窄带隙二噻吩并吡咯共聚物合成与光伏性能研究

二噻吩[3,2-b:2′,3′-d]并吡咯(Dithieno[3,2-b:2′,3′-d]pyrrole,DTP)分别与3种受体单元聚合得到聚合物P1~P3,受体单元分别为:吡咯并吡咯二酮(DPP)、二噻吩苯并噁二唑(DTBO)和喹喔啉衍生物(TQ).研究表明,3种聚合物都有较窄的带隙(P1:1.23 e V,P2:1.51 e V,P3:1.50 e V),有利于活性层材料对太阳光的吸收,其中P1获得了最宽的吸收(近1000 nm).将P1~P3与PC71BM共混制备光伏器件,当给受体比例为1∶3时,基于P1的光伏器件短路电流密度(short-circuit current density,JSC)为15.82 m A/cm~2,开路电压(open-circuit voltage,VOC)为0.38 V,能量转化效率(power conversion efficiency,PCE)达到3.33%,为3种聚合物中最高的效率.对于聚合物P2和P3,在给受体比例为1∶2时,光伏性能最好,此时P2与P3的PCE值分别为1.20%和1.37%,导致较低光电转换效率的因素是短路电流密度JSC(P2:9.70 m A/cm~2,P3:9.21 m A/cm~2)和开路电压VOC(约0.3 V)过低.     

三氟甲基取代Ir配合物的电子结构和磷光性质的理论研究

采用密度泛函理论m PW1PW91方法研究了三氟甲基(CF3)基团修饰的一类Ir磷光材料,即Ir(C∧C)(ppy)2、Ir(C∧C)(ppy)(Ort CF3)、Ir(C∧C)(ppy)(Me CF3)和Ir(C∧C)(ppy)(Par CF3)[(C∧C:3-甲基-1-(2,4-甲基苯)-1H-咪唑;ppy:2-苯基吡啶,Ort CF3=2-(2-(三氟甲基)苯基)吡啶;Me CF3:2-(3-(三氟甲基)苯基)吡啶;Par CF3:2-(4-(三氟甲基)苯基)吡啶]的电子结构和光学性质.理论计算得到Ir(C∧C)(ppy)2的电子结构、吸收光谱和磷光光谱与实验结果吻合得较好.通过与实验分子Ir(C∧C)(ppy)2对比,向ppy的邻位和对位引入CF3基团加强金属和配体之间的作用力,提高空穴和电子注入能力,吸收和磷光发射光谱发生红移.尤其,Ir(C∧C)(ppy)-(Ort CF3)比其他配合物在发射磷光时金属到配体的电荷转移(3MLCT)的贡献大、跃迁偶极矩(μS1)大、d轨道能级分裂大,并且单三重态分裂能(ΔES1-T1)小,这表明设计的分子Ir(C∧C)(ppy)(Ort CF3)有望成为好的磷光发光材料.     

六氟磷酸二(2-苯基吡啶)(2,2'-联噻唑)合铱(Ⅲ)的合成及在中性/暖白光二极管中的应用

以Ir Cl_3·3H_2O为铱(Ⅲ)源,2-苯基吡啶(ppy)为主配体,2,2'-联噻唑(btz)为辅助配体在乙二醇中回流反应后,再与NH_4PF_6水溶液进行离子交换反应,制得新颖橙光阳离子型有机铱(Ⅲ)配合物[(ppy)_2Ir·(btz)]PF_6.将其掺杂到硅树脂中用于Ga N蓝光(455 nm)芯片激发Y_3Al_5O_(12)∶Ce~(3+)(YAG∶Ce,以6.0%质量比掺杂于硅树脂中)构成的白光二极管时,白光色温明显降低.未掺杂[(ppy)_2Ir(btz)]PF_6时,白光色温为7133 K(冷白光),效率为137.1 lm/W,显色指数为79.9,色坐标为(0.31,0.31).当分别掺入1.0%,1.5%和2.0%的[(ppy)_2Ir(btz)]PF_6时,色温依次降为5645 K(冷白光)、4072 K(中性白光)和3161 K(暖白光),效率则分别为102.1,79.1和66.6 lm/W,显色指数分别为81.9,77.3和70.0,色坐标分别为(0.33,0.31),(0.36,0.33)和(0.42,0.38).实验结果表明,[(ppy)_2Ir(btz)]PF_6是一种可用于中性/暖白光LEDs的高效橙光材料.     

