using size-selective precipitation3with methanol and then redispersed in hexane.A flask containing5g of TOPO was heated to190°C under vacuum for several hours and then cooled to60°C after which 0.5mL of trioctylphosphine(TOP)was added.Roughly0.1-0.4µmol of CdSe dots dispersed in hexane was transferred into the reaction vessel via syringe,and the solvent was pumped off.Diethylzinc(ZnEt2)and hexamethyldisilathiane((TMS)2S) were used as the Zn and S precursors.The amounts of Zn and S precursors needed to grow a ZnS shell of desired thickness for each CdSe sample were determined as follows:First,the average radius of the CdSe dots was estimated from TEM or SAXS measurements.Next,the ratio of ZnS to CdSe necessary to form a shell of desired thickness was calculated based on the ratio of the shell volume to that of the core assuming a spherical core and shell and taking into account the bulk lattice parameters of CdSe and ZnS.For larger particles the ratio of Zn to Cd necessary to achieve the same thickness shell is less than for the smaller dots.The actual amount of ZnS that grows onto the CdSe cores was generally less than the amount added due to incomplete reaction of the precursors and to loss of some material on the walls of the flask during the addition. Equimolar amounts of the precursors were dissolved in2-4 mL of TOP inside an inert atmosphere glovebox.The precursor solution was loaded into a syringe and transferred to an addition funnel attached to the reaction flask.The reaction flask containing CdSe dots dispersed in TOPO and TOP was heated under an atmosphere of N2.The temperature at which the precursors were added ranged from140°C for23Ådiameter dots to220°C for55Ådiameter dots.22When the desired temperature was reached,the Zn and S precursors were added dropwise to the vigorously stirring reaction mixture over a period of5-10min.After the addition was complete,the mixture was cooled to 90°C and left stirring for several hours.A5mL aliquot of butanol was added to the mixture to prevent the TOPO from solidifying upon cooling to room temperature.The overcoated particles were stored in their growth solution to ensure that the surface of the dots remained passivated with TOPO.They were later recovered in powder form by precipitating with methanol and redispersed into a variety of solvents including hexane, chloroform,toluene,THF,and pyridine.(CdSe)CdS.Cadmium selenide nanocrystallites with diam-eters between33.5and35Åwere overcoated with CdS to varying thickness using the same basic procedure as that outlined for the ZnS overcoating.The CdS precursors used were Me2-Cd and(TMS)2S.The precursor solution was dripped into the reaction vessel containing the dots at a temperature of180°C and a rate of∼1mL/min.The solution became noticeably darker as the overcoat precursors were added.Absorption spectra taken just after addition of precursors showed a significant shift in the absorption peak to the red.To store these samples,it was necessary to add equal amounts of hexane and butanol since the butanol by itself appeared to flocculate the particles.Optical Characterization.UV-vis absorption spectra were acquired on an HP8452diode array spectrophotometer.Dilute solutions of dots in hexane were placed in1cm quartz cuvettes, and their absorption and corresponding fluorescence were measured.The photoluminescence spectra were taken on a SPEX Fluorolog-2spectrometer in front face collection mode. The room-temperature quantum yields were determined by comparing the integrated emission of the dots in solution to the emission of a solution of rhodamine590or rhodamine640 of identical optical density at the excitation wavelength. Wavelength Dispersive X-ray Spectroscopy.A JEOL SEM 733electron microprobe operated at15kV was used to determine the chemical composition of the composite quantum dots using wavelength dispersive X-ray(WDS)spectroscopy. One micrometer thick films of(CdSe)ZnS quantum dots were cast from concentrated pyridine solutions onto Si(100)wafers, and after the solvent had completely evaporated the films were coated with a thin layer of amorphous carbon to prevent charging.X-ray Photoelectron Spectroscopy.XPS was performed using a Physical Electronics5200C spectrometer equipped with a dual X-ray anode(Mg and Al)and a concentric hemispherical analyzer(CHA).Data were obtained with Mg K R radiation (1253.6eV)at300W(15keV,20mA).Survey scans were collected over the range0-1100eV with a179eV pass energy detection,corresponding to a resolution of2eV.Close-up scans were collected on the peaks of interest for the different elements with a71.5eV pass energy detection and a resolution of1eV.A base pressure of10-8Torr was maintained during the experiments.All samples were exchanged with pyridine and spin-cast onto Si substrates,forming a thin film several monolayers thick.Transmission Electron Microscopy.A Topcon EM002B transmission electron microscope(TEM)was operated at200 kV to obtain high-resolution images of individual quantum dots. An objective aperture was used to selectively image the(100), (002),and(101)wurtzite lattice planes.The samples were prepared by placing one drop of a dilute solution of dots in octane onto a copper grid supporting a thin film of amorphous carbon and then wicking off the remaining solvent after30s.A second thin layer of amorphous carbon was evaporated onto the samples in order to minimize charging and reduce damage to the particles caused by the electron beam.Small-Angle X-ray Scattering(SAXS)in Polymer Films. Small-angle X-ray scattering(SAXS)samples were prepared using either poly(vinyl butyral)(PVB)or a phosphine-func-tionalized diblock copolymer[methyltetracyclododecene]300-[norbornene-CH2O(CH2)5P(oct)2]20,abbreviated as(MTD300P20), as the matrix.23Approximately5mg of nanocrystallites of dispersed in1mL of toluene,added to0.5mL of a solution containing10wt%PVB in toluene,concentrated under vacuum to give a viscous solution,and then cast onto a silicon wafer. The procedure is the same for MTD300P20,except THF is used9464J.Phys.Chem.B,Vol.101,No.46,1997Dabbousi et al.as the solvent for both nanocrystallites and polymer.The resulting∼200µm thick film is clear to slightly opaque.X-ray diffraction spectra were collected on a Rigaku300Rotaflex diffractometer operating in the Bragg configuration using Cu K R radiation.The accelerating voltage was set at60kV with a300mA flux.Scatter and diffraction slits of1/6°and a0.3 mm collection slit were used.Small-Angle X-ray Scattering in Dilute Solutions.The X-ray source was a rotating copper anode operated at40kV and25mA.The apparent point source(electron beam irradiated area on the anode)was about10-2mm2.The beam was collimated onto a position sensitive detector,PSPE(ELPHYSE).A thin slit,placed before the filter,selects a beam with the dimensions of3×0.3mm2on the detector.The position sensitive linear detector has a useful length of50mm,placed at a distance D)370mm from the detector.The spatial resolution on the detector is200µm.This setup allows a continuous scan of scattering wavevectors between6×10-3 and0.40Å-1,with a resolution of about3×10-3Å-1.The samples used were quartz capillary tubes with about1 mm optical path,filled with the desired dispersion,and then flame-sealed after filling.The intensity from the reference,I ref, is collected first,and then the intensity from the sample,I s.The intensity used in the data analysis is the difference:I)I s-I ref.Wide-Angle X-ray Scattering(WAXS).The wide-angle X-ray powder diffraction patterns were measured on the same setup as the SAXS in polymer dispersions.The TOPO/TOP capped nanocrystals were precipitated with methanol and exchanged with pyridine.The samples were prepared by dropping a heavily concentrated solution of nanocrystals dispersed in pyridine onto silicon wafers.A slow evaporation of the pyridine leads to the formation of glassy thin films which were used for the diffraction experiments.III.Results and AnalysisA.Synthesis of Core-Shell Composite Quantum Dots. We use a two-step synthetic procedure similar to that of Danek et al.16and Hines et al.19to produce(CdSe)ZnS core-shell quantum dots.In the first step we synthesize nearly mono-disperse CdSe nanocrystallites ranging in size from23to55Åvia a high-temperature colloidal growth followed by size selective precipitation.3These dots are referred to as“bare”dots in the remainder of the text,although their outermost surface is passivated with organic TOPO/TOP capping groups. Next,we overcoat the CdSe particles in TOPO by adding the Zn and S precursors at intermediate temperatures.22The resulting composite particles are also passivated with TOPO/ TOP on their outermost surface.The temperature at which the dots are overcoated is very critical.At higher temperatures the CdSe seeds begin to grow via Ostwald ripening,and their size distribution deteriorates, leading to broader spectral line widths.Overcoating the particles at relatively low temperatures could lead to incomplete decom-position of the precursors or to reduced crystallinity of the ZnS shell.An ideal growth temperature is determined independently for each CdSe core size to ensure that the size distribution of the cores remains constant and that shells with a high degree of crystallinity are formed.22The concentration of the ZnS precursor solution and the rate at which it is added are also critical.Slow addition of the precursors at low concentrations ensures that most of the ZnS grows heterogeneously onto existing CdSe nuclei instead of undergoing homogeneous nucleation.This probably does not eliminate the formation of small ZnS particles completely so a final purification step in which the overcoated dots are subjected to size selective precipitation provides further assurance that mainly(CdSe)ZnS particles are present in the final powders.B.Optical Characterization.The synthesis presented above produces ZnS overcoated dots with a range of core and shell sizes.Figure1shows the absorption spectra of CdSe dots ranging from23to55Åin diameter before(dashed lines)and after(solid lines)overcoating with1-2monolayers of ZnS. The definition of a monolayer here is a shell of ZnS that measures3.1Å(the distance between consecutive planes along the[002]axis in bulk wurtzite ZnS)along the major axis of the prolate-shaped dots.We observe a small shift in the absorption spectra to the red(lower energies)after overcoating due to partial leakage of the exciton into the ZnS matrix.This red shift is more pronounced in smaller dots where the leakage of the exciton into the ZnS shell has a more dramatic effect on the confinement energies of the charge carriers.Figure2shows the room-temperature photoluminescence spectra(PL)of these Figure 1.Absorption spectra for bare(dashed lines)and1-2 monolayer ZnS overcoated(solid lines)CdSe dots with diameters measuring(a)23,(b)42,(c)48,and(d)55Å.The absorption spectra for the(CdSe)ZnS dots are broader and slightly red-shifted from their respective bare dot spectra.Figure2.Photoluminescence(PL)spectra for bare(dashed lines)and ZnS overcoated(solid lines)dots with the following core sizes:(a) 23,(b)42,(c)48,and(d)55Åin diameter.The PL spectra for the overcoated dots are much more intense owing to their higher quantum yields:(a)40,(b)50,(c)35,and(d)30.(CdSe)ZnS Core-Shell Quantum Dots J.Phys.Chem.B,Vol.101,No.46,19979465same samples before (dashed lines)and after (solid lines)overcoating with ZnS.The PL quantum yield increases from 5to 15%for bare dots to values ranging from 30to 50%for dots passivated with ZnS.In smaller CdSe dots the surface-to-volume ratio is very high,and the PL for TOPO capped dots is dominated by broad deep trap emission due to incomplete surface passivation.Overcoating with ZnS suppresses deep trap emission by passivating most of the vacancies and trap sites on the crystallite surface,resulting in PL which is dominated by band-edge recombination.Figure 3(color photograph)displays the wide spectral range of luminescence from (CdSe)ZnS composite quantum dots.The photograph shows six different samples of ZnS overcoated CdSe dots dispersed in dilute hexane solutions and placed in identical quartz cuvettes.The samples are irradiated with 365nm ultraviolet light from a UV lamp in order to observe lumines-cence from all the solutions at once.As the size of the CdSe core increases,the color of the luminescence shows a continuous progression from blue through green,yellow,orange,to red.In the smallest sizes of TOPO capped dots the color of the PL is normally dominated by broad deep trap emission and appears as faint white light.After overcoating the samples with ZnS the deep trap emission is nearly eliminated,giving rise to intense blue band-edge fluorescence.To understand the effect of ZnS passivation on the optical and structural properties of CdSe dots,we synthesized a large quantity of ∼40Ådiameter CdSe dots.We divided this sample into multiple fractions and added varying amounts of Zn and S precursors to each fraction at identical temperatures and addition times.The result was a series of samples with similar CdSe cores but with varying ZnS shell thickness.Figure 4shows the progression of the absorption spectrum for these samples with ZnS coverages of approximately 0(bare TOPO capped CdSe),0.65,1.3,2.6,and 5.3monolayers.