有机光电导体增感剂N,N'-二乙基-3,3'-二吩噻嗪基-甲苯基碘鎓盐的合成及光敏性研究

有机光电导体在静电复印、全息记录、信息存储等方面得到实际应用.特别是半导体激光器的研制成功,人们对研究适于近红外(780-850 nm)的有机光电导材料越来越感兴趣。它在半导体激光打印,影像印刷等应用中具有广阔的前景。     

有机电荷传输材料

光导体是一种重要的信息功能材料,可广泛应用于静电复印,全息照相,计算机终端仪器的激光打印,轻印刷制版等。自1938年美国人Calson^[1]等发明了利用感光导电现象的复写方式——电子照相以来,用于光导体的材料开发非常活跃。近年来,有机光导体(OPC)的实用化研究工作非常活跃,受到世人的瞩目.     

激光打印技术用改性PVK—TeNF光导材料

一、引言新一代的带有计算机控制,数字扫描,激光成象的激光印刷系统,引起了各方面极大的关注,该系统具有图象质量好,印刷速度快,版面可任意安排和调制的优点,而且体积小巧,还可实现台面印刷,一般还可直接印刷在普通纸张上,印刷速度可达120—300页/分。其印刷质量高,分辨率达600点/英寸,远高于常规印刷技术的质量,工作时噪音也小,且具有多功能印刷效果。这种新的激光印刷体系的版材所     

纳米粒子的制备及其在打印印刷领域的应用

本文简要介绍了几类纳米粒子的制备及其在打印印刷领域的应用.包括无机纳米粒子复合材料用于绿色打印制版、聚合物乳胶纳米粒子用于喷墨打印制备光子晶体、金属纳米粒子用于印刷电路以及纳米材料用于3D打印,并展望了其发展前景.     

激光诱导羟基磷灰石夹层纸表面碳化实现无墨打印

传统的油墨打印具有方便快捷的优势,但打印过程中墨水或碳粉的大量使用对人体和环境造成了不可忽视的危害。基于激光的高能粒子特性和光热辐射热效应,利用激光欠焦和聚焦两种工作模式,可实现激光无墨打印和微区加工。本文报道了一种基于羟基磷灰石的“有机-无机-有机”三明治结构多功能纸,并利用激光的光热辐射效应使功能纸表层有机材料——纤维素纤维表面温度升高,实现表层均匀碳化,夹层无机材料——羟基磷灰石阻挡能量继续传导防止纸张烧穿,以此来达到无墨打印的效果。基于激光烧蚀的无墨打印,能够显著降低打印成本,有利于激光烧蚀打印技术的推广。此外,采用激光烧蚀打印技术作用于功能纸上的打印效果具有稳定、绿色环保等特点,在档案存储用纸、食品包装用纸和后天致盲患者阅读等方面具有广泛的应用。     

液态金属印刷电子墨水研究进展

印刷电子是一种基于印刷原理的新兴电子增材制造技术,与传统电子加工方法相比,它在大面积、柔性化、个性化、低成本制造电子等方面具有无可比拟的优势。印刷电子所用的典型导电墨水通常分为三类：碳系、高分子及金属导电墨水,然而它们在打印后仍需借助高温后处理工艺,以进一步提升打印物及墨水的电导率及运行可靠性,步骤稍显繁琐;且由于相应纳米材料及墨水的配制较为复杂,也增加了使用的成本。液态金属作为一大类新出现的电子打印墨水,近年来正日益成为重要的研究领域,这种墨水具有电导率高、制备简单、无需后处理等独特优点。为推动这一方向的研究,本文评述了国内外围绕液态金属导电墨水物理化学性质的研究进展及对应的典型打印方法,并指出了进一步发展的方向。     