利用静电吸引作用提高光催化放氢效率

本文设计合成了两个分别带正电荷和负电荷的Ir(Ⅲ)配合物[Ir(ppy)₂(bpy)]⁺(ppy=2-苯基吡啶,bpy=2,2′-联吡啶)和[Ir(ppy)₂(pbs)]^-(pbs=1,10-菲啰啉-4,7-二苯磺酸钠)作为光敏剂,以[Co(bpy)₃]²⁺为放氢催化剂,比较了Ir(Ⅲ)配合物的光催化放氢效率.发现带负电荷的Ir(Ⅲ)配合物具有更高的光催化放氢效率,带负电荷光敏剂和带正电荷催化剂间的静电吸引可能对放氢效率的提高起到了重要作用.     

室温磷光材料二(2-苯基吡啶)(2-(2-吡啶)苯并咪唑)合铱(III)的合成及光电特性

以2-苯基吡啶(ppy)为主配体, 2-(2-吡啶)苯并咪唑(pybiH)为辅助配体合成了一种室温蓝绿色磷光发射材料二(2-苯基吡啶)( 2-(2-吡啶)苯并咪唑)合铱(III) ((ppy)₂Ir(pybi)), 通过傅里叶变换红外(FTIR)光谱、核磁共振氢谱(1H NMR)、质谱(MS)、元素分析对其结构进行了表征. 利用紫外-可见吸收光谱、荧光激发和发射光谱、循环伏安曲线, 结合含时密度泛函理论(TD-DFT)模拟计算研究了(ppy)₂Ir(pybi)的光物理特性及能级结构, 并研究了其电致发光性能. (ppy)₂Ir(pybi)的紫外吸收峰分别位于250, 295, 346和442 nm, 与理论模拟计算吻合得很好;(ppy)₂Ir(pybi)为蓝绿光发射, 发光峰分别位于495 和518 nm; (ppy)₂Ir(pybi) 的最高占据轨道(HOMO)和最低空轨道(LUMO)能级分别为-6.11和-3.43 eV, 光学带隙为2.68 eV; 以(ppy)₂Ir(pybi)为掺杂剂, 4,4'-N,N'-二咔唑基联苯(CBP)为主体材料, 制备电致磷光器件, 电致发射峰位于508 nm, 最大亮度为8451 cd·m^-2, 最大电流效率为17.6 cd·A^-1. 这些研究为(ppy)₂Ir(pybi)在有机电致发光领域的应用提供实验依据.     

位移谐振子模型对三(2-苯基吡啶)合铱磷光光谱影响的理论研究

采用谐振子模型理论探讨了振动模式对Ir(ppy)₃配合物的磷光光谱的影响.多原子分子发射光谱的一般形式可以从两个绝热电子态之间的热振动关联函数推导出,相应地势能面之间的位移和Duschinsky转动的影响也被包含在多维谐振子模型的表达式中,所得关系式模拟出了Ir(ppy)₃较为精细的磷光发射光谱.计算结果表明T₁态到S₀态之间的0→1振动跃迁对发射光谱贡献较大,尤其振动频率小于1600 cm^-1的振动模贡献更多,配体中苯和吡啶环上C=C和C=N的呼吸振动,是Ir(ppy)₃出现肩峰的主要原因.玻耳兹曼分布使得主峰和肩峰的强度下降,并且两峰相互接近.该谐振子模型与密度泛函理论(DFT)结合,可以较好地定量描述多原子分子光物理过程的发射光谱以及详细了解光谱谱图的细节.     