(See beginning of this section for definition of number of monolayers.)The spectra reflect a constant area under the lowest energy 1S 3/2-1S e absorption peak (constant oscillator strength)for the samples with varying ZnS coverage.As the thickness of the ZnS shell increases,there is a shift in the 1S 3/2-1S e absorption to the red,reflecting an increased leakage of the exciton into the shell,as well as a broadening of the absorption peak,indicating a distribution of shell thickness.The left-hand side of Figure 4shows an increased absorption in the ultraviolet with increasing ZnS coverage as a result of direct absorption into the higher band gap ZnS shell.The evolution of the PL for the same ∼40Ådiameter dots with ZnS coverage is displayed in Figure 5.As the coverage of ZnS on the CdSe surface increases,we see a dramatic increase in the fluorescence quantum yield followed by a steadydeclineFigure 3.Color photograph demonstrating the wide spectral range of bright fluorescence from different size samples of (CdSe)ZnS.Their PL peaks occur at (going from left to right)470,480,520,560,594,and 620nm (quartz cuvettes courtesy of Spectrocell Inc.,photography by F.Frankel).Figure 4.Absorption spectra for a series of ZnS overcoated samples grown on identical 42Å(10%CdSe seed particles.The samples displayed have the following coverage:(a)bare TOPO capped,(b)0.65monolayers,(c)1.3monolayers,(d)2.6monolayers,and (e)5.3monolayers (see definition for monolayers in text).The right-hand side shows the long wavelength region of the absorption spectra showing the lowest energy optical transitions.The spectra demonstrate an increased red-shift with thicker ZnS shells as well as a broadening of the first peak as a result of increased polydispersity.The left-hand side highlights the ultraviolet region of the spectra showing an increased absorption at higher energies with increasing coverage due to direct absorption into the ZnS shell.9466J.Phys.Chem.B,Vol.101,No.46,1997Dabbousi et al.after∼1.3monolayers of ZnS.The spectra are red-shifted (slightly more than the shift in the absorption spectra)and showan increased broadening at higher coverage.The inset to Figure 5charts the evolution of the quantum yield for these dots as a function of the ZnS shell thickness.For this particular sample the quantum yield starts at15%for the bare TOPO capped CdSe dots and increases with the addition of ZnS,approaching a maximum value of50%at approximately∼1.3monolayer coverage.At higher coverage the quantum yield begins to decrease steadily until it reaches a value of30%at about∼5 monolayer coverage.In the following sections we explain the trends in PL quantum yield based on the structural characteriza-tion of ZnS overcoated samples.C.Structural Characterization.Wa V elength Dispersi V e X-ray Spectroscopy.We analyze the elemental composition of the ZnS overcoated samples using wavelength dispersive X-ray spectroscopy(WDS).This method provides a quantitative analysis of the elemental composition with an uncertainty of less than(5%.We focus on obtaining a Zn/Cd ratio for the ZnS overcoated samples of interest.Analysis of the series of samples with a∼40Ådiameter core and varying ZnS coverage gives the Zn/Cd ratios which appear in Table1.The WDS analysis confirms that the Zn-to-Cd ratio in the composite dots increases as more ZnS is added.We also use this technique to measure the Se/Cd ratio in the bare dots.We consistently measure a Se/Cd ratio of∼0.8-0.9/1,indicating Cd-rich nanoparticles.X-ray Photoelectron Spectroscopy.Multiple samples of ∼33and∼40Ådiameter CdSe quantum dots overcoated with variable amounts of ZnS were examined by XPS.Figure6shows the survey spectra of∼40Ådiameter bare dots and ofthe same sample overcoated with∼1.3monolayers of ZnS.Thepresence of C and O comes mainly from atmospheric contami-nation during the brief exposure of the samples to air(typicallyaround15min).The positions of both C and O lines correspondto standard values for adsorbed species,showing the absenceof significant charging.24As expected,we detect XPS linesfrom Zn and S in addition to the Cd and Se lines.Althoughthe samples were exchanged with pyridine before the XPSmeasurements,small amounts of phosphorus could be detectedon both the bare and ZnS overcoated CdSe dots,indicating thepresence of residual TOPO/TOP molecules bound to Cd or Znon the nanocrystal surfaces.25The relative concentrations ofCd and Se are calculated by dividing the area of the XPS linesby their respective sensitivity factors.24In the case of nano-crystals the sensitivity factor must be corrected by the integral∫0d e-z/λd z to account for the similarity between the size of the nanocrystals and the escape depths of the electrons.26Theintegral must be evaluated over a sphere to obtain the Se/Cdratios in CdSe dots.In the bare CdSe nanocrystals the Se/Cdratio was around0.87,corresponding to46%Se and54%Cd.This value agrees with the WDS results.We use the Auger parameter,defined as the difference inbinding energy between the photoelectron and Auger peaks,toidentify the nature of the bond in the different samples.24Thisdifference can be accurately determined because static chargecorrections cancel.The Auger parameter of Cd in the bare andTABLE1:Summary of the Results Obtained from WDS,TEM,SAXS,and WAXS Detailing the Zn/Cd Ratio,Average Size, Size Distribution,and Aspect Ratio for a Series of(CdSe)ZnS Samples with a∼40ÅDiameter CdSe Cores and Varying ZnS CoverageZnS coverage(TEM)measd TEM size measd averageaspect ratiocalcd size(SAXSin polymer)measd Zn/Cdratio(WDS)calcd Zn/Cd ratio(SAXS in polymer)calcd Zn/Cd ratio(WAXS)bare39Å(8.2% 1.1242Å(10%0.65monolayers43Å(11% 1.1646Å(13%0.460.580.71.3monolayers47Å(10% 1.1650Å(18% 1.50 1.32 1.42.6monolayers55Å(13% 1.233.60 2.9 5.3monolayers72Å(19% 1.23 6.80 6.8 Figure5.PL spectra for a series of ZnS overcoated dots with42(10%Ådiameter CdSe cores.The spectra are for(a)0,(b)0.65,(c)1.3,(d)2.6,and(e)5.3monolayers ZnS coverage.The position of themaximum in the PL spectrum shifts to the red,and the spectrumbroadens with increasing ZnS coverage.(inset)The PL quantum yieldis charted as a function of ZnS coverage.The PL intensity increaseswith the addition of ZnS reaching,50%at∼1.3monolayers,and then declines steadily at higher coverage.The line is simply a guide to the eye.Figure6.(A)Survey spectra of(a)∼40Ådiameter bare CdSe dots and(b)the same dots overcoated with ZnS showing the photoelectron and Auger transitions from the different elements present in the quantum dots.(B)Enlargement of the low-energy side of the survey spectra, emphasizing the transitions with low binding energy.(CdSe)ZnS Core-Shell Quantum Dots J.Phys.Chem.B,Vol.101,No.46,19979467overcoated samples is466.8(0.2eV and corresponds exactly to the expected value for bulk CdSe.In the case of ZnS the Auger parameter for Zn in the1.3and2.6monolayer ZnS samples is757.5eV,which is also very close to the expected value of758.0eV.The degree of passivation of the CdSe surface with ZnS is examined by exposing the nanocrystal surface to air for extended periods of time and studying the evolution of the Se peak. The oxidation of CdSe quantum dots leads to the formation of a selenium oxide peak at higher energies than the main Se peak.27Figure7shows the formation of a SeO2peak at59eV after an80h exposure to air in both the bare,TOPO capped, CdSe and0.65monolayer ZnS overcoated samples.These results indicate that in the0.65monolayer samples the ZnS shell does not completely surround the CdSe nanocrystals,and there are still Se sites at the surface that are susceptible to oxidation. In samples with an estimated coverage of∼1.3monolayers ZnS or more the oxide peak does not appear even after prolonged exposure to air,indicating that the CdSe surface is possibly protected by a continuous ZnS shell.After exposure to air for 16h,the bare CdSe nanocrystals display a selenium oxide peak which represents13%of the total Se signal,and the Se/Cd ratio decreases to0.77,corresponding to43%Se and57%Cd.The same sample after80h exposure to air had a ratio of Se/Cd of 0.37(28%Se and72%Cd),and the SeO2peak area was22% of the total Se signal.For a∼40Ådiameter sample,34%of the atoms are at the surface which means that in the sample measured most of the surface Se has been desorbed from the surface after80h.In the samples with more than 1.3 monolayers of ZnS coverage no change in the Se/Cd ratio was detected even after exposure to air for80h.Although no Cd-(O)peak appears after similar exposure to air,the Cd Auger parameter shifts from466.8eV for bare unoxidized CdSe to 467.5eV for particles exposed to air for80h.The Auger parameter for the1.3and2.6monolayer coverage samples remains the same even after prolonged exposure to air. Another method to probe the spatial location of the ZnS relative to the CdSe core is obtained by comparing the ratios of the XPS and Auger intensities of the Cd photoelectrons for bare and overcoated samples.14,28The depth dependence of the observed intensity for the Auger and XPS photoemitted electrons iswhere J0is the X-ray flux,N(z)i is the number of i atoms,σi is the absorption cross section for atoms i,Y i,n is the emission quantum yield of Auger or XPS for atoms i,F(KE)is the energy-dependent instrument response function,andλ(KE)is the energy-dependent escape depth.Taking the ratio of the intensities of the XPS and Auger lines from the same atom,Cd or Zn,it is possible to eliminate the X-ray flux,number of atoms, and absorption cross sections from the intensity equations for the Auger and the primary X-ray photoelectrons.The value of the intensity ratio I)i overcoated(Cd)/i bare(Cd),where i)i XPS-(Cd)/i Auger(Cd),is only a function of the relative escape depths of the electrons.Therefore,due to the smaller escape depths of the Cd Auger electrons in both ZnS(13.2Å)and CdSe(10Å)compared to the Cd XPS photoelectron(23.7Åin ZnS and 15Åin CdSe),the intensity I should increase with the amount of ZnS on the CdSe surface.Calculated values of1.28and 1.60for the0.65and2.6monolayer,respectively,confirm the growth of ZnS on the surface of the CdSe dots. Transmission Electron Microscopy.High-resolution TEM allows us to qualitatively probe the internal structure of the composite quantum dots and determine the average size,size distribution,and aspect ratio of overcoated particles as a function of ZnS coverage.We image the series of(CdSe)ZnS samples described earlier.Figure8shows two dots from that series, one with(A)no ZnS overcoating(bare)and one with(B)2.6 monolayers of ZnS.The particles in the micrographs show well-resolved lattice fringes with a measured lattice spacing in the bare dots similar to bulk CdSe.For the2.6monolayer sample these lattice fringes are continuous throughout the entire particle; the growth of the ZnS shell appears to be epitaxial.A well-defined interface between CdSe core and ZnS shell was not observed in any of the samples,although the“bending”of the lattice fringes in Figure8B s the lower third of this particle is slightly askew compared with the upper part s may be suggestive of some sort of strain in the material.This bending is somewhat anomalous,however,as the lattice fringes in most particles were straight.Some patchy growth is observed for the highest coverage samples,giving rise to misshapen particles,but we do not observe discrete nucleation of tethered ZnS particles on the surface of existing CdSe particles.We analyze over150 crystallites in each sample to obtain statistical values for the length of the major axis,the aspect ratio,and the distribution of lengths and aspect ratios for all the samples.Figure9shows histograms of size distributions and aspect ratio from these same samples.This figure shows the measured histograms for(A)Figure7.X-ray photoelectron spectra highlighting the Se3d core transitions from∼40Åbare and ZnS overcoated CdSe dots:(a)bare CdSe,(b)0.65monolayers,(c)1.3monolayers,and(d)2.6monolayers of ZnS.The peak at59eV indicates the formation of selenium oxide upon exposure to air when surface selenium atoms areexposed.Figure8.Transmission electron micrographs of(A)one“bare”CdSe nanocrystallite and(B)one CdSe nanocrystallite with a2.6monolayer ZnS shell.I)JN(z)iσiYi,nF(KE)e-z/λ(KE)(1)9468J.Phys.Chem.B,Vol.101,No.46,1997Dabbousi et al.。
SYNTHESIS AND CHARACTERIZATION OF POLYROTAXANES MADE FROM α-CDs THREADED ONTO TRIBLOCK COPOLYME
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Synthesis and characterization of antimony-doped tin oxide (ATO) nanoparticles by a new hydrothermal
Materials Chemistry and Physics87(2004)10–13Materials science communicationSynthesis and characterization of antimony-doped tin oxide(ATO) nanoparticles by a new hydrothermal methodJianrong Zhang,Lian Gao∗State Key Lab of High Performance Ceramics and Superfine Microstructure,Shanghai Institute of Ceramics,Chinese Academy of Sciences,Shanghai200050,PR ChinaReceived31March2004;received in revised form21May2004;accepted7June2004AbstractAntimony-doped tin oxide(ATO)nanoparticles have been synthesized by mild hydrothermal method free from the widely used metal chlo-rides.The obtained particles were characterized by means of XRD,BET,Hall effect measurements,XPS and TEM.X-ray diffraction shows that all Sb ions came into the SnO2lattice to substitute Sn ions,though the hydrothermal temperature was as low as120◦C.Increasing the heat treatment temperature accelerates the growth of the nanoparticles,changes the electrical conductivity,the distribution of the Sb ions and relative amount of the two oxidation states Sb5+and Sb3+.TEM shows the ATO nanoparticles were monodispersed in the range of3–5nm.©2004Elsevier B.V.All rights reserved.Keywords:Tin(IV)oxide;Doping;Hydrothermal synthesis;XPS1.IntroductionAntimony-doped tin oxide(ATO)is an important mem-ber of transparent conductive oxides(TCOs)[1–3]that hasbeen extensively studied for its chemical,mechanical andenvironmental stabilities[4].ATOfilms are highly conduct-ing,and electrons can tunnel easily in either direction be-tween the adsorbed electroactive species and the SnO2con-duction band[5].The introduction of Sb into the tin oxidelattice greatly increases the electron conductivity,which ren-ders this material used as an excellent conductive agent[6].ATO is transparent throughout the visible region,while re-flects infrared light.These features enable ATO to be used astransparent electrodes,heat mirrors and energy storage de-vices,have potential uses in photovoltaic and optoelectronicdevices[7,8].Nanoparticulate ATO has been used as elec-trochromic material for the production of printed displays[9]and anode material in lithium-ion batteries[10].In ad-dition,ATO has applications in nuclear waste management,good catalyst for olefin oxidation[11,12].So far,ATO particles have been synthesized by solid-statereaction[13],coprecipitation[6,7,9],Pechini[13]and hy-drothermal methods[14].The coprecipitation improves the∗Corresponding author.Tel.:+86-21-5241-2718;fax:+86-21-5241-3122.E-mail address:liangaoc@(L.Gao).reactivity of the components and Pechini method enhancesthe chemical homogeneity.But a post-calcination at over500◦C is required to incorporate Sb atoms into the tin ox-ide lattice;as a consequence,a large particle size and heavydegree of agglomeration are rge amount oforganic compounds employed in the Pechini method act notonly as complexes,but also as fuel,evolving much heat dur-ing calcination,which accelerates the growth and agglomer-ation of obtained ATO particles.The hydrothermal methoddoes not need a calcination process,and the dispersity ofthe particles is greatly improved,but a comparatively highhydrothermal temperature(270◦C)is needed.The startingmaterials used in the wet chemical methods are all frommetal chlorides,such as SnCl4,SnCl2,SbCl3and SbCl5.Itis well known that chlorine ions adsorbed on tin hydrox-ide are very difficult to be removed,and large amount ofproduct is lost during the repeated washing.The residualchlorine ions affect the surface and electrical properties,leading to both volatile antimony and tin compounds,caus-ing agglomeration among particles and sintering to highertemperature[15].For these reasons,new methods shouldbe developed to improve the yield and quality of ATOnanoparticles.In this paper,we report a new method for direct synthesisof conductive ATO nanoparticles with high specific surfaceareas by mild hydrothermal process from the starting mate-rials granulated tin and Sb2O3.The influence of hydrother-0254-0584/$–see front matter©2004Elsevier B.V.All rights reserved.doi:10.1016/j.matchemphys.2004.06.004J.Zhang,L.Gao /Materials Chemistry and Physics 87(2004)10–1311mal treatment temperature on the crystallite size,lattice pa-rameters,electrical conductivity and surface properties of the ATO nanoparticles is discussed.2.ExperimentalIn a typical synthesis,30mL of concentrated HNO 3(67wt.