印刷有机数字电路及应用

印刷有机电子技术是基于印刷原理的有机电子器件制造技术,是指将有机电子材料配制成功能性油墨,用印刷方式来制造电子器件与系统的方法,其发展涉及到材料化学、微电子学等多个学科方面的知识。其独特的制造方式和器件形态具有柔性、低成本、大面积制造等优势,并且与传统硅基电子器件在应用场合上形成了互补,在生物传感、电子皮肤、柔性显示等领域展示出优势。为了及时跟进这一快速发展的领域,对领域的发展有宏观的把握,本文从印刷技术和电路系统的角度进行了全面概述,介绍了喷墨打印、丝网印刷和转印印刷等印刷技术和基于印刷技术制备的有机数字电路(反相器、与非门、环形振荡器、D触发器),以及实现功能化的印刷电子应用(RFID、电子皮肤、OLED显示驱动背板等);最后,对本领域目前存在的问题和未来发展方向做了简要探讨。     

基于羧酸银的光敏热成像技术进展

最近10年,光敏热显影成像材料在技术上取得了重要进展,特别是以羧酸银作为银源的这类材料.这些进展集中体现在1995年为满足商品需要而研制成功的世界上第一个具有高分辨力、可作诊断使用的医用X射线胶片的Kodak DryView激光成像片上.此后,采用同样技术的一类特殊片种,即高反差的印刷胶片也随之问世.这些产品的实践应用都相当成功,已被多家公司所采用.这些新产品得益于三个方面的技术进展:改进成像层的照相性质、高影像质量和低成本的激光成像硬件,这也是此研究工作的焦点.在这类材料上所取得的重要成就反映在它们的高分辨力、高最大密度、低最小密度以及整张胶片性质的均一性上.所有这些优点,再加上超过100年的影像稳定性,使原来“老”的光敏热显影技术发生了一次脱胎换骨的变化,成为了当今最新的一种硬拷贝成像介质.     

纳米科技的发展对卤化银技术进步的影响

纳米科技和纳米材料在过去的十几年得到了迅速的发展,并将继续发展并渗透到各个领域,给世界和人类生活带来不可估量的影响.“纳米技术”真的是一个新的概念 ?事实上,某些材料的制备和使用早已经涉及了这个长度范围.卤化银照相技术就是“老”的纳米技术之一.在早期,从事卤化银照相的人们凭经验和有限的能力控制材料的某些结构在纳米级范畴.随着纳米科学的发展,纳米技术在卤化银照相领域的使用走过了从无意识到有目的的过程,促进了照相科学的发展.本论文将结合卤化银技术在 21世纪的发展趋势,从三个方面 (在纳米级研究卤化银照相、卤化银微晶上的纳米结构、纳米卤化银微粒)探讨纳米科学对卤化银技术进步的影响.     

方酸菁染料的合成

方酸菁染料业经证明具有光谱增感作用,但迄今未见其作为照相材料应用的报道.1973年法国Siegfried等将其用于巨脉冲红宝石激光的无源切换;最近Morel等又研究了它们在太阳能电池中的应用.作者合成了八个方酸菁染料,并对它们的照相性能和光电转换特性作了初步研究;发现其中的个别化合物不但具有良好的光谱增感作用,而且与照相工业中常用的染料“1833”相比,衰退也比较慢;部分化合物还表现出相当高的光电转换效率. 作者曾报道方酸的合成.本文介绍另一种方法,即以醋酸钠-醋酸环化1,1,3-三氯-2,     

Redox energetics and kinetics of uranyl coordination complexes in aqueous solution

Detailed voltammetric results for five uranyl coordination complexes are presented and analyzed using digital simulations of the voltammetric data to extract thermodynamic (E(1/2)) and heterogeneous electron-transfer kinetic (k(0) and alpha) parameters for the one-electron reduction of UO(2)(2+) to UO(2)(+). The complexes and their corresponding electrochemical parameters are the following: [UO(2)(OH(2))(5)](2+) (E(1/2) = -0.169 V vs Ag/AgCl, k(0) = 9.0 x 10(-3) cm/s, and alpha = 0.50); [UO(2)(OH)(5)](3-) (-0.927 V, 2.8 x 10(-3) cm/s, 0.46); [UO(2)(C(2)H(3)O(2))(3)](-) (-0.396 V, approximately 0.1 cm/s, approximately 0.5); [UO(2)(CO(3))(3)](4-) (-0.820 V, 2.6 x 10(-5) cm/s, 0.41); [UO(2)Cl(4)](2-) (-0.065 V, 9.2 x 10(-3) cm/s, 0.30). Differences in the E(1/2) values are attributable principally to differences in the basicity of the equatorial ligands. Differences in rate constants are considered within the context of Marcus theory of electron transfer, but no specific structural change(s) in the complexes between the two oxidation states can be uniquely identified with the underlying variability in the heterogeneous rate constants and electron-transfer coefficients.     