聚合物掺杂的高亮度磷光有机电致发光器件

采用新型贵金属铱的配合物(pbi)2Ir(acac)作为客体磷光发光材料, 分别以4%和5%(w)的浓度掺杂于聚合物主体材料poly(N-vinylcarbazole) (PVK)中, 利用旋涂工艺制备了结构为indium-tin oxide (ITO)/PVK:(pbi)2Ir(acac)/2,9-二甲基-4,7-二苯基-1,10-菲咯啉(BCP)/Mg:Ag的有机电致发光器件, 对磷光材料(pbi)2Ir(acac)的紫外-可见吸收光谱﹑光致发光光谱以及聚合物掺杂的磷光器件的电致发光特性进行了研究. 结果表明, 两种掺杂浓度的器件均具有8 V左右的启亮电压, 器件在启亮后的最大流明效率分别为1.53和1.31 lm·W-1, 最大亮度分别为11210和9174 cd·m-2; 同时, 器件的电致发光光谱与色坐标均不随偏置电压和客体掺杂浓度的变化而改变, 具有稳定的色纯度. 分析了主体材料PVK到磷光客体(pbi)2Ir(acac)的能量转移机制, 并探讨了随着器件电流密度和客体掺杂浓度的逐渐增加, 器件流明效率的变化趋势.     

磷光客体三重态能级对基于PVK主体的电致发光器件的影响

将磷光客体掺入PVK:PBD主体材料中是获得高效率磷光电致发光器件 (PhPLED)的有效途径.然而,分别掺杂Ir(pppy)₃、Ir(F-pppy)₃和Ir(F₂-pppy)₃三种磷光客体的PhPLED器件性能件却显著不同.我们分别模拟主-客体间能量转移和客体直接捕获电子空穴对两种机制,研究了三种客体材料的磷光发射及其衰减过程.研究表明:平衡的载流子注入和客体高效率的载流子捕获是实现Ir-配合物掺杂的PhPLED器件性能优良的主要机制,PVK较低的三重态能级使其无法成为蓝光磷光电致发光器件的主体,在PVK中掺入PBD的方法,则进一步降低了主体材料的三重态能级,这是蓝光磷光电致发光器件运行效率较低的主要原因.本文的研究结果可为高分子磷光电致发光器件的制备技术和新型磷光主体的设计提供参考.     

铱配合物的电致化学发光性能研究

结构相关的铱配合物[Ir(ppy)2L1](PF6)和[Ir(ppy)2L2](PF6)(ppy=2-苯基吡啶,LI=4-(2,2'-联吡啶-3-乙炔基)-N-(吡啶-2-亚甲基)-N-(噻吩-3-亚甲基)苯胺,L2=4-(2,2'-联吡-3-乙炔基)-N-二(吡啶-2-亚甲基)-苯胺)都具有优良的电致发光(ECL)性...     

新型酰胺功能化铱[III]配合物的光电性能

设计并制备三种具不同官能团的铱[III]邻菲啰啉配合物: [Ir(ppy)₂phen-Br]Cl, [Ir(ppy)₂phen-COOH]Cl, [Ir(ppy)₂phen-Si]Cl,以及对比参照物[Ir(ppy)₂phen-NH₂]Cl.其中, ppy为2-苯基吡啶, phen-Br为2-溴-2甲基-N-(1, 10-菲啰啉-5-基)丙酰胺, phen-COOH为4-[(1, 10-菲啰啉-5-基)氨基]-4-酰基丁烯酸, phen-Si为5-[N, N-二-3-(三乙氧硅)基]酰亚胺-1, 10-菲啰啉, phen-NH₂为5-氨基-邻菲啰啉,并采用核磁共振(NMR)、质谱(MS)、紫外-可见(UV-Vis)吸收光谱、荧光(PL)光谱法和循环伏安法(CV)等对上述配合物进行了分析和表征.光物理性能研究结果表明:这些配合物在蓝-紫色可见光区域有较强吸收,可发射出明亮的黄色到橙红色荧光,量子效率达到12%以上.相比较于参照物[Ir(ppy)₂phen-NH₂]Cl (5.78 μs),三种新型配合物在量子效率未明显降低甚至提高的前提下,荧光寿命有了显著的提高(9.18-12.00 μs).其中, [Ir(ppy)₂phen-Br]Cl (1)不但有最高的荧光量子产率(32%)和最长的荧光寿命(12.00 μs),而且也具有最好的氧传感性能, I₀/I (无氧与纯氧条件下的荧光强度比值)可达到10.91.这使得[Ir(ppy)₂phen-Br]Cl有望成为接枝型,较高性能的光学氧传感器的候选氧敏指示剂.除此之外,还通过含时密度泛函理论(TD-DFT)计算对配合物光电性能进行补充说明,理论计算表明:这些配合物是以铱为中心的近似八面体结构,理论计算结果与实际实验数据相一致.     