%)was poured into a stainless Telfon-lined 100-mL capacity autoclave containing 2g of granulated tin (pu-rity 99.95%),calculated amount of Sb 2O 3(the molar ratio [Sb]/[Sn]was set at 5:100in all reactions)and 50mL of H 2O.A large amount of brown gas (NO 2)gave off immedi-ately,and the mixed starting materials turned into a yellow colloid.The autoclave was sealed and heated to maintain at 120–170◦C for 10h,and then air-cooled to room tempera-ture.The resulting blue-colored products (characteristic of ATO particle)were collected and washed with water and enthanol,finally dried at 100◦C for 5h.The ATO nanoparticles obtained at different hydrother-mal temperatures were characterized by powder X-ray diffraction (XRD)(Model D/MAX 2550v;Rigaku Co.,Tokyo,Japan)with λ=0.15418nm,Cu K ␣and transmis-sion electron microscopy (TEM)(JEM-200CX TEM).The specific surface area of the powders was measured with a Micromeritics ASAP 2010analyzer using the multipoint Brunauer,Emmett and Teller (BET)adsorption and the av-erage grain size (d BET )of the particles were calculated from the formula d =6/ρA ,where ρis the theoretical density of SnO 2and A is the specific surface area of the powder.The conductivity of the 500MPa uniaxially pressed pellets was measured by the Hall effect measurements.The X-ray photoelectron (XPS)measurements were carried out at Mi-crolab 310-F Spectrometer with an X-ray gun for Mg K ␣radiation.The step width was 0.1eV and the spectra were referred to C1s emission at 284.6eV .3.Results and discussionFig.1shows the XRD patterns of the ATO nanoparticles.All peak positions agree well with the reflections of bulk cassiterite SnO 2.No phase ascribed to antimony compounds was detected,indicating that all antimony ions came into the lattice of bulk SnO 2to substitute for tin ions [7].The widths of the reflections were considerably broadened,and the av-Table 1Characterizations of the hydrothermally synthesized ATO nanoparticles Hydrothermal temperature (◦C)Lattice parameter D XRD (nm)Surface area (m 2g −1)d BET (nm)Conductivity (102S cm −1)a (Å)c (Å)V (Å3)120 4.758 3.18472.08 2.7234 3.72140 4.737 3.18671.49 3.2216 4.081704.7533.17871.794.01874.661020304050607080(310)(002)(220)(211)(200)(101)(110)(c)(b)(a)I n t e n s i t y /(a .u .)2θ/(o)Fig.1.XRD patterns of the ATO nanoparticles hydrothermally synthe-sized at different temperatures:(a)at 120◦C;(b)at 140◦C;(c)170◦C,respectively.erage crystallite sizes of the particles determined from the (110)plane by the Scherrer’formula were listed in Table 1.The size increased from 2.7nm at 120◦C to 3.2nm at 140◦C and 4.0nm at 170◦C,respectively.To the authors’knowl-edge,the specific surface areas are the largest,correspond-ingly decreased from 234m 2g −1at 120◦C to 187m 2g −1at 170◦C,which witnessed the growth of the nanoparti-cles.The much high surface areas may be ascribed to the free of Cl −ions that cause agglomeration among particles and the advantage of hydrothermal synthesis.The compar-ison of the crystallite size and the particle size calculated based on the surface area reveals that the nanoparticles are almost monodispersed.The lattice parameters determined by least-squares refinement are listed in Table 1.The unit cell volume of the sample obtained at 120◦C (72.08Å3)is larger than the pure SnO 2(71.56Å3JCPDS 21–1250),de-creased to 71.49Å3at 140◦C,again increased to 71.79Å3at 170◦C,respectively.The reason can be explained as fol-lows.On one hand,nanocrystalline oxide particles exhibit a lattice expansion with reduction in particle size [16].On the other hand,the antimony incorporated into the SnO 2lat-tice exists in two oxidation states,Sb(III)and Sb(V);the Sb(V)has a smaller ionic radius (r =0.60Å)than tin ion (r =0.69Å),while Sb(III)ion (r =0.76Å)is larger than tin ion [7].So,the Sb(III)/Sb(V)content ratio can change the lattice parameters.Taking no consideration of the expansion of the crystallite size on the lattice parameters,we suppose that in the 120◦C sample,most of the Sb ions are in Sb(III)12J.Zhang,L.Gao /Materials Chemistry and Physics 87(2004)10–13oxidation state;so,the unit cell volume is much larger than pure tin oxide.When the hydrothermal temperature was in-creased to 140◦C,most of the Sb(III)ions are oxidated to Sb(V);as a result,the cell volume decreased,even smaller than pure tin oxide.Further increase in the temperature to 170◦C,most of the Sb(V)ions again reduced to Sb(III)or some of the Sb ions are separated to the grain surface and the cell volume increased.This supposition can be supported by the electrical measurements and X-ray photoelectron spec-troscopy (XPS).The electrical conductivities of the ATO nanoparticles were also shown in Table 1.The conductivities were several orders of magnitude higher than the pure SnO 2,increased from 2×102S cm −1at 120◦C to the highest value at 140◦C,8×102S cm −1,and again reduced to 6×102S cm −1at 170◦C,respectively.These values are lower than the dense ATO films [17],which are ascribed to a high activation energy for electron to cross the grain boundaries between the nanoparticles.The conductivity mechanism of the ATO material is well known,the Sb(V)ions incorpo-rated into the SnO 2lattice act as an electron donors,while the Sb(III)ions compensate the donor electrons.At higher calcination temperatures (>600◦C)[18],the antimony ions incline to segregate to the grain boundary,trapping an electron pair in the bulk bandgap [19].So,the change of conductivity with the hydrothermal temperature is ascribed to the change of Sb(V)/Sb(III)ratio or the segregation of Sb.To further elucidate the relation between lattice param-eter and electrical conductivity of the ATO nanoparticles,we investigated the surface properties of the ATO materi-als by XPS,which is powerful to obtain surface informa-tion of the ATO particles [16].Because of overlapping of O1s and Sb3d5/2lines,the Sb3d3/2line is used to deter-mine the Sb concentration by making use of the relation between the prewave of Sb3d5/2and Sb3d3/2ratio fixed to be 1.44.A typical entire spectrum of the particles ob-tained at 140◦C is shown in Fig.2.The binding energy of1000800600400200I n t e n s i t y /C P S Binding Energy/(eV)Fig.2.XPS survey spectrum of the nanoparticles hydrothermally synthe-sized at 140◦C.Table 2XPS investigations of the ATO nanoparticles obtained at different tem-peratures Hydrothermal temperature (◦C)Binding energy (eV Sb3d3/2)[Sb 5+]/[Sb](%)Sb surface enrichment 120539.6521140539.8087 1.3170539.72533.2the Sb3d3/2as a function of hydrothermal temperature is shown in Table 2.As can be seen,the binding energy shifts from 539.65eV at 120◦C to 539.80eV at 140◦C,again de-creases to 539.70eV at 170◦C,respectively.The shift to higher binding energy declares that an increasing amount of Sb ions are in the oxidation state +5.The distribution be-tween Sb 3+and Sb 5+,and surface enrichment of Sb ions were also listed in Table 2.In the 120◦C hydrothermally treated sample,almost all the Sb ions are in the oxidation state +3,which leads to a lattice expansion and a low electri-cal conductivity.The Sb ions are homogeneously distributed in the material and shows no Sb surface enrichment.Increas-ing the treatment temperature to 140◦C,most of the Sb ions are oxidated to Sb 5+and evolve large amount of electrons,the unit cell volume decreased sharply,the Sb ions showed a tendency to segregate to the surface of the ATO nanopar-ticles.Further increase in the temperature to 170◦C,more Sb ions are segregated to the particle surface and the surface enrichment increases to about 2.5,which had been observed by other authors [20,21].The enriched Sb ions are in the oxidation state +3,as a consequence,the unit cell volume shrinks and the electrical conductivity decreases.What the XPS results correlates perfectly with the XRD and electricalmeasurements.Fig.3.TEM image of the ATO nanoparticles obtained at 140◦C.J.Zhang,L.Gao/Materials Chemistry and Physics87(2004)10–1313The mechanism of the formation of conductive ATOnanoparticles at comparatively low temperature can bedescribed as follows.As HNO3was added to the mixedstarting materials,a reaction occurred3Sn+Sb2O3+6H+→3Sn2++2Sb+3H2OThen,the excessive HNO3also oxidized the unreactedSn and freshly obtained Sn2+,Sb,rendering these metalions highly activated,which was evidenced by the appear-ance of the colloid.In the following hydrothermal pro-cess,the antimony ions were very easy to incorporate intoSnO2lattice and endow the nanocrystals with electricalconductivity.Fig.3shows TEM image of the ATO nanoparticles hy-drothermally treated at140◦C.All particles have a size rang-ing from3–5nm,average size of4nm with well-definededges.The nanoparticles were monodispersed in accordancewith what the above had revealed.4.ConclusionsMonodispersed ATO nanoparticles with high specific sur-face areas has been synthesized by hydrothermal method.The method free form chlorides shortened the synthesisprocess and improve the particle quality,the use of acti-vated intermediates greatly decreased the hydrothermal tem-perature to120◦C.The highest electrical conductivity(8×102S cm−1)is obtained at a hydrothermal temperature 140◦C,accompanied with the smallest unit cell volume(71.49Å3)and the highest Sb5+concentration,about87%of the Sb ions are in the oxidation state Sb5+.This methodputs forward a new strategy to synthesize multicomponentnanocrystalline oxides.References[1]T.T.Emons,J.Q.Li,L.F.Nazar,J.Am.Chem.Soc.124(2002)8516.[2]C.Goebbert,R.Nonninger,M.A.Aegerter,A.Schmidt,Thin SolidFilms351(1999)79.[3]K.Y.Rajpure,M.N.Kusumade,M.N.Neumann-Spallart, C.H.Bhosale,Mater.Chem.Phys.64(2000)184.[4]A.Gamard,O.Babot,B.M.C.Jousseaume Rascle,T.Toupance,G.Campet,Chem.Mater.12(2000)3419.[5]G.C.Jorge,P.M.Andrew,urence,D.W.Michael,Angew.Chem.Ed.42(2003)3011.[6]Z.C.Orel,B.Ore,M.Hodoscek,V.Kaucic,J.Mater.Sci.27(1992)313.[7]J.Rockenberger,U.Felde,M.Tisher,L.Troger,M.Haase,H.Weller,J.Chem.Phys.112(2000)4296.[8]H.S.Varol,A.Hinsch,Sol.Energ.Mat.Sol.C40(1996)273.[9]J.P.Coleman,J.J.Freeman,P.Madhukar,J.H.Wagenknecht,Displays20(1999)145.[10]A.C.Bose,D.Kalpana,P.Thangadurai,S.Ramasamy,J.PowerSource107(2002)138.[11]V.Dusatre,D.E.William,J.Phys.Chem.B102(1998)6732.[12]R.koivula,R.Hajula,J.Lehto,Micropor.Mesopor.Mater.55(2002)231.[13]M.I.B.Bernardi,S.Cava,C.O.P.Santos,E.R.Leite,C.A.Paskocimas,E.Longo,J.Eur.Ceram.Soc.22(2002)2911.[14]T.Nuta,U.Felde,M.Haase,J.Chem.Phys.110(1999)12142.[15](a)O.Vasykiv,Y.Sakka,J.Am.Ceram.Soc.84(2001)2489;(b)J.S.Pena,T.BrousseL.Sanchez,J.Morals,D.M.Schleich,J.Power Sources9798(2001)232;(c) A.Roosen,H.Hausener,Adv.Ceram.Mater.3(1988)131.[16]P.Vaqueiro,M.A.Lopez-Quintela,Chem.Mater.9(1997)2836.[17]K.Y.Rajpure,M.N.Kusumade,M.N.N.Spallart, C.H.Bhosale,Mater.Chem.Phys.64(2000)184.[18]K.Sun,J.Liu,N.D.Browning,J.Catal.205(2002)266.[19]R.G.Egdell,T.J.Walker,G.Beamson,J.Electron.Spectrosc.Relat.Phenomena128(2003)59.[20]D.Szczuko,J.Werner,S.Ostwald,S.G.Behr,K.Wetzig,Appl.Surf.Sci.179(2001)301.[21]J.C.V olta,P.Bussiere,G.Coudurier,J.Herrmann,J.C.Vedrine,Appl.Catal.16(1985)315.。
Synthesis and characterization of ATO SiO2 nanocomposite coating obtained by sol–gel method
Synthesis and characterization of ATO/SiO 2nanocompositecoating obtained by sol–gel methodXiaoChuan Chen *The Key Laboratory of Materials Physics,Institute of Solid State Physics,Chinese Academy of Sciences,Hefei 230031,People’s Republic of ChinaReceived 19June 2004;accepted 20December 2004Available online 11January 2005AbstractA new sol–gel route was developed for synthesizing homogeneous nanocomposite thin film that was composed of Sb-SnO 2(ATO)nanoparticles and silica matrix.TEM studies show that as-prepared composite thin film contains the amorphous silica matrix and ATO nanocrystalline particles that were dispersed homogeneously in silica matrix.The oxalic acid is an excellent dispersant for colloidal stability of ATO aqueous sol at pH b 5.The result of Zeta potential measurement shows that dispersion mechanism comes from the chemisorption of oxalic acid on the surface of ATO nanoparticles.The thermal treatment in reducing atmosphere considerably promotes grain growth of ATO nanoparticles and changes the optical property of ATO/SiO 2nanocomposite thin film.D 2005Elsevier B.V .All rights reserved.Keywords:Sol–gel preparation;Thin films;Nanocomposites;Sb-doped SnO 21.IntroductionTin oxide is a wide band gap nonstoichiometric semi-conductor with a low n-type resistivity [1–3].The resistance can be reduced further by doping Sb,F elements [4,5].F-doped SnO 2(FTO),Sb-doped SnO 2(ATO)conducting thin films not only have high transparency in the visible region but also are good infrared reflecting materials [6,7].ATO thin films have been used in many fields such as heat shielding coating on low-emissivity window for energy saving [8].Fabrication techniques used to deposit ATO thin film include dip coating based on sol–gel method;sputtering and spray pyrolysis.The sol–gel route has several advantages over the other method.It is a low cost and simple process and makes the precise control of doping concentration easier [9,10].In order to improve the scratching abrasive resistance of ATO thin film prepared by sol–gel route [11,12]a novel sol–gel route has been proposed.In this technological process an organic–inorganic hybrid silica sol was used as the pre-cursor of protecting matrix.The ATO functional componentwas homogeneously distributed in a transparent silica matrix.The mixed structure is of benefit to preventing the crack of thin film in drying and annealing process [13].When a composite material containing two oxides with different pho-to index hopes to keep high transmittance in visible light re-gion the second phase component must be dispersed homogeneously into the amorphous matrix at a level of nanometer.In this work a transparent nanocomposite thin film com-posed of ATO and silica was synthesized by the sol–gel route.The sol–gel method includes (a)the synthesis of ATO sol and hybrid organic–inorganic silica sol;(b)mixing of two nanoparticulate sols.A TEM investigation of phase structure in ATO–silica composite gel is reported.The optical proper-ties and crystallizability of composite thin film is discussed.2.Experimental2.1.Preparation of ATO aqueous solAll the chemical reagents used in the synthesis experi-ment were obtained from commercial sources without0167-577X/$-see front matter D 2005Elsevier B.V .All rights reserved.doi:10.1016/j.matlet.2004.12.033*Tel.:+865515591477;fax:+865515591434.E-mail address:chenxiaochuan126@.Materials Letters 59(2005)1239–1242/locate/matletfurther purification.The aqueous ATO sol were prepared by a co-precipitation process from hydrolysis of SnCl4d5H2O and SbCl3,and followed by the peptization of the precipitate. The reaction was performed at room temperature.In the co-precipitation procedure aqueous NH4OH solution was added directly to the mixture solution of SnCl4d5H2O and SbCl3 until the pH of the mixture reach6–8,where pale yellow ATO hydroxide precipitate were produced.Peptization of ATO hydroxide with the aqueous solution containing oxalic acid gives a yellowish transparent sol.Finally ATO sol was heated and refluxed at608C for4h.2.2.Synthesis of hybrid organic–inorganic silica solThe hybrid organic–inorganic silica-based sols were synthesized as follows:First a mixture solution of tetrae-thoxysilane(TEOS),3-glycidoxypropyltrimethoxysilane (GPTS),isopropyl and alcohol in weight ratio1:1:2.5:3.5 was prepared.Then a suitable amount of deionized water (pH=1,by HCl addition)was added to the mixture solution. The mole ratio of TEOS and H2O is about1:6to1:8.The mixed solution was stirred and heated under reflux at808C for16h.The synthesized transparent hybrid silica sol was used as protecting component of nanocomposite thin film.2.3.Preparation of ATO/SiO2nanocomposite thin filmsA transparent functional gelled film was deposited from the mixture sol comprising the hybrid organic–inorganic silica sol and the ATO sol.Deposition was performed on the glass substrate at room temperature by a simple dip coating process.After being dried at room temperature the nano-composite gelled thin film was thermally densified at a temperature up to4008C in a reducing atmosphere containing N2and vapor of alcohol.2.4.InstrumentationThe Zeta potential measurement of the0.5wt.