Controllable formation of nanoscale patterns on TiO2 by conductive-AFM nanolithography

We report on the nanopatterning of double-bond-terminated silane (5-hexenyltrichlorosilane, HTCS) molecules on titania (TiO2) using conductive atomic force microscopy (AFM). The influences of tip electrostatic potential and scanning velocity, relative humidity and of the repeated application of voltage on the topographic height, width, and hydrophilic and hydrophobic contrast of the resultant patterns were investigated. Tip voltage and tip velocity ( v) were applied between -10 V 相似文献   

Trace Determination of Zirconium（Ⅳ） by Anodic Adsorptive Voltammetry at a Carbon Paste Electrode

A new sensitive adsorptive voltammetric method was described for the determination ofzirconium at a carbon paste electrode (CPE) in the presence of alizarin complexone (ALC).Optimal analytical conditions are: 1.0~ l0“6 or 5.0x l0“7 mol/L ALC, 0.20 mol/L HAC-NaAc (pH4.3), accumulation for 60 s at 0 V (vs. SCE), and linear scanning from 0 V to 1.0 V at 250 mV/s.The peak potential of the complex is at 0.81 V. By using a model JP-303 polarographic analyzer,2.0~ l0l~ mol/L (S/N=3) zirconium can be detected with a 90 s accumulation, when the 2nd-orderderivative linear sweep technique is used, and the linear range is 6.0~ 10l~-2.0~ l0s mol/L (5.0~ l07mol/L ALC) and 2.0~108-2.0~ l07 mol/L (1.0~ 10.6 mol/L ALC), respectively. The developedmethod was applied to the determination of trace zirconium in the ore samples with satisfactoryresults.     

孔雀石绿增感聚苯乙炔的光导体

采用电位放电技术研究孔雀石绿（ＭＧ）增感顺式聚苯乙炔（ｃｔ－ＰＰＡ）光导体的光敏性，发现孔雀石绿是顺式聚苯乙炔新的有效增感剂。以Ａｌ／ｃｔ－ＰＰＡ：ＭＧ：ＰＣ（１００：５：１０）（１～１．５μｍ）／ＰＶＫ：ＴＰＡ：ＰＣ（１０：１０：１）（１５～２０μｍ）构成的光导体显示好的光敏性：表面接受电位，Ｖｍａｘ＞７００Ｖ；残余电位，Ｖｍｉｎ＜５０Ｖ；暗衰速率，ＲＤ＜１０Ｖ／ｓ；光衰放电量，△Ｖｔ＞５０％（１．０ｓ）；半衰时间，Ｔ１２＝０．８７Ｓ；感光灵敏度，Ｓ＝２．３×１０－３（１ｘ．ｓ）－１，较未增感ＰＰＡ光导体有较大的提高。ＭＧ对ＰＰＡ为光谱增感     

Model compound studies of the beta-O-4 linkage in lignin: absolute rate expressions for beta-scission of phenoxyl radical from 1-phenyl-2-phenoxyethanol-1-yl radical