势能面移动对三（2-苯基吡啶）合铱磷光光谱影响的理论研究

采用密度泛函理论及赝势基组对三（2-苯基吡啶）合铱（Ir（ppy）3）的基态及三重态结构进行优化,并分析了这两个态各自的振动模式,在此基础上计算了电子从三重态跃迁回基态的势能面移动,得到了该过程的重整能．由于0→1跃迁对Ir（ppy）s的磷光光谱有重要影响,我们利用Frank-Condon因子与势能面移动的联系,在给定的半高宽下,计算并得到了Ir（ppy）3的磷光光谱,结果与实验吻合较好．     

分级微纳结构TiO2空心球的制备及其在DSSC中的应用

以钛酸四丁酯为钛源,无水乙醇为溶剂,通过碳球模板法制备出直径为200nm、壳厚20～25nm的TiO2空心球（HS）.通过X射线衍射（XRD）、透射电子显微镜（TEM）、扫描电子显微镜（SEM）和N2吸附脱附等对产物的形貌、晶相组成、孔结构和紫外-可见光谱性质进行了表征,结果显示所制备的锐钛矿相TiO2空心微球是由初级结构纳米级TiO2晶粒构成的.将这种TiO2空心球应用于染料敏化太阳电池（DSSC）领域可以提高光阳极对光的散射.通过制备P25/HS-TiO2双层膜电极,相比单纯的P25纳米晶电极（Jsc=13.5mAcm？2,Voc=0.653V,FF=0.53,η=4.95%）可以得到更高的光电转化效率（Jsc=15.79mAcm？2,Voc=0.653V,FF=0.55,η=6.66%）.     

N,N-二苯基取代的芳炔化合物的合成及光伏性能

以简单原料出发,通过Sonogashira偶联反应和三甲基硅基(TMS)的保护与脱保护,合成了一系列N,N-二苯基取代的芳炔化合物SC1～SC5.这类化合物是以N,N-二苯基为电子给体,羧基为电子受体,芳香炔体系为共轭桥的染料.将化合物SC5吸附到TiO2膜上制备成有机染料敏化太阳能电池,在AM 1.5,100 mW/cm2的模拟太阳光下,电池的光电转换效率(IPCE)值最大达到64%,而且在350～580 nm的范围内都可达到50%以上.电池的短路电流密度Jsc=8.0mW/cm2,开路电压Voc=0.75 V,填充因子为FF=0.70,总光电转换效率η=4.2%.     