%ATO aqueous sol was carried out with a ZETASIZER3000HS A measuring system(MALVERN).0.1N HNO3was used to adjust the pH of reference ATO sol that does not contain oxalic acid.The X-ray diffractometer(XRD)was used for the structural characterization of the as-dried and thermally densified ATO–SiO2nanocomposite material.The micro-structure feature of nanocomposite gel film and annealed film were observed with a transmission electron microscope (TEM)(type JEM-2010).The sample for TEM study was prepared as follows:A droplet of mixed sol consisting of ATO colloidal sol and hybrid silica sol was dropped on a copper grid covered with organic film,and after solvents were vaporized a nanocomposite thin film was deposited on the copper grid.The chemical composition of annealed nanocomposite thin film was measured using an energy dispersive X-ray analysis system(EDS)equipped with a scanning electron microscope.Optical transmission was determined using a Varian Cary5E spectrophotometer in the wavelength range of300–2500nm.3.Results and discussion3.1.Surface adsorption studiesWhen oxalic acid was added to the ATO suspension the pH of suspension was adjust to2by the ionization of oxalic acid.Peptization with oxalic acid turns slowly the initial turbid ATO suspension into transparent stable sol.If without addition of oxalic acid ATO nanoparticles in the suspension will show aggregating behavior and begin precipitating at pH b5.The experimental result tells us that colloidal stability of ATO sol comes from addition of oxalic acid.Oxalic acid molecule acts as a surface-modifying agent and prevents aggregation of ATO particles.Fig.1shows the result of Zeta potential measurement at different pH level.The date shows that surface of ATO nanoparticles in aqueous sol is positively charged at pH\5without the addition of oxalic acid.The addition of oxalic acid decreases the Zeta potential of surface and changes the surface to a negative charge in the pH range2–4.According to the dissociation constant of oxalic acid the neutral molecules and negatively charged HO–(CO)2–OÀ1ions are predominant components in aqueous solution at2b pH b3.In initial suspension surface of ATO nanoparticles has a charge especially opposing the oxalic acid ions.The electrostatic force generated by the opposing charges will facilitate the ions transport stage of adsorption reaction.Now we assume that markedinteraction Fig.1.Zeta potential of ATO aqueous sol as a function of pH;0.5wt.% ATO content was used.X.C.Chen/Materials Letters59(2005)1239–1242 1240exist between oxalic acid ions and positive surface hydroxylgroups Q Sn–OH 2+or neutral surface hydroxyl groups Q Sn–OH.The oxalic acid ions can be preferentially adsorbed to the surface of ATO nanoparticles by hydrogen bond or Q Sn–O–C bond.The adsorbed ions neutralize surface positive charges and ultimately reverse the surface to a negative Zeta potential.Fig.1shows that the magnitude of negative Zeta potential is not large enough to stabilize the ATO nanoparticle electrostatically in sol.After oxalic acid was added to the suspension the transparent sol is found to remain stable almost infinitely at pH b 4.The only possible explanation is that effective dispersion mechanism comes from a combination of electrostatic and steric repulsion between oxalic acid ions that were adsorbed on surface of different ATO particles.3.2.XRD and EDS studiesFig.2shows XRD spectra of the ATO–silica nano-composite sample.The pattern (a)relates to the nano-composite gel obtained as dried at room temperature and the pattern (a)shows the presence of a very broad diffraction peak attributable only to cassiterite structure.The XRD patterns of nanocomposite samples show little difference between as-dried and thermally densified samples.Theresult indicates that ATO colloidal particles have developed a nanocrystal structure of cassiterite during sol preparation which contains a hydrothermal process at 608C.TheFig.2.XRD pattern of ATO–SiO 2composite gel:(a)as-dried at room temperature;(b)heat-treated at 5008C in air for 1h.Table 1Elemental concentration of ATO/SiO 2nanocomposite thin film Sample Atomic concentration,%V olume ratio,SiO 2/ATO O Si Sn Sb As-dried69.6917.2510.722.351.5Fig.3.Diffraction pattern and TEM image of ATO–SiO 2nanocomposite thin film as-dried at room temperature:(a)ED pattern;(b)TEMimage.Fig.4.Diffraction pattern and TEM image of ATO–SiO 2composite thin film thermal-treated at 3008C in reducing atmosphere for 2h:(a)ED pattern;(b)TEM image.X.C.Chen /Materials Letters 59(2005)1239–12421241hydrothermal process under atmosphere is also an effective method for promoting the crystallization of ATO nano-particles in the aqueous solution [14,15].The element contents in ATO–SiO 2film are shown in Table 1.Measured Si/Sn+Sb atom ratio of sample is about 1.3:1.The SiO 2/ATO volume ratio in the nanocomposite is calculated from the atom ratio and theory density.3.3.TEM and UV–Vis–Nir spectra studiesThe TEM image of as-dried ATO–SiO 2nanocomposite thin film is shown in Fig.3(b).We can observe that ATO nanoparticles are homogeneously dispersed in SiO 2-based amorphous matrix without any evidence of aggregation.ATO grains are found to have a size range of 3–5nm in diameter.Fig.3(a)shows a typical electron diffraction pattern of ATO nanocrystalline grain.Four electron dif-fraction (ED)rings can be indexed to the pattern of ATO with cassiterite structure.The result is in good agreement with XRD analysis.The structural change induced by thermal treatment of ATO thin film has been investigated.Fig.4shows the ED pattern and TEM image taken from ATO–SiO 2nanocomposite thin film which was annealed at 3008C in reducing atmosphere.The contrast morphology in this image shows some large crystal grains with diameter range from 20nm to 25nm.The ED pattern taken from the same sample contains some sharp spots resulting from thelarge crystallites.The observed results indicate that thermal treatment in reducing atmosphere can accelerate grain growth of ATO nanoparticles.The growth of crystal grain was accompanied by the disappearance of grain boundary and increased electrical conductivity and Nir-light reflec-tance of ATO film [1].The optical transmission spectra of ATO thin film deposited on the glass substrate of 1mm thick are shown in Fig.5.A high transmission of 85%is observed in the visible region.The reduction of transmission in the Nir wavelength arises from improved conductivity of nanocrystalline ATO particles that were heat-treated in the reducing atmosphere.4.ConclusionsThe transparent ATO–SiO 2nanocomposite thin films have been prepared successfully by the sol–gel method.The transmission of thin film is rather high in the visible region,range between 85%and 90%as well as the transmission in Nir region has been decreased to 41%.The thermal treatment in reducing atmosphere is an effective method for promoting crystalline grain growth of ATO nanoparticles.The oxalic acid is an excellent dispers-ing agent for ATO nanoparticle in the aqueous solution in pH range 2–4.References[1]G.Frank,E.Kauer,H.Kostlin,Thin Solid Films 77(1981)107.[2]M.S.Castro,C.M.Aldao,J.Eur.Ceram.Soc.20(2000)303.[3]O.Safonova,I.Bezverkhy,P.Fabrichnyi,M.Rumyantseva, A.Gaskov,J.Mater.Chem.7(1997)997.[4]S.Shanthi,C.Subramanian,P.Ramasamy,Cryst.Res.Technol.34(1998)1037.[5]A.E.Rakhshani,Y .Makdisi,H.A.Ramazaniyan,J.Appl.Phys.83(2)(1998)1049.[6]C.Goebbert,R.Nonninger,M.A.Aegerter,H.Schmidt,Thin SolidFilms 351(1999)79.[7]C.Terrier,J.P.Chatelon,J.A.Roger,Thin Solid Films 295(1997)95.[8]H.Ohsaki,Y .Kokubu,Thin Solid Films 351(1999)1.[9]M.A.Aegerter,N.Al-Dahoudi,J.Sol–Gel Sci.Technol.27(2003)81.[10]A.N.Banerjee,S.Kundoo,P.Saha,K.K.Chattopadhyay,J.Sol–GelSci.Technol.28(2003)105.[11]S.W.Kim,Y .W.Shin,D.S.Bae,J.H.Lee,J.Kim,H.W.Lee,ThinSolid Films 437(2003)242.[12]K.Abe,Y .Sanada,T.Morimoto,J.Sol–Gel Sci.Technol.26(2003)709.[13]J.Gallardo,A.Duran,I.Garcia,J.P.Celis,M.A.Arenas,A.Conde,J.Sol–Gel Sci.Technol.27(2003)175.[14]D.Y .Zhang,D.Z.Wang,G.M.Wang,Y .H.Wu,Z.Wang,Mater.Sci.Eng.,B,Solid-State Mater.Adv.Technol.8(1991)189.[15]S.J.Kim,S.D.Park,Y .H.Jeong,S.Park,J.Am.Ceram.Soc.82(1999)927.Fig.5.UV–Vis–Nir transmission spectra:(a)550nm thick ATO–SiO 2thin film which was coated on glass substrate;(b)glass substrate.X.C.Chen /Materials Letters 59(2005)1239–12421242。
硼酸酯合成
Synthesis and Characterization of Monodisperse OligofluorenesJungho Jo,+[b]Chunyan Chi,+[a]Sigurd Hˆger,[c]Gerhard Wegner,*[a]and Do Y.Yoon*[b]Introduction9,9-Disubstituted polyfluorenes find extensive scientific and technological application as efficient organic blue-light-emit-ting diode materials.[1,2]Polyfluorenes showextremely high photoluminescence quantum yields,high thermal and oxida-tive stability,and good solubility in common organic sol-vents for easy processing by spin-or dip-coating methods.[3]They also exhibit interesting thermotropic liquid-crystal characteristics,[4]and consequently,upon annealing in the nematic melts,the polymer chains were shown to be easily aligned on a rubbed polyimide surface.[5]Such an alignment of the polymer results in the polarization of the emitted light and improves the charge carrier mobility,a prerequisite for the fabrication of an organic thin-film transistor.[6]Thus,the ability of the polyfluorenes to align excellently paves the way to make thin films with highly anisotropic electrooptical and electrical properties.[7]Polyfluorenes are readily prepared by Ni 0-mediated cou-pling of the corresponding dibromo monomers.Polymers obtained by this method have weight-averaged molecular weights (M w )of the order of several hundred thousand with polydispersities of around three (according to GPC analysis against polystyrene standards).The long chain lengths and the polydispersity in chain lengths lead to complex structur-al characteristics of the thin films and make it very difficult to establish a proper structure±property relationship.More-over,the normal synthetic procedure leads to incorporation of a small amount of chemical defects,which may be re-sponsible for undesirable green-band emission characteris-tics.[8]Therefore,for better understanding of the structure±prop-erty relationships of polyfluorenes,it would be very helpful to study the properties of a series of pure oligomers with well-defined length and no chemical defects.The absorption spectra of a series of oligomers will allow the estimation of the effective conjugation length of the polymer.[9]In addi-tion,a detailed study of the photoluminescence spectra of pure oligomers may help to solve questions concerning the origin of the green-emission band observed in the photolu-minescence and electroluminescence spectra of polyfluorene films.[10]Moreover,well-defined,defect-free oligofluorenes may also be welcome as active materials in organic light-emitting diodes and organic thin-film transistors.Monodispersed dialkyl fluorene oligomers were first re-ported by Klaerner and Miller.[11]They showed that the Ni 0-mediated oligomerization of 2,7-dibromo-9,9-bis(n -hexyl)-fluorene in the presence of 2-bromofluorene as an end-cap-ping agent gives a mixture of oligomers and low-molecular-weight polymers that could be fractionated by HPLC.From the spectroscopic properties of the samples,the effective[a]C.Chi,+Prof.Dr.G.WegnerMax Planck Institute for Polymer Research Ackermannweg 10,55128Mainz (Germany)Fax:(+49)6131-379-100E-mail:wegner@mpip-mainz.mpg.de [b]J.Jo,+Prof.Dr.D.Y.YoonSchool of Chemistry,Seoul National University San 56±1,Sillim-dong,Seoul,151±747(Korea)Fax:(+82)2-877-6814E-mail:dyyoon@snu.ac.kr [c]Prof.Dr.S.HˆgerPolymer-Institut,Universit‰t KarlsruheHertzstrasse 16,76187Karlsruhe (Germany)[+]These authors contributed equally to this work as part of their Ph.D.theses.Abstract:An efficient synthesis of 9,9-bis(2-ethylhexyl)fluorene oligomers up to the heptamer is reported,with repet-itive Suzuki and Yamamoto coupling reactions employed in the synthesis.The key steps for preparation of the es-sential intermediates include Pd-cata-lyzed transformation of aryl bromides to aryl boronic esters (Miyaura reac-tion)and the application of the much higher reactivity of aryl boronic esters over aryl bromides in the Pd-catalyzed cross-coupling reaction with aryl diazo-nium salts.Variation of the UV/Vis ab-sorption and photoluminescence char-acteristics with chain length is report-ed.Moreover,glass transition and liquid-crystal characteristics of the oligomers are described and compared with those of the polymer.Keywords:fluorene ¥glasses ¥liq-uid crystals ¥oligomerization ¥pho-toluminescenceFULL PAPERconjugation length was estimated to be approximately 12fluorene units.Lee and Tsutsui prepared a series of oli-gofluorenes up to the tetramer by a repetitive2n divergent approach from2,7-dibromo-9,9-bis(n-hexyl)fluorene,with coupling with bis(n-hexyl)fluorene-2-borate and subsequent bromination of the coupling product.[12]Anemian et al.syn-thesized monodisperse dihexylfluorene oligomers up to the hexamer by a combination of Suzuki and Yamamoto cou-pling reactions.