Arrhenius rate expressions were determined for beta-scission of phenoxyl radical from 1-phenyl-2-phenoxyethanol-1-yl, PhC*(OH)CH2OPh (V). Ketyl radical V was competitively trapped by thiophenol to yield PhCH(OH)CH2OPh in competition with beta-scission to yield phenoxyl radical and acetophenone. A basis rate expression for hydrogen atom abstraction by sec-phenethyl alcohol, PhC*(OH)CH3, from thiophenol, log(k(abs)/M(-1) s(-1)) = (8.88 +/- 0.24) - (6.07 +/- 0.34)/theta, theta = 2.303RT, was determined by competing hydrogen atom abstraction with radical self-termination. Self-termination rates for PhC*(OH)CH3 were calculated using the Smoluchowski equation employing experimental diffusion coefficients of the parent alcohol, PhCH(OH)CH3, as a model for the radical. The hydrogen abstraction basis reaction was employed to determine the activation barrier for the beta-scission of phenoxyl from 1-phenyl-2-phenoxyethanol-1-yl (V): log(k beta)/s(-1)) = (12.85 +/- 0.22) - (15.06 +/- 0.38)/theta, k beta (298 K) ca. (64.0 s(-1) in benzene), and log(k beta /s(-1)) = (12.50 +/- 0.18) - (14.46 +/- 0.30)/theta, k beta (298 K) = 78.7 s(-1) in benzene containing 0.8 M 2-propanol. B3LYP/cc-PVTZ electronic structure calculations predict that intramolecular hydrogen bonding between the alpha-OH and the -OPh leaving group of ketyl radical (V) stabilizes both ground- and transition-state structures. The computed activation barrier, 14.9 kcal/mol, is in good agreement with the experimental activation barrier.     

Bithiophene-imide-based polymeric semiconductors for field-effect transistors: synthesis, structure-property correlations, charge carrier polarity, and device stability

Developing new high-mobility polymeric semiconductors with good processability and excellent device environmental stability is essential for organic electronics. We report the synthesis, characterization, manipulation of charge carrier polarity, and device air stability of a new series of bithiophene-imide (BTI)-based polymers for organic field-effect transistors (OFETs). By increasing the conjugation length of the donor comonomer unit from monothiophene (P1) to bithiophene (P2) to tetrathiophene (P3), the electron transport capacity decreases while the hole transport capacity increases. Compared to the BTI homopolymer P(BTimR) having an electron mobility of 10(-2) cm(2) V(-1) s(-1), copolymer P1 is ambipolar with balanced hole and electron mobilities of ～10(-4) cm(2) V(-1) s(-1), while P2 and P3 exhibit hole mobilities of ～10(-3) and ～10(-2) cm(2) V(-1) s(-1), respectively. The influence of P(BTimR) homopolymer M(n) on film morphology and device performance was also investigated. The high M(n) batch P(BTimR)-H affords more crystalline film microstructures; hence, 3× increased electron mobility (0.038 cm(2) V(-1) s(-1)) over the low M(n) one P(BTimR)-L (0.011 cm(2) V(-1) s(-1)). In a top-gate/bottom-contact OFET architecture, P(BTimR)-H achieves a high electron mobility of 0.14 cm(2) V(-1) s(-1), only slightly lower than that of state-of-the-art n-type polymer semiconductors. However, the high-lying P(BTimR)-H LUMO results in minimal electron transport on exposure to ambient. Copolymer P3 exhibits a hole mobility approaching 0.1 cm(2) V(-1) s(-1) in top-gate OFETs, comparable to or slightly lower than current state-of-the-art p-type polymer semiconductors (0.1-0.6 cm(2) V(-1) s(-1)). Although BTI building block incorporation does not enable air-stable n-type OFET performance for P(BTimR) or P1, it significantly increases the OFET air stability for p-type P2 and P3. Bottom-gate/top-contact and top-gate/bottom-contact P2 and P3 OFETs exhibit excellent stability in the ambient. Thus, P2 and P3 OFET hole mobilities are almost unchanged after 200 days under ambient, which is attributed to their low-lying HOMOs (>0.2 eV lower than that of P3HT), induced by the strong BTI electron-withdrawing capacity. Complementary inverters were fabricated by inkjet patterning of P(BTimR)-H (n-type) and P3b (p-type).     