Efficient eosin y dye-sensitized solar cell containing Br-/Br3- electrolyte

We found that Br-/Br3- is more suitable than an I-/I3- couple in dye-sensitized solar cells in terms of higher open-circuit photovoltage (Voc) production and higher overall energy conversion efficiency (eta) if the dye sensitizer has a more positive potential than that of Br-/Br3-. Under simulated AM1.5 one sun, an eosin Y dye-sensitized solar cell containing 0.4 M LiBr + 0.04 M Br2 electrolyte in acetonitrile yielded a short-circuit photocurrent (Jsc) of 4.63 mA cm(-2), Voc of 0.813 V, and fill factor (FF) of 0.693, corresponding to 2.61% of eta. Under the same conditions except for the electrolyte 0.4 M LiI + 0.04 M I2 in acetonitrile instead, the device produced 1.67% of eta (Jsc = 5.15 mA cm(-2), Voc = 0.451 V, FF = 0.721). Replacement of I-/I3- with Br-/Br3- in eosin Y dye-sensitized solar cells yielded a significant increase in Voc offset by slight decreases in Jsc and FF, leading to an increase in eta by 56%. The significant gain in Voc was attributed to the enlarged energy level difference between the redox potential of the electrolyte and the Fermi level of TiO2 and the suppressed charge recombination as well. The rate for charge recombination between bromine and the injected electrons was determined to be first order in bromine.     

Hybrid solar cells constructed of macroporous n-type GaP coated with PEDOT:PSS

Hybrid organic–inorganic solar cell devices were fabricated utilizing macroporous n-type Ga P and poly(3,4-ethylenedioxythiophene):poly(4-styrene sulfonate)(PEDOT:PSS).The high-aspect ratio structures of the macroporous Ga P resulted in higher photocurrent and external quantum yield as a function of wavelength.Photocurrent–voltage measurements as a function of light intensity revealed information on the dependence of short-circuit current(Jsc) and open-circuit voltage(Voc) on light intensity.Under 1.0 Sun illumination,hybrid macroporous Ga P/PEDOT:PSS devices showed Jscof2.34 m A cmà2,Vocof 0.95 V,fill factor of 0.54,and overall efficiency of 1.21%.The extent of the influence of dopant density of Ga P on hybrid device performance was probed with current density–voltage measurements.The addition of a gold nanoparticle coating on macroporous Ga P prior to PEDOT:PSS coating showed increased device performance,with overall efficiency of 1.81%.Gold-modified planar Ga P/PEDOT:PSS showed decreased Jscand Vocvalues and lower external quantum yield over all wavelengths.     

Structural tuning of low band gap intermolecular push/pull side-chain polymers for organic photovoltaic applications

A series of novel low band gap donor-acceptor (D-A) type organic co-polymers (BT-F-TPA,BT-CZ-TPA and BT-SI-TPA) consisting of electron-deficient acceptor blocks both in main chains (M1) and at the pendant (M2) were polymerized with different electron rich donor (M3-M5) blocks,i.e.,9,9-dihexyl-9H-fluorene,N-alkyl-2,7-carbazole,and 2,6-dithinosilole,respectively,via Suzuki method.These polymers exhibited relatively low band gaps (1.65-1.88 eV) and broad absorption ranges (680-740 nm).Bulk heterojunction (BHJ) solar cells incorporating these polymers as electron donors,blended with [6,6]-phenyl-C61-butyric acid methyl ester (PC61BM) or [6,6]-phenyl-C71-butyric acid methyl ester (PC71BM) as electron-acceptors in different weight ratios were fabricated and tested under 100 mW/cm2 of AM 1.5 with white-light illumination.The photovoltaic device containing donor BT-SI-TPA and acceptor PC71BM in 1:2 weight ratio showed the best power conversion efficiency (PCE) value of 1.88％,with open circuit voltage (Voc) =0.75 V,short circuit current density (Jsc) =7.60 mA/cm2,and fill factor (FF) =33.0％.     