[13]Oligomers with n repeating units contain-ing only one bromine atom at positions2or7on the end fluorenes were prepared by coupling the corresponding monoboronate(nÀ1)with2-bromo-7-iodo-9,9-bis(n-hexyl)-fluorene at the iodo site,which is significantly more reactive than the bromo site.The resulting monobromo oligomers were then coupled by a Yamamoto reaction.Most recently, a detailed description of the synthesis,optical properties, and solid-state properties of defined oligofluorenes,up to the hexadecamer,containing chiral substituents at position9 was presented by Geng et al.[14]Here again,the iodo/bromo selectivity in the Suzuki coupling reaction and the use of tri-methylsilyl groups as dormant iodides were used as key fac-tors in the oligomer synthesis.The enormous success of the Suzuki reaction[15]in the preparation of these oligomers arises from the high yield of the coupling reaction together with the easy availability of the boronic acids and the boronates.[16]They are prepared in good to excellent yields by halogen±metal exchange and subsequent trapping of the aryl lithium compound with trial-kylborates.Recently,the scope of this reaction has been dra-matically expanded by the discovery that aryl boronates are also available directly from the aryl halides by a Pd0-cata-lyzed reaction with the pinacol ester of diboron(the Miyaura reaction).[17]This transformation avoids the use of strongly basic organometallic reagents and thus allows the preparation of a wide variety of functionalized aryl boronic esters.Here,we present the synthesis of oligofluorenes from the dimer up to the heptamer by Suzuki and Yamamoto reac-tions,[18]with the Miyaura reaction employed for the first time for the preparation of the aryl boronates.Also,we have taken advantage of a large difference in the reactivity between aryl diazonium salts and aryl bromides in the Suzuki coupling reaction[19]in the preparation of the key in-termediates.The oligomers have been characterized with re-gards to their optical(absorption and photoluminescence) properties and their phase behavior,including glass transi-tion and liquid-crystal characteristics.Finally,the properties of the oligomers are compared with those of the polymer in order to gain newinsights into the polymer properties.Results and DiscussionSynthesis of oligofluorenes:The synthetic route towards the oligofluorenes is shown in Scheme1.First,2,7-dibromofluor-ene and2-bromofluorene were alkylated with2-ethylhexyl bromide to give the di-and monobromides of fluorene,1 and3,respectively.Both of these compounds,as well as the corresponding boronic acids,have already been reported in the literature.[11±14]However,in our synthesis,we trans-formed the aryl bromides into the corresponding aryl boron-ic esters with the Miyaura reaction.In these reactions the corresponding boronic esters,2and4,are formed in high yields(>90%)and can easily be purified by column pounds4and2were then coupled with3 to give the fluorenyl dimer5and trimer6,respectively. Scheme1.Synthesis of the oligofluorenes:a)2-Ethylhexyl bromide,50% aqueous NaOH/DMSO,room temperature;b)bis(pinacolato)diboron, AcOK/DMF,[Pd(dppf)Cl2],608C;c)[Pd(PPh3)4],toluene/aqueous Na2CO3,reflux;d)BF3¥OEt2,butylnitrite/dichloromethane,À108C;e)Pd(OAc)2/EtOH,reflux;f)Br2,dichloromethane,reflux;g)[Ni(cod)2], COD,Bipy,toluene/DMF,808C.DMSO=dimethylsulfoxide,DMF= N,N-dimethylformamide,dppf=1,1’-bis(diphenylphosphanyl)ferrocene, COD=cycloocta-1,5-diene,Bipy=2,2’-bipyridine.FULL PAPER G.Wegner,D.Y.Yoon et al.To synthesize the longer fluorene oligomers,the unsym-metrical monobrominated intermediates,such as9and11, are essential.However,these intermediates cannot be ob-tained directly by bromination of5or6with bromine,since statistical product mixtures are obtained which are very dif-ficult to separate on a large scale.One possibility to obtain the monobrominated intermediates is to use compounds with one potential reaction site in a protected form(for ex-ample,trimethylsilyl groups instead of bromo or iodo func-tionalities[20])as described by Geng et al.[14]Another way is to use fluorene derivatives with two reaction sites of signifi-cantly different reactivity.In the latter case,the use of bro-moiodofluorene derivatives is quite obvious since the reac-tivity of aryl iodides towards the Suzuki coupling is substan-tially higher than the reactivity of aryl bromides;this con-cept has already been used by Anemian et al.[13]A good alternative approach is to use the large reactivity difference between aryl diazonium salts and aryl bromides in the cross-coupling reaction with aryl boronates.Since the reaction with aryl diazonium salts does not need a base such as Na2CO3,which is essential in the Suzuki coupling reac-tion with aryl bromides,the coupling reaction takes place only at the site of the diazonium salt.Hence,we employed this reaction in our synthetic procedure as follows.2-Amino-7-bromofluorene was alkylated with2-ethylhex-yl bromide to give7in82%yield;7was subsequently trans-formed into the corresponding diazonium salt8(81%). Cross-coupling reaction of4and8with Pd(OAc)2gave9in 70%yield within an hour.This result shows that the reactiv-ity difference between aryl diazonium salts and aryl halides is larger than that between aryl iodides and aryl bromides.9 was transformed into the corresponding boronic ester10in 56%yield with the Miyaura reaction.Subsequently,the cross-coupling reaction of10and8gave11in48%yield. Another method we have used to obtain the monobro-mides is to treat the monoboronate with an excess of the di-bromofluorene.Indeed,the coupling of4with an excess of 1was successfully performed by using only1.5equivalents of1to give the monobrominated dimer9in50%yield(not shown in Scheme1).Similarly,the monobrominated trimer 11was obtained in45%yield by the reaction of4with1.5-fold excess of the dibrominated product12,which was pre-pared from5in90%yield.[21]Both methods led to identical compounds,thereby demonstrating the validity of our syn-thetic methodology.Yamamoto homocoupling re-actions of9and11gave the flu-orenyl tetramer13and hexam-er15,respectively,both in%50%yield.The fluorenylpentamer14was obtained witha cross-coupling reaction of9and2in47%yield.The highreactivity of the diazonium saltswas also used to prepare the di-bromofluorenyl trimer16,which was obtained in54%yield by coupling of2and8.Although16can,in principle,also be prepared by the bromination of6,a detailed mass spectral analysis of the crude reaction products showed that varying amounts of tribromide contaminate the dibromide. Since even small amounts of an impurity affect the liquid-crystalline behavior of the oligomers,we avoided the bromi-nation of the fluorenyl trimer and higher oligomers in our oligomer synthesis.The fluorenyl heptamer17was obtained in38%yield by cross-coupling reaction of10and16. Optical properties of oligofluorenes:Electronic absorption spectra of monodisperse oligo(9,9-bis(2-ethylhexyl)fluorene-2,7-diyl)compounds5,6,13,14,15,and17in diluted chloroform solution with the same fluorene unit concentra-tion(1.0î10À5m)are shown in Figure1and the data are col-lected in Table1.The oligofluorenes exhibit unstructured absorption bands, as is also seen for polyfluorenes.[3]The absorption maximum is red-shifted with increasing number(n)of fluorene units. The molar extinction coefficients(e)of the oligofluorenes showa good approximation of a linear increase w ith n from dimer to heptamer,as seen in Table1.The increment is 30.3î103L molÀ1cmÀ1for each repeat unit.The plot of the wave number of the maximum absorption versus1/nfollows Figure1.UV/Vis absorption of oligofluorenes(dimer to heptamer)in chloroform solution at room temperature at a fixed concentration of flu-orene repeat units of1.0î10À5mole LÀ1.Table1.Summary of UV/Vis absorption(n max(abs))and photoluminescence(n max(PL))spectra for the fluoreneoligomers and polymer,from chloroform solutions and solid films.[a]Sample Solution Filmn max(abs)e max n max(PL)n max(abs)n max(PL)[cmÀ1][L molÀ1cmÀ1][cmÀ1][cmÀ1][cmÀ1]dimer530580491702740025970304002710025770trimer628740813302538024100286502513023870tetramer13279301115002475023470275502439023200pentamer14274001417002445023150270302398022940hexamer15271701730002433023040268802381022780heptamer17268802003002427023040268102370022730polymer26110±2410022940259102359022570[a]Since the resolution of the low-energy peak was too low at the temperature at which the data were record-ed,only the n max values of the two high-energy components are given.Synthesis and Characterization of Monodisperse Oligofluorenes2681±2688a linear fit,as shown in Figure 2.The polymer has a maxi-mum absorption at 26110cm À1(383nm);[3]hence,we can estimate an effective conjugation length of 14repeat unitsfrom the plot in Figure 2,a figure that can be compared with the reported value of 12for poly(9,9-bis(n -hexyl)fluor-ene-2,7-diyl).[11]The UV/Vis absorption spectra of thin films of the oligofluorenes on quartz substrates are practically identical to the solution data except for slight red-shifts in the absorption maxima,as listed in Table 1.Figure 3a shows the photoluminescence (PL)spectra of the oligomers from dimer 5to heptamer 17in chloroform with the same concentration of fluorene units (1.0î10À6m ),excited at the corresponding energy of maximum absorp-tion.Similar to polyfluorenes,three well-resolved fluores-cence bands are observed.They may be assigned to the 0±0,0±1,and 0±2intrachain singlet transitions.[22]The spectral position and the intensity of the PL maximum changes with the number of fluorene units,n .This is explained by the in-crease of effective conjugation from dimer 5up to heptamer 17.Notably,the relative intensity of the three emission bands also changes with n .The relative intensity of the 0±0transition increases with n ,while that of the 0±2transition decreases.This may be related to an increase of the intra-chain coupling interaction with the molecule×s length.Normalized solid-state PL spectra of oligofluorenes 5,6,13,14,15,and 17from thin films on a quartz plate excited at the absorption maxima are shown in Figure 3b and the key data are listed in Table 1.Relative to the PL spectra measured in solution,red shifts in the emission maxima are observed and the relative intensities of the 0±2intrachain singlet transition increase in all cases.Most importantly,the green-band emission usually seen for the polymer [3]is absent for all of the oligomers (Figure 3b).Even upon high-temperature annealing (1808C)in air,this green emission is still negligible for the oligomers.This result casts doubt on the widely discussed hypothesis that the green emission seen with varable intensity in polymer samples (Figure 3b)origi-nates from excimer formation by interchain interaction.It is difficult to see why such interchain interactions should be suppressed in the case of oligomers if this explanation was true.Phase transition characteristics of oligofluorenes :The DSC traces shown in Figure 4clearly exhibit the glass transition temperatures for all of the oligomers in the low-temperature range,followed by an endothermic transition for the tetram-er 13,pentamer 14,hexamer 15,and heptamer 17as the temperature is increased.The latter transition is identified as the liquid-crystalline to isotropic transition from the po-larized optical microscopy study.The Schlieren texture and the very small enthalpy value of the transition,as shown in Table 2,indicate that the liquid-crystal structure is probably of nematic character,but a further study on this topic is in progress.The isotropization temperature T iso of this liquid-crystal-line to isotropic transition extrapolates to a hypothetical T iso (Polymer)for n !¥of 4758C if plotted in the coordi-nates T iso =T iso (n !¥)(1ÀKX E )where X E is the molefrac-Figure 2.Plot of n ˜max versus reciprocal degree of polymerization n.Figure 3.a)Fluorescence spectra of oligofluorenes (dimer to heptamer)in chloroform solution at room temperature at a fixed concentration of fluorene repeat units of 1î10À6mole L À1.b)Photoluminescence spectra of thin films of the oligofluorenes (dimer to heptamer).The spectrum for the polymer,also shown in this figure,was obtained for a sample an-nealed at 1808C for 1h in air.FULL PAPERG.Wegner,D.Y.Yoon et al.tion of end groups and K is an empirical constant.This tem-perature is well above the decomposition range of the high polymer.In this regard,it is important to note that the poly-mer exhibits a well-known ™melting∫transition around 1608C.Above 1608C the polymer exists in a nematic liquid-crystal phase;belowthat temperature another solid phase is formed,the true nature of which is not yet understood.It may be of higher order smectic type but of such a rigidity of the packing that a transition to a glassy state is suppressed.Whether this substantial difference in the phase structure and nature of transitions has consequences for the electro-optical properties of these materials needs to be studied fur-ther.The glass transition temperatures,listed in Table 2,tend to level off as the chain length increases and exhibit n À1de-pendence of the type:T g =64.0À174.7n À1.Therefore,the extrapolated T g for the polymer is estimat-ed to be approximately 648C.The occurrence of this glass transition is difficult,if not impossible,to see in the DSC thermogram for the polymer (see Figure 4).This may be due to the above-mentioned differences of the liquid-crystal phases in the polymer and in the oligomers.ConclusionOligofluorenes up to the heptamer can be synthesized on the hundred-milligram scale by a stepwise route involving Suzuki and Yamamoto coupling reactions.The synthesis of the boronates for the Suzuki coupling is based on the Pd-catalyzed transformation of aryl bromides into boronates,a process that avoids strongly basic aryl lithium intermediates.Therefore,this methodology has potential for the synthesis of oligofluorenes containing a variety of functional groups.The synthesis of mono-or dibrominated fluorenyl oligomers,which are essential for expanding of the chain length,is based on the much higher reactivity of aryl boronates over aryl bromides in the Pd-catalyzed cross-coupling reaction with aryl diazonium salts.The pure oligomers as solid films do not showthe unde-sired green-band emission characteristics of the polymer.Moreover,they are found to align more readily to form monodomains on various surfaces,as will be published else-where.The oligomers from tetramer to heptamer show a liquid-crystal phase with clearly defined isotropization tem-peratures;this allows extrapolation to the expected isotropi-zation temperature of the polymer at around 4758C,well above the thermal decomposition temperature.Most impor-tantly,the oligofluorenes do not showthe same high-order phase that the polymer exhibits belowthe melting tempera-ture of approximately 1608C.However,unlike the polymer,the oligomers do showa glass transition temperature w hichexhibits n À1dependence and allows extrapolation to a hypo-thetical glass transition