Cooperative ligation,back-bonding,and possible pyridine-pyridine interactions in tetrapyridine-vanadium(II): a visible and X-ray spectroscopic study

The binding of pyridine by V(II) in aqueous solution shows evidence for the late onset of cooperativity. The K(1) governing formation of [V(py)](2+) (lambda(max) = 404 nm, epsilon(max) = 1.43 +/- 0.3 M(-1) cm(-1)) was determined spectrophotometrically to be 11.0 +/- 0.3 M(-)(1), while K(1) for isonicotinamide was found to be 5.0 +/- 0.1 M(-1). These values are in the low range for 3d M(2+) ions and indicate that V(II).py back-bonding is not significant in the formation of the 1:1 complex. Titration of 10.5 mM V(II) with pyridine in aqueous solution showed an absorption plateau at about 1 M added pyridine, indicating a reaction terminus. Vanadium K-edge EXAFS analysis of 63 mM V(II) in 2 M pyridine solution revealed six first-shell N/O ligands at 2.14 A and 4 +/- 1 pyridine ligands per V(II). UV/vis absorption spectroscopy indicated that the same terminal V(II) species was present in both experiments. Model calculations showed that in the absence of back-bonding only 2.0 +/- 0.2 and 2.4 +/- 0.2 pyridine ligands would be present, respectively. Cooperativity in multistage binding of pyridine by [V(aq)](2+) is thus indicated. XAS K-edge spectroscopy of crystalline [V(O(3)SCF(3))(2)(py)(4)] and of V(II) in 2 M pyridine solution each exhibited the analogous 1s --> (5)E(g) and 1s --> (5)T(2g) transitions, at 5465.5 and 5467.5 eV, and 5465.2 and 5467.4 eV, respectively, consistent with the EXAFS analysis. In contrast, [V(py)(6)](PF(6))(2) and [V(H(2)O)(6)]SO(4) show four 1s --> 3d XAS transitions suggestive of a Jahn-Teller distorted excited state. Comparison of the M(II)[bond]N(py) bond lengths in V(II) and Fe(II) tetrapyridines shows that the V(II)[bond]N(py) distances are about 0.06 A shorter than predicted from ionic radii. For [VX(2)(R-py)(4)] (X = Cl(-), CF(3)SO(3)(-); R = 4-Et, H, 3-EtOOC), the E(1/2) values of the V(II)/V(III) couples correlate linearly with the Hammett sigma values of the R group. These findings indicate that pi back-bonding is important in [V(py)(4)](2+) even though absent in [V(py)](2+). The paramagnetism of [V(O(3)SCF(3))(2)(py)(4)] in CHCl(3), 3.8 +/- 0.2 mu(B), revealed that the onset of back-bonding is not accompanied by a spin change. Analysis of the geometries of V(II) and Fe(II) tetrapyridines indicates that the ubiquitous propeller motif accompanying tetrapyridine ligation may be due to eight dipole interactions arising from the juxtaposed C-H edges and pi clouds of adjoining ligands, worth about -6 kJ each. However, this is not the source of the cooperativity in the binding of multiple pyridines by V(II) because the same interactions are present in the Fe(II)-tetrapyridines, which do not show cooperative ligand binding. Cooperativity in the binding of pyridine by V(II) is then assigned by default to V(II)-pyridine back-bonding, which emerges only after the first pyridine is bound.     

硫在疏质子介质中电化学还原机理的研究 II: 第二步氧化还原过程的研究

用电化学方法研究了硫在DMSO溶剂中的第二步氧化还原过程. 该过程在扫速大于200mV/s时表现为简单的电子转移过程; 扫速小于200mV/s时转化为ECE机理. 发现了S8^4^-, S3^2^-, S4^2^-的氧化峰, 峰电位分别为 -1.50, -0.96, -0.60(相对于银参比电极), 对S8^2^-/S8^4^-电对测定了标准电极电位和标准速率常数, 分别是-1.547±0.002V(相对于银参比电极)和3.3×10^-^3cm/s.     