以5-取代-8-羟基喹啉和2-苯基吡啶为配体的金属铱配合物的合成、表征及光致、电致发光性质

本文通过在8-羟基喹啉的5位上引入氨基和取代的苯基,合成了系列二-[2-苯基吡啶（C^N）][5-取代-8-羟基喹啉（N^O）]铱（Ⅲ）配合物（（C^N）2IrQ）.这里CN代表2-苯基吡啶,Q代表5-取代-8-羟基喹啉.通过1HNMR、13CNMR、MS、元素分析、单晶X-衍射等对配合物的化学和晶体结构进行了表征.利用循环伏安、UV-Vis、光致和电致发光光谱等对它们的光物理性质进行了表征.热重分析表明苯环上的取代基对配合物热稳定性有很大影响.常温下,几种5-取代苯基喹啉铱配合物的溶液和固体产生红色磷光发射,光致发光（PL）光谱在666和687nm附近出现两个强度基本相等的发射峰.配合物的发光性质主要受喹啉环和5位苯基的影响,苯环上的取代基团对配合物的发光性质影响不大.而5-氨基喹啉铱配合物PL光谱的最大发射峰在550nm,其PL光谱主要受2-苯基吡啶的影响.将配合物二-[2-苯基吡啶（C^N）][5-（4-甲氧基苯基）-8-羟基喹啉（N^O）]铱（Ⅲ）（7b）掺杂在聚2,7-（9,9-二辛基）芴（PFO）和30%（质量分数）的2-对叔丁基苯基-5-对联苯基-1,3,4-口恶二唑（PBD）的主体材料中,制备了聚合物发光器件（OLED）,器件电致发光（EL）光谱的发射峰在672nm处,18V时最大亮度为350cd/m2,在电压14V时CIE色坐标值为（0.61,0.33）,是一红光OLED器件.     

Cyclometallated iridium(III) complexes with substituted 1,10-phenanthrolines: a new class of highly active organometallic second order NLO-phores with excellent transparency with respect to second harmonic emission

[Ir(ppy)(2)(5-R-1,10-phen)][PF(6)] (ppy = cyclometallated 2-phenylpyridine, phen = phenanthroline, R = H, Me, NMe(2), NO(2)) and [Ir(ppy)(2)(4-R',7-R'-1,10-phen)][PF(6)] (R' = Me, Ph) complexes are characterized by one of the highest second order NLO response (measured by the EFISH technique) reported for a metal complex, mainly due (as suggested by a theoretical SOS-TDDFT investigation) to MLCT processes from the ppy-Ir based moiety acting as donor push system to pi* orbitals of phen, acting as an acceptor pull system; the good transparency to the second harmonic emission renders these NLO-phores appealing as building blocks for molecular materials with second harmonic generation.     

High‐efficiency organic electroluminescent devices using iridium complex emitter and arylamine‐containing polymer buffer layer

We have developed efficient organic electroluminescent (EL) devices using a phosphorescent material, tris(2‐phenylpyridine) iridium, Ir(ppy)₃, as an emitter material and a polymer buffer layer, tetraphenyldiamine‐containing poly(arylene ether sulfone) (PTPDES) doped with tris(4‐bromophenyl) aminium hexachloroantimonate (TBPAH) as an electron acceptor. In this device, a high external quantum efficiency of 21.6% and a luminous efficiency of 82 lm/W (77 cd/A) at 3.0 V were obtained. These high efficiencies can be explained by high quantum efficiency due to phosphorescent Ir(ppy)₃ and high luminous efficiency realized by the use of the polymer buffer layer. Copyright © 2002 John Wiley & Sons, Ltd.     

Excitation energy migration in oligo(p-phenylenevinylene) based organogels: structure-property relationship and FRET efficiency

Excitation energy migration (EM) and assisted energy transfer (ET) properties of a few oligo(p-phenylenevinylene) (OPV) based organogelators with different end functional groups have been studied using picosecond time-resolved emission spectroscopy (TRES). EM was found to be more efficient in OPV gelators with small end functional groups (OPV3-4) when compared to that of the gelators with bulky end groups (OPV1-2) in the gel state. TRES studies at elevated temperature and in chloroform solution highlight the role of the self-assembled scaffolds in assisting the EM and ET processes. Increase in temperature and solvent polarity leads to the aggregate breaking and hence adversely affects the EM and ET efficiencies. The effect of EM efficiency on the fluorescence resonance energy transfer (FRET) properties of the OPV gels was studied by using OPV1 and OPV3 as the donors and OPV5 as the acceptor. Better transfer of excitation energy was observed in the donor system (OPV3) having higher EM efficiency even at very low concentration (3.1 mol%) of the acceptor molecules, whereas ET efficiency was lower in the donor system (OPV1) with low EM efficiency.