of the polymer at around 648C.As this glass transition refers to a freezing of a liquid-crystal phase not seen for the polymer,it is not too surprising that this phenomenon cannot be detected for the polymer.Experimental SectionGeneral remarks :Reactions requiring an inert gas atmosphere were con-ducted under argon and the glassware was oven-dried (1408C).Tetrahy-drofuran (THF)was distilled from potassium prior to mercially available chemicals were used as received.1H NMR and 13C NMR spec-tra were recorded on Bruker DPX 250or AC 300spectrometers (250and 300MHz for 1H,62.5and 75.48MHz for 13C).Chemical shifts are given in ppm,referenced to residual proton resonances of the solvents.Thin-layer chromatography was performed on aluminium plates precoated with Merck 5735silica gel 60F 254.Column chromatography was per-formed with Merck silica gel 60(230Æ400mesh).Field desorption spec-tra were recorded on a VG ZAB 2-SE FPD machine.Differential scan-ning calorimetry was measured on a Mettler DSC 30with a heating or cooling rate of 10K min À1.Polarization microscopy was performed on a Zeiss Axiophot apparatus with a nitrogen-flushed Linkam THM 600hot stage.UV/Vis spectra were recorded at room temperature with a Perkin±Elmer Lambda 9UV/Vis/NIR spectrophotometer.Photoluminescence spectra were obtained on a Spex Fluorolog II (212)apparatus.Optical properties of solid thin films were normally obtained for samples spin-coated on a quartz substrate from dilute chloroform solutions and dried under vacuum.Elemental analysis were performed by the University of Mainz.Melting points were measured with a Reichert hot-stage appara-tus and are uncorrected.2,7-Dibromo-9,9-bis(2-ethylhexyl)fluorene (1):2-Ethylhexylbromide (38.73g,185.18mmol,35.74mL)was added to a mixture of 2,7-dibromo-fluorene (25.0g,77.16mmol)and triethylbenzylammonium chloride (0.878g, 3.86mmol,5mol %)in DMSO (125mL)and 50%aqueousFigure 4.DSC traces for the oligofluorenes (dimer to heptamer;second heating at 108C min À1).The DSC trace for the polymer is also shown for comparison.Table 2.Summary of glass transition temperature (T g ),isotropization temperature (T iso ),and the enthalpy of isoptropization value (D H iso )for the oligofluorenes.Sample T g [K]T iso [K]D H iso [J g À1]dimer 5252±±trimer 6274±±tetramer 132953370.50pentamer 143013990.47hexamer 153074630.71heptamer 173155190.74Synthesis and Characterization of Monodisperse Oligofluorenes 2681±2688NaOH(31mL).The reaction mixture was stirred at room temperature for5h.An excess of diethyl ether was added,the organic layer was washed with water,diluted HCl,and brine,then dried over MgSO4.The solvent was removed under vacuum and the residue was purified by column chromatography over silica gel with n-hexane as the eluent(R f= 0.78)and solidified from EtOH atÀ308C to give1as a white solid (36.21g,85.6%):M.p.45±548C;1H NMR(250MHz,CD2Cl2):d=7.57±7.43(m,6H),1.94(d,J=5.35Hz,4H),0.89±0.68(m,22H),0.55±0.41(m, 8H)ppm;13C NMR(62.5MHz,CDCl3):d=152.3,139.1,130.1,127.4, 121.0,55.3,44.3,34.6,33.6,28.0,27.1,22.7,14.0,10.3ppm;MS(FD): m/z:548.2[M+].2-Bromo-9,9-bis(2-ethylhexyl)fluorene(3):Compound3was prepared ac-cording to the method used for1by using2-ethylhexylbromide(43.3g, 224.5mmol,39.9mL),2-bromofluorene(25.0g,102.0mmol),triethylben-zylammonium chloride(1.16g,5.10mmol,5mol%),DMSO(165mL), and50%aqueous NaOH(41mL).Purification by column chromatogra-phy over silica gel with n-hexane as the eluent(R f=0.72)gave3as a col-orless liquid(43.14g,90.1%):1H NMR(250MHz,CD2Cl2):d=7.70±7.26 (m,7H),1.97(m,4H),0.90±0.43(m,30H)ppm;13C NMR(62.5MHz, CDCl3):d=152.8,150.0,140.3,129.8,127.3,126.9,124.0,120.9,120.4, 119.6,55.1,44.4,34.6,33.6,28.0,27.0,22.7,14.0,10.4ppm;MS(FD): m/z:470.2[M+].2,7-Bis(4,4,5,5-tetramethyl[1.3.2]dioxaborolan-2-yl)-9,9-bis(2-ethylhexyl)-fluorene(2):Under an argon atmosphere,1(2.43g,4.43mmol),bis(pina-colato)diboron(4.05g,15.94mmol),KOAc(2.60g,26.57mmol),and Pd(dppf)Cl2(0.226g,0.266mmol)were dissolved in DMF(40mL)and heated to608C overnight.After the reaction mixture was cooled to room temperature,water and diethyl ether were added.The aqueous phase was extracted with diethyl ether and the combined organic layers were dried over MgSO4.The solvent was removed under vacuum and the resi-due was purified by column chromatography over silica gel with petrole-um ether/dichloromethane(3:1)as the eluent(R f=0.34)and solidified from EtOH atÀ308C to give2as a white solid(2.60g,91.5%):M.p.85.5±87.68C;1H NMR(250MHz,CD2Cl2):d=7.84±7.69(m,6H),2.00 (d,J=5.3Hz,4H), 1.36(s,24H),0.86±0.50(m,22H),0.48±0.45(m, 8H)ppm;13C NMR(62.5MHz,CDCl3):d=150.1,143.9,133.5,130.4, 119.2,83.5,54.7,44.0,34.6,33.5,27.8,27.2,24.8,22.7,14.1,10.3ppm;MS (FD):m/z:643.0[M+].2-(4,4,5,5-Tetramethyl[1.3.2]dioxaborolan-2-yl)-9,9-bis(2-ethylhexyl)fluor-ene(4):Compound4was prepared according to the method used for2 by using3(14.07g,30.0mmol),bis(pinacolato)diboron(12.19g, 48.0mmol),KOAc(8.82g,90.0mmol),and[Pd(dppf)Cl2](1.23g, 1.5mmol)in DMF(300mL).Column chromatography over silica gel with petroleum ether/dichloromethane(4:1)as the eluent(R f=0.59)af-forded4as an oily product(14.78g,95.5%):1H NMR(250MHz, CD2Cl2):d=7.82±7.64(m,4H),7.36±7.21(m,3H),2.0±1.86(m,4H), 1.34(s,24H),0.86±0.65(m,22H),0.50±0.43(m,8H)ppm;13C NMR (62.5MHz,CDCl3):d=151.0,149.5,144.2,141.1,133.6,130.3,126.6, 124.1,120.0,118.8,83.5,54.8,44.5,44.1,34.6,33.5,28.2,27.8,27.3,26.8, 24.8,22.7,14.1,10.5,10.1ppm;MS(FD):m/z:516.7[M+].9,9,9’,9’-Tetrakis(2-ethylhexyl)-2,2’-bifluorene(5):A mixture of4(5.17g, 10.0mmol)and3(4.69g,10.0mmol)in toluene(50mL)and2m aqueous Na2CO3solution(25mL,50mmol)was degassed by pump and freeze cycles(3î)and[Pd(PPh3)4](0.577g,0.5mmol)was added under argon. The solution was heated to reflux with vigorous stirring for20h.After the reaction mixture was cooled to room temperature,diethyl ether and water were added.The organic layer was separated and washed with di-luted HCl and brine,then dried over MgSO4.The solvent was removed under vacuum and the residue was purified by column chromatograpy over silica gel with petroleum ether as the eluent(R f=0.47)to give5 (7.08g,90.8%):1H NMR(250MHz,CD2Cl2):d=7.73±7.80(m,4H), 7.57±7.64(m,4H),7.25±7.44(m,6H),2.04±2.14(m,8H),0.49±0.88(m, 60H)ppm;13C NMR(62.5MHz,CDCl3):d=150.9,150.6,141.1,140.4, 126.8,126.3,126.0,124.1,122.9,119.6,54.9,44.5,34.6,33.8,28.2,26.9, 22.7,14.0,10.3ppm;MS(FD):m/z:779.4[M+];elemental analysis: calcd for C58H82(779.2):C89.39,H10.61;found:C89.29,H10.79.9,9,9’,9’,9’’,9’’-Hexakis(2-ethylhexyl)-2,2’-7’,2’’-terfluorene(6):Compound 6was prepared according to the method used for5by using2(2.0g, 3.12mmol),3(4.40g,9.36mmol),and[Pd(PPh3)4](0.36g,0.31mmol)in toluene(30mL)and2m Na2CO3aqueous solution(15.6mL,31.2mmol)for27h.After cooling to room temperature,the mixture was diluted with ethyl acetate and the organic layer was washed with diluted HCl and brine,then dried over MgSO4.The solvent was removed under vacuum and the residue was purified by column chromatography over silica gel with petroleum ether as the eluent(R f=0.22)to give6as a col-orless viscous gum(2.32g,63.8%):1H NMR(250MHz,CD2Cl2):d= 7.83±7.73(m,6H),7.61±7.66(m,8H),7.44±7.25(m,6H),2.13±2.05(m, 12H),0.90±0.49(m,90H)ppm;13C NMR(62.5MHz,CDCl3):d=151.2, 150.9,150.6,141.1,140.4,140.1,126.8,126.3,126.0,124.1,122.9,119.7, 119.6,54.9,44.6,34.6,33.8,28.2,27.1,22.8,14.0,10.3ppm;MS(FD):m/ z:1168.2[M+];elemental analysis:calcd for C87H122(1167.9):C89.47,H 10.53;found:C89.26,H10.42.2-Amino-7-bromo-9,9-bis(2-ethylhexyl)fluorene(7):Compound7was prepared according to the method used for1by using2-ethylhexylbro-mide(7.78g,40.3mmol,7.2mL),2-amino-7-bromofluorene(5.0g, 19.2mmol),triethylbenzylammonium chloride(220mg,1mmol,5 mol%),DMSO(50mL),and50%aqueous NaOH(3.8mL).The reac-tion mixture was stirred for2h.Purification by column chromatography over silica gel with n-hexane/dichloromethane(6.5:3.5)as the eluent (R f=0.47,0.44,and0.38;the title product separated into three spots,due to the diaseteroisomers)gave7as a slightly yellowoily product(7.65g, 82%):1H NMR(300MHz,CD2Cl2):d=7.46±7.37(m,4H),6.70±6.63(m, 2H),3.81(br s,2H),1.84±1.90(m,4H),0.92±0.73(m,22H),0.57±0.52 (m,8H)ppm;13C NMR(75MHz,CDCl3):d=152.5±152.4(three peaks, 2îC),146.9±146.8(three peaks),141.4,131.5±131.4(three peaks),129.8, 127.4±127.3(three peaks),120.9,119.9,118.7±118.5(three peaks),114.2, 110.9±110.8(three peaks),55.2,44.9±44.8(four peaks),35.0,33.9±33.7 (four peaks),28.5±28.3(four peaks),23.2,14.3,10.6±10.4(four peaks)ppm;MS(FD):m/z:484.0[M+].2-Bromo-9,9-bis(2-ethylhexyl)fluorenyl-7-diazonium tetrafluoroborate (8):A solution of7(3.48g,7.18mmol)in CH2Cl2(10mL)was slowly added to BF3¥OEt2(11.46mmol,1.42mL)with stirring under an argon athmosphere atÀ108C.After10min,a solution of butyl nitrite(1.18mL, 10.01mmol)in CH2Cl2(4mL)was slowly added and the mixture stirred for additional30min at08C.n-Pentane(200mL)was added and the mix-ture was stored atÀ208C overnight.The precipitate was filtered off, washed with cold diethyl ether and dried in air to give8as a pale yellow solid(3.39g,81%):1H NMR(300MHz,[D6]acetone):d=9.08(m,1H), 8.87(m,1H),8.53(m,1H),8.16(m,1H),8.06(s,1H),7.77(m,1H), 2.30±2.20(m,4H),0.88±0.45(m,1H)ppm;13C NMR(75MHz,acetone-d6):d=156.6,154.2±153.9(three peaks),153.8,137.9±137.8(three peaks), 134.6,132.6±132.5(three peaks),129.5±129.4(three peaks),129.0±128.8 (three peaks),126.7,125.8,123.7±123.6(three peaks),111.9±111.6(three peaks),57.6±57.5(three peaks),44.5±44.3(four peaks),35.9±35.8(two peaks),34.7±33.9(three peaks),28.9±28.5(three peaks),28.0,23.4±23.3 (two peaks),14.3±14.2(two peaks),10.7±10.3(three peaks)ppm;decom-position temperature:988C.7-Bromo-9,9,9’,9’-tetrakis(2-ethylhexyl)-2,2’-bifluorene(9):A mixture of 4(0.90g, 1.74mmol),8(1.12g, 1.92mmol),and Pd(OAc)2(40mg, 0.178mmol)in ethanol(30mL)was heated to608C for1h(no addition-al base was added).After cooling to room temperature,the mixture was diluted with diethyl ether and the organic layer was washed with brine and dried over MgSO4.The solvent was removed under vacuum and the residue was purified by column chromatography over silica gel with pe-troleum ether as the eluent(R f=0.49)to give9as an oily product(1.04g,70%):1H NMR(250MHz,CD2Cl2):d=7.80±7.26(m,13H),2.14±2.04(m,8H),0.88±0.52(m,60H)ppm;13C NMR(62.5MHz, CDCl3):d=153.0,151.0,150.6,141.0,140.5,140.1,139.2,129.9,127.4, 126.8,126.4,126.0,124.1,122.9,120.9,120.3,119.6,54.9,44.5,34.6,33.8, 28.2,27.1,22.7,14.0,10.3ppm;MS(FD):m/z:857.6[M+].2-[9,9,9’,9’-Tetrakis(2-ethylhexyl)-7,2’-bifluoren-2-yl]-4,4,5,5-tetrame-thyl[1.3.2]dioxaborolan(10):Compound10was prepared according to the method used for2by using9(970mg,1.1mmol),bis(pinacolato)di-boron(450mg,1.8mmol),KOAc(326mg,3.3mmol),and[Pd(dppf)Cl2] (45mg,0.055mmol)in DMF(10mL).Column chromatography over silica gel with n-hexane/CH2Cl2(9:1)as the eluent(R f=0.12)gave10as an oily product(570mg,55.7%):1H NMR(300MHz,CD2Cl2):d=7.86±7.73(m,6H),7.65±7.60(m,4H),7.41(m,1H),7.36±7.27(m,2H),2.09±2.04(m,8H),1.35(s,12H),0.88±0.49(m,90H)ppm;13C NMR(75MHz, CD2Cl2):d=152.8,151.6,151.3,150.5±150.3,144.6,141.7,141.1±140.6, 134.1,131.1±130.9,127.4,127.0,126.6±126.5,124.8,123.6±123.4,120.8,FULL PAPER G.Wegner,D.Y.Yoon et al.。
东华大学应用化学专业导论-精细化学品导论
[5] 4-[(4-Chlorophenyl)(phenyl)methyl]piperazin-1-ium picrate monohydrate, Acta Cryst. E, 2012, 68(8), o2486
精细化学品导论
李洪启 2012-11-27
个人简介
李洪启: 67792594, 13391141551, hongqili@
3#学院楼6113室
2004.9-
: 东华大学化学化工与生物工程学院
2003.4-2004.4: Aix-Marseille大学法国科学研究中心研究员
2002.5-2003.3: 日本爱媛大学应用化学系访问学者
[32] 3,3’,5,5’-Tetrabromo-2,2’-bithiophene, Acta Cryst., 2009, E65, o952 [33] Gabapentinium picrate, Acta Cryst., 2009, E65, o783 [34] 4-(4-Carboxybenzyl)-1-methylpiperazin-1-ium picrate, Acta Cryst., 2009, E65,
dione skeleton, Chem. Cent. J., 2010, 4, 18
[22] (2E)-1-(1,3-Benzodioxol-5-yl)-3-(2-bromophenyl)prop-2-en-1-one, Acta Cryst., 2010, E66(6), o1289
Synthesis and characterization of metal complexes
Synthesis and characterization ofmetal complexesIntroductionMetal complexes have been actively studied due to their potential applications in various fields such as catalysts, materials, and medicine. The synthesis and characterization of metal complexes are fundamental steps towards understanding their properties and behaviors. In this article, we will discuss some of the methods and techniques used for synthesizing and characterizing metal complexes, as well as their applications.Synthesis of metal complexesThe synthesis of metal complexes can be achieved through various methods such as salt metathesis, ligand exchange, and coordination polymerization. Salt metathesis involves replacing one metal ion in a salt with another metal ion. Ligand exchange involves replacing one ligand in a metal complex with another ligand. Coordination polymerization involves the combination of metal ions and organic ligands to form a three-dimensional network structure.One example of a metal complex synthesis method is ligand exchange. In this method, a metal complex with a specific ligand is reacted with a new ligand to form a different metal complex. For example, the reaction between copper(II) sulfate and sodium acetate results in the formation of copper(II) acetate.CuSO4 + 2NaOAc → Cu(OAc)2 + Na2SO4Another example is coordination polymerization. In this method, metal ions and organic ligands are combined in a solution to form a solid network structure. For example, the reaction between zinc(II) nitrate and 2,6-naphthalenedicarboxylic acid results in the formation of a porous coordination polymer called MOF-5.Zn(NO3)2 + H2bdc → Zn4O(H2bdc)3 + 2HNO3Characterization of metal complexesCharacterization of metal complexes is important in understanding their physical and chemical properties. Techniques such as X-ray crystallography, infrared spectroscopy, and nuclear magnetic resonance (NMR) spectroscopy can be used to identify the structure and composition of metal complexes.X-ray crystallography involves the analysis of crystals using X-rays to determine the positions of atoms in a molecule. It provides information on the three-dimensional structure of a metal complex. Infrared spectroscopy involves the measurement of the energy absorbed by a molecule due to vibrations of its chemical bonds. It provides information on the functional groups present in a metal complex. NMR spectroscopy involves the measurement of the absorption of energy by nuclei in an external magnetic field. It provides information on the electronic environment surrounding metal ions in a complex.Applications of metal complexesMetal complexes have a wide range of applications in various fields. They can act as catalysts in chemical reactions, for example, the use of palladium complexes as catalysts in Suzuki coupling reactions. They can also be used as materials in the form of coordination polymers for gas storage or catalysis. In medicine, metal complexes can be used as contrast agents in imaging techniques or as anticancer drugs.ConclusionIn summary, the synthesis and characterization of metal complexes are important for understanding their properties and behavior. Various methods and techniques can be used for synthesizing and characterizing metal complexes. Applications for metal complexes are diverse and extend to fields such as catalysis, materials, and medicine. With continued research and development, metal complexes are expected to play an increasingly important role in these fields.。