Programmable gate delayed ion mobility spectrometry-mass spectrometry: a study with low concentrations of dipropylene-glycol-monomethyl-ether in air

The concept of using a short ionisation event, in this case a pulsed corona discharge, in conjunction with programmed gate delay is described. This technique is proposed for the selective study of different ionisation processes within the reaction region of an ion mobility spectrometer. The utility of such an approach was tested in a study of the ionisation of dipropylene-glycol-monomethyl-ether (DPM); a compound commonly used to test the operation of ion mobility spectrometers. Dipropylene-glycol-monomethyl-ether at a concentration of 113 microg m(-3) in air, with a water level of 75 mg m(-3) in air, was analysed using a switchable, high resolution ion mobility spectrometer, operating in the positive mode at 40 degrees C at ambient pressure. The ion mobility spectrometer was fitted with a pulsed corona discharge ionisation source, doped with ammonia at a concentration of 1.3 mg m(-3) in the reaction region, and interfaced to a mass spectrometer. Synchronisation of the ionisation event to the operation of the shutter grids for the drift region enabled different parts of the product ion population to be injected into the drift tube, and programming the gate delays produced a map of the gate delay verses drift time response surface. Ammonium bound dipropylene-glycol-monomethyl-ether was observed, [(DPM)NH4]+ (m/z 166) as well as the ammonium bound dimer [(DPM)2NH4]+ (m/z 314), the same as those observed with a 63Ni source. Two other species were also observed, but their molecular identity was not elucidated. One of them m/z 146, also observed with 63Ni, formed ammonium bound ions [(m/z 146)NH4]+ (K0= 1.49 cm2 V(-1) s(-1)), ammonium bound dimer ions [(m/z 146)2NH4]+(K0= 1.18 cm2 V(-1) s(-1)) and a mixed cluster ion with DPM [(m/z 146)(DPM)NH4]+(K0= 1.18 cm2 V(-1) s(-1)); while the other, m/z 88 a decomposition product, formed ammonium bound monomer [(m/z 88)NH4]+(K0= 1.68 cm2 V(-1) s(-1)), dimer ions [(m/z 88)2NH4]+(K0= 1.40 cm2 V(-1) s(-1)) and a mixed cluster ion containing DPM and ammonium, [(DPM)(m/z 88)2NH4]+(K0= 1.40 cm2 V(-1) s(-1)). The assignment of responses to these ions required the additional dimensionality in the data provided from the gate delay studies. The relationships evident in the programmable gate delay data enabled these ions to be differentiated from alternative assignments of possible nitrogen clusters, formed at the interface of the mass spectrometer.     

高效毛细管电泳分析羊栖菜多糖对肿瘤机体红细胞合淌度的影响

为了分析羊栖菜多糖（SFPS）对肿瘤机体红细胞合淌度的影响,建立了肿瘤动物模型,分高、中、低剂量腹腔给予羊栖菜多糖7 d,采集并制备红细胞悬液,应用高效毛细管电泳法检测红细胞的合淌度。实验条件:毛细管为75 μm×50 cm,电泳缓冲液为含2 g/L羟丙基甲基纤维素的磷酸盐溶液(0.1 mol/L,pH 7.4),压力进样为3.448 kPa×10 s,分离电压为20 kV,柱温为25 ℃,电渗淌度为2.16×10-4 cm2·V-1·s-1。实验结果表明：羊栖菜多糖能降低肿瘤机体红细胞的电泳迁移时间(阴性对照组为15.76 min,SFPS低剂量组为13.96 min,SFPS中剂量组为12.90 min,SFPS高剂量组为13.51 min,正常对照组为11.51 min),增加红细胞的合淌度(阴性对照组为1.06×10-4 cm2·V-1·s-1,SFPS低剂量组为1.19×10-4 cm2·V-1·s-1,SFPS中剂量组为1.29×10-4 cm2·V-1·s-1,SFPS高剂量组为1.23×10-4 cm2·V-1·s-1,正常对照组为1.45×10-4 cm2·V-1·s-1),SFPS 3个剂量组红细胞的合淌度与阴性对照组比较均有非常显著的差异(P＜0.01)。羊栖菜多糖能够改变肿瘤机体红细胞的合淌度,并使之趋向于正常机体水平,这可能与其改变红细胞表面的电荷密度有关。高效毛细管电泳法可以作为检测红细胞生理状态和功能的一种辅助工具。