Synthesis and Characterization of Er3+∶Y3Al5O12 Nanocrystalline Powders Prepared by Sol-Gel Met
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Synthesis and characterization of three-dimensional crosslinked networks based on self-assemly of a -cyclodextrins with thiolated 4-arm PEG using a three-step oxidationHuaiqing Yu,Zeng-guo Feng,*Ai-ying Zhang,Ling-gang Sun and Lijun QianReceived 5th December 2005,Accepted 2nd February 2006First published as an Advance Article on the web 16th February 2006DOI:10.1039/b517206cA kind of novel three-dimensional crosslinked networks based on the self-assemly of a -CDs with thiolated four-arm PEG was prepared by thiol-disulfide interchange reaction using a three-step oxidation.The supramolecular structure of the resulting hydrogels was characterized via FTIR,1H NMR,XRD,DSC and TGA measurements.The results demonstrated that the channel-type crystalline structure of inclusion complexes is still maintained after the multi-step oxidation.According to the swelling and degradation tests,the swelling behaviors and degradationproperties can be readily regulated by tuning the feed compositions of a -CDs and PEG-thiolated prepolymer.Furthermore,the threading a -CDs clearly protects disulfide bonds from an attack of a reduced form of glutathione as a result of prolonging the degradation time of the hydrogels in water.IntroductionSupramolecular architectures with topological characteristics have attracted considerable attention experimentally and theoretically.1Inclusion complex (IC)is a topological molecule composed of macrocycles threaded onto a linear polymer backbone via non-covalent interactions.2Because of the introduction of mechanical interlinking,it possesses different topologies and properties compared with a conventional small molecule or polymer.Cyclodextrins (CDs)are a kind of cyclic oligomers of a -D -glucose linked by a -1,4-glycoside bonds.3Their most familiar members are a -,b -,and c -CDs consisting of six,seven,and eight glucose units,respectively.Owing to the water-solubility and ability to selectively include a large range of guest molecules,cyclodextrins have been the most widely studied macrocyclic molecules.4Since Harada et al.first reported the inclusion complexes resulting from PEG and a -CDs in 1990s,5an enormous variety of ICs based on CDs have been extensively investigated.However,most of the inclusion complexes reported up to now are prepared by using linear polymer axles.6Making more complicated and well-ordered two or three-dimensional polyrotaxane systems is very interesting in terms of their novel topologies and properties.Jiao and coworkers reported ICs made from low molecular weight multi-arm PEG (three,four and six arms)with a -CDs.7Sabadini and Cosgrove described a synthesis of inclusion complexes with high molecular weight star-shaped PEG containing 13and 15arms.8Zhu et al.prepared inclusion complexes using hyperbranched polyether and a -CDs,9and found that these complexes show a novel lamellar morpho-logy and possess a juxtaposed structure.Furthermore,Okumura et al.disclosed a topological hydrogel by chemically cross-linking a -CDs threaded onto PEG molecular chain.10Unlike classical hydrogels,this polyrotaxane-based hydrogel can absorb water as high as 400times its dry weight and exhibits better flexible and tensile properties than the normal chemically crosslinked hydrogels.Recently,Sarvothaman and Ritter developed a mutually interlocked gel from host–guest complexes of a -CD and methylated b -cyclodextrin with diacrylates and dimethacrylates of small molecular diols in the presence of a redox initiator system in water.11Meanwhile,our group had developed a series of supra-molecular structured hydrogels by photopolymerization of physical hydrogels yielded from (meth)acryloyl terminated PCL–PEG–PCL 12and PLA–PEG–PLA 13with a -CDs.Owing to incorporating degradable polyester blocks into the pre-polymers,the resultant hydrogels are degradable in water.Recently,we have reported a kind of thermosensitive and supramolecular structured hydrogels via copolymerization of N -isopropylacrylamide with photocurable polypseudo-rotaxanes as cross-linkers under UV irradiation.14The results suggested that the original thermosensitivity of the prepoly-mers disappear upon threading a -CDs onto the prepolymer backbones and reappear after poly(N -isopropyl-acrylamide)is introduced.As is well known,thiol is a multi-functional reagent in the area of organic and polymeric chemistry.Descriptions about the use of thiols in chemical reactions can be traced back over 100years.Nowadays,the thiol-disulfide interchange reaction has resumed extensive interest,partially fuelled by its special role in DNA activation and repression,15as well as remarkable advantages in injectable tissue engineering.16On the one hand,disulfide bonds can be degraded into thiols in cytosol responding to the reduction potential mainly developed by high concentrations (5mM)of a reduced form of glutathione.On the other hand,disulfide bonds are stable in the oxidative environment of the cell exterior.17This dual character has beenBeijing Institute of Technnology,No.5South Street Zhongguancun,District Haidian,Beijing 100081,PR China.E-mail:sainfeng@;Fax:+861068912927;Tel:+861068912650PAPER /softmatter |Soft MatterD o w n l o a d e d o n 30 M a r c h 2011P u b l i s h e d o n 16 F e b r u a r y 2006 o n h t t p ://p u b s .r s c .o r g | d o i :10.1039/B 517206Capplied in some gene delivery materials.18In the present work,we intended to prepare a kind of novel three-dimensional crosslinked networks of polypseudorotaxanes made from the self-assembly of a -CDs with thiolated four-arm PEG by thiol-disulfide interchange reaction.It is expected that the resulting hydrogels have the potential to be used as drug and gene delivery carriers,biosensors as well as injectable tissue-engineering scaffolds.ExperimentalMaterialsFour-arm PEG (4A-PEG,M n =21100)was supplied by Liming Research Institute of Chemical Industries,Henan,China and a -CD was received from Sigma,USA.p -Toluenesulfonic acid,a reduced form of glutathione as well as thioglycolic acid (TGA)were supplied by VAS Chemical Reagents Company,Tianjin,China.TGA was distilled under reduced pressure before using.All other solvents and reagents were of analytical grade.Measurements1H NMR (400MHz)spectra were recorded as solutions on a Bruker ARX 400NMR instrument at room temperature and tetramethylsilane (TMS)as internal standard.FTIR spectra were measured using Shimadzu IR Prestige-21FTIR spectro-meter at room temperature in the range between 4000and 500cm 21,with a resolution of 2cm 21and 20scans.Powder samples were prepared by dispersing the samples in KBr and compressing the mixtures to form disks.Gel permeation chromatography (GPC)analysis was carried out with a chromatographic system equipped with a Waters 1515isocratic HPLC pump and a Waters 2414refractive index detector.Three columns were in series (Waters styragel HT3,HT4,and HT5,7.86300mm).THF was used as eluent at a flow rate of 1.0ml min 21.Monodispersed polystyrene standards were used to obtain a calibration curve.Wide-angle X-ray diffraction (WAXRD)measurements were performed on powder and film samples using Panaltic X 9pert PRO X-ray diffractometer.The radiation source used was Ni-filtered Cu K a radiation with a wavelength of 0.154nm.The voltage was set to be 40KV and the current 40mA.Samples were placed on a sample holder and scanned from 4.5to 60u in 2h at a speed of 0.0017u s 21.Thermogravimetric analysis (TGA)of samples was made using TA Instrument 2000thermogravimetric analyzer at a heating rate of 20u C min 21with nitrogen used as purge gas.Differential scanning calorimetry (DSC)measurements were carried out using a TA Instrument 2910differential scanning calorimeter.The DSC thermograms covered the temperature range of 2100to 150u C at a scanning rate of 10u C min 21.The swelling behaviors of dried gels were studied by a general gravimetric method.Dried films (a diameter of 10mm and a thickness of 2mm)were incubated in distilled water or DMSO at 25u C,and the swollen weight for each sample was recorded at regular time intervals after excess surface solvent was blotted carefully with moistened filter paper.Theprocedure was repeated until there was no further weight increase.The swelling ratio (SR)was calculated by the eqn (1):SR ~m 1{m 0m 0|100%(1)where m 0stands for the initial weight of dried gel and m 1the weight of the swelling gel at a prescribed time interval.Preparation of thiolated four-arm PEGFour-arm PEG was chain-end thiolated by esterification reaction with TGA using p -toluenesufonic acid as a catalyzer.Briefly,10mg p -toluenesufonic acid,10g of 4A-PEG,and 0.8g TGA were added to 100ml of toluene preheated to 120u C.The reaction proceeded for 10h under nitrogen atmosphere and was driven forward by the continuous removal of water produced.The thiolated prepolymer was purified by precipita-tion into anhydrous ether (200ml)at 5u C.This sequence was repeated three times using dichloromethane as a solvent.The product was then dried under vacuum at room temperature for 2days with yield of 90%.FTIR/cm 21:2866(CH 2,CH 3),1736(C L O),1109(C–O);1H NMR (CDCl 3)/ppm:d 4.298(s,8H,–CH 2–O–C(L O)–), 3.577–3.645(m,1980H,–OCH 2–CH 2–O–),3.287–3.307(d,8H,–O–C(L O)–CH 2–),2.145–2.150(t,4H,–SH).The GPC result showed a unimodal peak with a polydispersity index of 1.12.Preparation of polypseudorotaxaneA saturated aqueous solution containing a predetermined amount of a -CDs was added to a certain volume of 20wt%end-thiolated PEG solution in water at room temperature.The resulting mixture was sonicated for 10min and then stood for gelation.A gelation occurred rapidly to yield a physical hydrogel because of the supramolecular self-assembly of a -CDs with the prepolymer.The gel was washed with a small amount of distilled water and then directly freeze-dried to give rise to polypseudorotaxane.Preparation of gel film crosslinked by disulfide bond formation A physical gel was firstly prepared in PBS buffer (pH =7.4)containing a predetermined amount of the prepolymer and a -CDs.After being stirred vigorously,the gel was poured onto 1062mm poly(tetrafluoroethylene)disc and allowed to crosslink in air and dry spontaneously at room temperature for 3days.The sample was then dried under vacuum to constant weight and weighted as W i .Thereafter,air-crosslinked film disc was further oxidized by immersion in 0.1wt%H 2O 2for 1h.The film disc was then rinsed with distilled water and dried in air and at ambient temperature for 1day.The dried film disc was again immersed in 50wt%DMSO aqueous solution in order to attain thoroughly crosslinking.After 6h,the 50wt%DMSO aqueous solution was displaced with pure DMSO to leach out unthreaded a -CDs as well as uncrosslinked prepolymers presumably entrapped in the gel network.This course was carried out for 3days and the solvent was refreshed daily.Finally,after being rinsed with a large amount of distilled water,the film disc was dried at 40u C under vacuum to constant weight,and weighted as W t .D o w n l o a d e d o n 30 M a r c h 2011P u b l i s h e d o n 16 F e b r u a r y 2006 o n h t t p ://p u b s .r s c .o r g | d o i :10.1039/B 517206CFor the sake of expression,the supramolecular structured hydrogels studied in this work were designed as 4A-m ,in which m stands for the feeding molar ratio of a -CDs to the prepolymer.For comparison,the corresponding gel without adding a -CDs,denoted as 4A-0,was also prepared adopting the similar oxidation procedure.Results and discussionPreparationA physical gelation took place quickly at room temperature upon mixing a thiolated 4-arm PEG prepolymer solution with a saturated aqueous solution of a -CDs.The resulting physical hydrogel was freeze-dried to give IC or polypseudorotaxane.It is known that thiol can be transformed to disulfide bond using a number of oxidants,like dilute nitric acid,iodine,bromine,hypochlorous acid and so on.Furthermore,the disulfide bond may also be formed by oxygen in atmosphere under weak alkaline conditions.19In the present study,the physical gel formed from the self-assemly of a -CDs with thiolated 4-arm PEG in PBS buffer was firstly oxidized in air to form a film.The pure thiolated prepolymer without adding a -CDs was found to be crosslinked well under this condition.However,the threading a -CDs impaired the thiol-disulfide interchange reaction of the prepolymer to afford very weakly crosslinked hydrogels when only oxidized in air.For further crosslinking,the dried film sample was again immersed into 0.1wt%H 2O 2solution for 1h owing to longtime immersion could lead to the serious oxidation degradation of PEG molecular chains.As a result,this treatment greatly improved the crosslinked network integrity,but did not still provide the film with satisfactory mechanical properties.It was reported that DMSO oxidation had been often used in disulfide bond formation.20Thence,the film disc was finally immersed in 50wt%aqueous solution of DMSO.After 6h,the solution was displaced with pure DMSO to leach out unthreaded a -CDs as well as uncrosslinked prepolymers presumably entrapped in the hydrogel network.Consequently,the well crosslinked film disc was obtained by this three-step oxidation crosslinking process.The supramolecular self-assembly of a -CDs with thiolated 4-arm PEG and corresponding oxidation crosslinking reactions are shown in Scheme 1.A series of film discs consisting of 20,40and 80a -CDs per thiolated prepolymer were synthesized using the three-step oxidation procedure.The resultant film discs were opaque in water,but transparent in DMSO as depicted in Fig. 1.However,the thiol-disulfide interconversion was observed to hardly proceed any more when the feed molar ratio of a -CDs to the prepolymer exceeds 120.In order to determine the amount and percent coverage of the threading a -CDs,the film discs were degraded in 50mM of high concentration of a reduced form of glutathione,and then calculated via 1H NMR analysis.As presented in Table 1,the amount of the threading a -CDs per thiolated PEG prepolymer and percentage coverage of a -CDs are 26and 10.8%in sample 4A-20,61and 25.4%in 4A-40as well as 82and 34.1%in 4A-80,respectively.The amounts of the threading a -CDs are all higher than the theoretical feed values,possibly attributed to that most uncrosslinked prepolymers have been extracted out duringthe course of preparation of film disc samples.Moreover,the gel content (GC)was also calculated according to the eqn (2):GC ~W tW i|100%(2)As can be seen in Table 1,the gel contents of all supramolecular structured hydrogels are in the range from 76.2%to 81.4%after the three-stepoxidation.Scheme 1Schematic illustration of supramolecular self-assembly and oxidation crosslinkingprocesses.Fig.1The photograph of a supramolecular structured hydrogel (a)in H 2O and (b)in DMSO.Table 1Gel content with and without adding a -CDs,the threading amount of a -CDs in per thiolated prepolymer and percent coverage of a -CDs NameGel content a (%)CD/PEG bCoverage c (%)S4-096.300S4-2076.22610.8S4-4081.46125.4S4-8078.58234.1aGel content is calculated by (W t /W i )6100%.b The average number of a -CDs found per thiolated 4-arm PEG chain.cCoverage =(2CD/PEG)/(PEG repeat units),resuming 2PEG repeat units per a -CD.D o w n l o a d e d o n 30 M a r c h 2011P u b l i s h e d o n 16 F e b r u a r y 2006 o n h t t p ://p u b s .r s c .o r g | d o i :10.1039/B 517206CCharacterizationDMSO is a better solvent for disolving polypseudorotaxanes formed from PEG and a -CDs,but the dissolution will result in the dethreading of a -CDs substantially from PEG backbones.In general,the 1H NMR spectra of the polypseudorotaxanes in DMSO appear identical to that of a physical blend of the two components,indicating that these polypseudorotaxanes exist as a dynamical mixture of threaded and unthreaded species.In contrast,the formation of polyrotaxanes will broaden the resonance peaks of a -CDs attributing to the decrease in conformational flexibility caused by introducing bulky stop-pers to impede a -CDs sliding out of PEG axles.21Slight changes in the chemical shifts of a -CDs are generally observed because of the changes of chemical environments as a consequence of the host–guest interaction.221H NMR spectra of a pure a -CD(A)and a polypseudorotaxane made from the thiolated four-arm PEG prepolymer with a -CDs (theoretical feed molar ratio of a -CDs to prepolymer is 40)(B)are shown in Fig.2.However,the peaks of a -CD in the poly-pseudorotaxane were found to be slightly broadened as compared to pure a -CD,most likely resulted from the formation of disulfide bonds to yield polyrotaxane to some extent in DMSO-d 6owing to air oxidation during the course of measurement.The largest chemical shift of H(3)proton of a -CD was noticed to shift downfield in this case as compared with its free counterpart.Other resonance peaks in the polypseudorotaxane were assigned as follows:O(2)H at d 5.429–5.434,O(3)H at 5.504–5.521,H(1)at 4.792–4.799,and O(6)H at 4.462–4.488ppm,respectively.Multiple resonances appeared at d 3.506–3.791are the chemical shift of H(3),H(6)H(5)protons and PEG,and at 3.275–3.408ppm those of H 2O,H(2),and H(4).FTIR spectra of a -CD (A),4A-40(B)and thiolated four-arm PEG (C)are illustrated in Fig.3.The thiolated PEG spectrum exhibits vibrating bands at 1109and 1736cm 21,which are attributed to the C–O–C stretching mode and the characteristic stretching vibration of carbonyl group in ester,respectively.The pure a -CD spectrum displays extremely strong band around 3383cm 21,assigned to the symmetric and asymmetric O–H stretching mode.The broad hydroxyl band is shifted to higher frequency at 3419cm 21owing to the formation of ICs,which is most likely a consequence of the non-covalent interaction between O–H of a -CD and the prepolymer backbone.What is more,there are evident differences in the positions and intensities of the spectra between free a -CD and supramolecular structured hydrogel,suggesting a host–guest interaction indeed existed rather than a simple physical mixture of a -CD and thiolated PEG.TGA thermal analysis is a powerful technique from which the supramolecular interaction between host and guest molecules in ICs can be determined.The supramolecular structured hydrogels undergo a two-step thermal degradation process.The fist step is mainly attributed to the decomposition of a -CDs,while the second mainly to that of the guest prepolymers.Here,the temperature at which two tangents intersect is used as the decomposition temperature of a particular component (T d )to quantitatively evaluate the thermal stability of the samples.As outlined in Fig.4,the T d values for a -CD (A)and 4A-0(B)are 287and 392u C,separately.Upon threading a -CDs onto the prepolymer chains to form the supramolecular structured networks,the T d data for the component a -CD and prepolymer are 325and 398u C for 4A-20(C),321and 402u C for 4A-40(D),and 318and 397u C for 4A-80(E),respectively,and they are all higher than their free counterparts.This fact clearly implies that the thermal stability of individual component is sub-stantially improved as long as an inclusion complex is formed between them.Fig.5shows the DSC curves of pure a -CD (A),4A-0(B),4A-20(C),4A-40(D)and 4A-80(E).There is adistinctD o w n l o a d e d o n 30 M a r c h 2011P u b l i s h e d o n 16 F e b r u a r y 2006 o n h t t p ://p u b s .r s c .o r g | d o i :10.1039/B 517206Cendothermic peak at58.7u C corresponding to the melting point of PEG crystalline phase in the sample4A-0.Upon the formation of ICs,the corresponding endothermic peak is absent as evidenced in the supramolecular structured gels of 4A-40and4A-80,because the PEG molecular chain is included in the channel of the host a-CD lattice,which restricts its aggregating to form the crystalline phase.23 However,the endothermic peak in4A-20is still observable. This is possibly ascribed to that the threading amount of a-CDs in this sample is too low to thoroughly limit the aggregation and crystallization of PEG chain.Meanwhile,its fusion temperature moves to a lower range(at52.9u C),and the enthalpy change decreases dramatically with forming IC. Evidently,the decreasing in the fusion temperature and the enthalpy change are caused by the perturbation of crystal-lization resulted from the partial inclusion of PEG molecular chain into the channel of the host a-CDs.The XRD patterns of a-CD(A),thiolated four-arm PEG (B),a polypseudorotaxane consisting of the thiolated pre-polymer and a-CDs(theoretical feed molar ratio of a-CDs to prepolymer is40)(C),a pure gel of4A-0(D),and supra-molecular structured gels of4A-20(E),4A-40(F)and4A-80(G)are presented in Fig.6.The diffraction peaks of pure a-CD appear at12.36,22.09and26.70u,respectively.The thiolated prepolymer presents only two strong peaks at19.09and 23.24u.The diffraction pattern of the polypseudorotaxane is rather different from that of either a-CD or the thiolated PEG, showing a strong peak at2h=20.06u(d=4.42A˚).This is a characteristic peak to form a channel-type crystalline struc-ture.5While,the diffraction patterns in the supramolecular structured hydrogels resemble that of the polypseudorotaxane exhibiting a strong peak at about2h=20u.Thus,it can be deduced that there also exists the channel-type crystalline structure in these polyrotaxane-related hydrogel networks.But all the characteristic diffraction peaks slightly shift to lower range,such as the characteristic peak in4A-20appeared at 19.80u,4A-40at19.75u and4A-80at19.68u.Swelling behaviors of supramolecular structured hydrogels According to the feed compositions,a series of hydrogels with a-CDs and without a-CDs were prepared and their swelling ratios were measured in distilled water and DMSO at25u C, respectively.As illustrated in Fig.7,the hydrogel of4A-0(A) made from the pure thiolated prepolymer has the highest SR in water.The SR of the supramolecular structured hydrogels of 4A-20(B),4A-40(C)and4A-80(D)was found to decrease with increasing the content of a-CDs threaded onto the network chain.A rational explanation is that the channel-type crystalline structure formed from the self-assembly of a-CDs with the prepolymer impairs water to enter the hydrogel matrix.Furthermore,their SR in DMSO was also measured. As pictured in Fig.8,the swelling behaviors in DMSO evidently differ from that in distilled water.First,4A-0(A) hardly swells in DMSO,showing poor dissolution ability for PEG.Second,the SR of all supramolecular structured hydro-gels of4A-20(B),4A-40(C)and4A-80(D)is higher than that in distilled water,suggesting that DMSO is capable of unfolding crystalline congeries formed from theself-assembly Downloadedon3March211Publishedon16February26onhttp://pubs.rsc.org|doi:1.139/B51726Cof a-CDs.Third,the discipline of SR depended on the a-CDs to thiolated prepolymer feed molar ratio in DMSO is also different from that in water.The SR of the gel4A-40(C)is higher than that of other two samples of4A-20(B)and4A-80 (D).Although DMSO here is a better solvent able to com-pletely unfold the channel-type crystalline structure leading a-CDs to disperse along the whole molecular chain,it is not true for the pure thiolated PEG-based three-dimensional crosslinked hydrogel networks.Consequently,the resulting SR is the competing balance between DMSO to unfold the crystalline lattice of uncovered and covered PEG segments with a-CDs.In other words,the swelling behaviors of this kind of supramolecular structured hydrogels can be readily regulated via varying the feed compositions of a-CDs and thiolated4-arm PEG prepolymer.Degradation behaviors of supramolecular structured gelsFig.9shows a change in SR of the gels with a different amount of threading a-CDs and unthreading a-CDs in PBS buffer (pH=7.4)containing a high concentration(50mM)of a reduced form of glutathione.The SR of4A-0(A)quickly increases until about4h and then immediately decreases, indicating typical bulk erosion with water uptake.On the other hand,such a drastic increase of the SR is not observed in the supramolecular structured hydrogels,and their complete degradtaion times are prolonged with increasing the threading amount of a-CDs to20h for4A-20(B),36h for4A-40(C)and 84h for4A-80(D).This fact implies that a-CDs threaded onto the hydrogel network chains have protected disulfide bonds during the course of the reduction degradation.This is most likely owing to the threading a-CDs holding back the attacking of the reductive agent glutathione on disulfide bonds included in the cavities of a-CDs.Thiol-disulfide interchange reaction under mild conditions is very interesting.Controlling the formation and cleavage of the disulfide bonds in the supramolecular structured hydrogels through changing external conditions could help us to design and prepare a kind of novel smart polyrotaxane-related three-dimensional crosslinked hydrogels to achieve the drug and gene controlled release and tissue engineering scaffold injectable.In this study,a three-step oxidation crosslinking procedure was used,via O2in air,0.1wt%H2O2as well as DMSO,respectively,to fulfill the thiolated4-arm PEG crosslinked well,which is evidently too harsh to meet the demands for the drug and gene controlled delivery,and in situ crosslinking injectable tissue engineering.Therefore,looking for more biocompatible oxidation methods is our ongoing study.Furthermore,a great number of hydroxyl groups exit in each a-CD threaded onto the polymer backbones,which can be also used as active positions for further chemical modifications.ConclusionsIn this study,a kind of novel three-dimensional crosslinked hydrogel networks of polypseudorotaxanes based on the self-assemly of a-CDs with the thiolated4-arm PEG was synthesized via thiol-disulfide interchange reaction by means of a three-step oxidation.The channel-type crystalline structure of inclusion complexes was found to remain in the hydrogel network chains after the oxidation crosslinking process.The a-CDs threaded onto the network chains protected disulfide bonds from the reduction attack ofa Downloadedon3March211Publishedon16February26onhttp://pubs.rsc.org|doi:1.139/B51726Creduced form of glutathione.Their swelling behaviors and degradation properties can be tailored by changing the feed composition of a -CDs and thiolated PEG prepolymer.A further chemical modification of the a -cyclodextrins is our next target to afford clear gels in water.The potential biomedical applications of these supramolecular structured hydrogels in the area of drug and gene delivery carriers,as well as injectable tissue engineered scaffolds are now under investigations.AcknowledgementsThe authors gratefully acknowledge a grant from the Natural Science Foundation of China (No.20374008)and BIT Research Fund (No.200302B02).References1 D.A.Leigh,J.K.Y.Wong,F.Dehez and F.Zerbetto,Nature ,2003,4,24,174;J.W.Lee and K.Kim,Top.Curr.Chem.,2003,228,111;F.Huang and H.W.Gibson,Prog.Polym.Sci.,2005,30,982.2S.A.Nepolgodiev and J.F.Stoddart,Chem.Rev.,1998,98,1956.3Cyclodextrin Chemistry ,ed.M.L.Bender and M.Komiyama,Springer-Verlag,Berlin,1978.4 A.Harada,Adv.Polym.Sci.,1997,133,141.5 A.Harada and M.Kamachi,Macromolecules ,1990,23,2821.6Y.Kawaguchi,T.Nishiyama,M.Okada,M.Kamachi and A.Harada,Macromolecules ,2000,33,4472;T.Michishita,Y.Tskashima and A.Harada,Macromol.Rapid Commun.,2004,25,1159;F.E.Porbeni,E.M.Edeki,I.D.Shin and A.E.Tonelli,Polymer ,2001,42,6907;H.Fujita,T.Ooya and N.Yui,Macromol.Chem.Phys.,1999,200,706;J.Li,B.Chen,X.Wang and S.H.Goh,Polymer ,2004,45,1777;J.Y.Li and D.Y.Yan,Macromolecules ,2001,34,1542;K.M.Huh,T.Ooya,S.Sasaki and N.Yui,Macromolecules ,2001,34,2402.7H.Jiao,S.H.Goh and S.Valiyaveettil,Macromolecules ,2002,35,1980.8 E.Sabadini and T.Cosgrove,Langmuir ,2003,19,9683.9X.Y.Zhu,L.Chen,D.Y.Yan,Q.Chen,Y.F.Yao,Y.Xiao,J.Hou and J.Y.Li,Langmuir ,2004,20,484.10Y.Okumura and K.Ito,Adv.Mater.,2001,13,485.11M.K.Sarvothaman and H.Ritter,Maromol.Rapid Commun.,2004,25,1948.12S.P.Zhao,Z.G.Feng and D.X Piao,Chem.J.Chin.Univ.,2003,24,186;Z.G.Feng and S.P.Zhao,Polymer ,2003,44,5177.13H.Wei,A-Y.Zhang,L.Qian,H.Yu, D.Hou,R.Qiu and Z-G.Feng,J.Polym.Sci.,Part A:Polym.Chem.,2005,43,2941.14H.Wei,H.Yu,A-Y.Zhang,L-G.Sun,D.Hou and Z-G.Feng,Macromolecules ,2005,38,8833.15H.Kadokura,F.Katzen and J.Beckwith,Annu.Rev.Biochem.,2003,72,111.16X.Z.Shu,Y.Liu,F.S.Palumbo,Y.Luo and G.D.Prestwich,Biomaterials ,2004,25,1339;S.Cai,Y.Liu,X.Z.Shu and G.D.Prestwich,Biomaterials ,2005,26,6054;Y.Lee,H.Koo,G-W.Jin,H.Mo,M.Y.Cho,J-Y.Park,J.S.Choi and J.S.Park,Biomacromolecules ,2005,6,24.17 D.P.Jones,J.L.Carlson,V.C.Mody Jr,J.Cai,M.J.Lynn and P.Sternberg Jr,Free Radical Biol.Med.,2000,28,625.18V.S.Trubetskoy,V.G.Budker,L.J.Hanson,P.M.Slattum,J.A.Wolff and J.E.Hagstrom,Nucleci Acids Res.,1998,26,4178;E.Dauty,J.-S.Remy,T.Blessing and J.-P.Behr,J.Am.Chem.Soc.,2001,123,9227.19X.Z.Shu,Y.Liu,F.Palumbo and G.D.Prestwich,Biomaterials ,2003,24,3825.20J.P.Tam,C.Wu,W.Liu and J.Zhang,J.Am.Chem.Soc.,1991,113,6657.21T.Zhao and H.W.Beckham,Macromolecules ,2003,36,9859.22H.S.Choi,T.Ooya,S.Sasaki,N.Yui,Y.Ohya,T.Nakai and T.Ouchi,Macromolecules ,2003,36,9313.23X.Li,J.Li and K.W.Leong,Macromolecules ,36,1209.D o w n l o a d e d o n 30 M a r c h 2011P u b l i s h e d o n 16 F e b r u a r y 2006 o n h t t p ://p u b s .r s c .o r g | d o i :10.1039/B 517206C。