聚磷氮烯及其衍生物电子结构的理论研究

用分子轨道和晶体轨道方法,对聚磷氮烯及其衍生物的电子结构进行了研究,以期更深入地了解聚磷氮烯的结构和性能.研究发现,链状聚磷氮烯和环状三聚磷氮烯为平面结构,其它的环状聚磷氮烯则为巢式结构,吸电子基团取代有使环状聚磷氮烯主链环取平面结构的倾向.研究还发现,无论是链状还是环状聚磷氮烯,都表现为半导体.取代基效应表明,吸电子基团-F和-CN的取代,使聚合物的电子亲和势(EA)和电离能(IP)均增大,能隙减小,给电子基团-CH₃和-OCH₃的取代,使聚合物的IP减少;吸电子基团取代有利于n-型掺杂,给电子基团取代有利于p-型掺杂,但都不改变其半导体的特性.     

聚茚并茚及其取代衍生物的理论研究

用子洽场全略微分晶体轨道法对聚茚并茚及其取代衍生物的电子结构进行了计算研究,探讨了取代基效应。计算得到聚茚并茚及其取代物是一类具有较低带隙的半导体。取代基效应表明,吸电子基团的取代使聚合物的电子亲和势增大,而给电子基团的取代则导致电离势减小,但取代基效应不能改变聚合物的半导体性质。     

共轭CN与非共轭CF3吸电子取代基对PPV类衍生物分子结构及光电性质的影响

运用密度泛函DFT B3LYP／6-31G(d)方法对CN和CF3吸电子基团取代的PPV类衍生物的三聚体进行了几何构型优化，并采用含时密度泛函TD-DFT、B3LYP／6-31G(d)方法计算了其相应化合物的紫外吸收光谱．通过对CN和CF3取代的PPV类衍生物的分子几何结构、前线分子轨道能级、电子云分布规律的分析，从理论上解释了共轭CN与非共轭CF3吸电子取代基对其光谱性质影响的差异：前者使相应PPV类衍生物的吸收光谱发生红移，后者则发生蓝移．计算结果还表明用TD-DFT方法计算该体系的紫外吸收光谱值与实验数据吻合得很好；另外引入CN和CF3基团之后，使其相应的PPV衍生物的LUMO能级降低，电子亲合势增加，都是很好的电子传输材料．     

推/拉电子取代基对PCBM结构及光谱性质影响的理论研究

应用密度泛函理论(DFT)方法计算[6,6]-苯基-C₆₁-丁酸甲酯(PCBM)及其苯环对位取代得到的4种衍生物的几何和电子结构. 采用第一激发能校正了分子的最低未占据分子轨道(LUMO)能级, 探讨了推/拉电子基团对分子前线轨道的影响. 在全优化几何构型的基础上, 采用含时密度泛函理论(TD-DFT)方法研究了电子吸收光谱特征和电荷转移态性质, 并讨论了推/拉电子基团对体系电子吸收光谱性质的影响. 通过对重组能和电子亲和势的计算, 预测了PCBM与4种衍生物的电子能力及电子迁移率大小的关系. 结果表明, 在PCBM中, 在苯环的对位引入推电子基团可以提高分子的前线轨道能级, 改变前线轨道电子云分布, 明显增强可见光范围内的吸收强度, 增加可见光范围内的电荷转移吸收, 且激发态的电荷转移随着引入基团推电子能力的增加而增强. 化合物5的激发态分子内电荷转移性质最强, 且具有较独特的光伏性质. 而在同样位置引入拉电子基团, 则降低了分子前线轨道能级对电子吸收光谱的影响.     

用于监控过氧化氮的近红外荧光探针的光物理性质及PET机理

含有机硒的七甲川菁染料是基于光诱导电子转移(PET)的近红外(IR)荧光探针, 能在生理条件下高灵敏、高选择性地监控过氧化氮. 本文应用含时密度泛函理论(TD-DFT)计算方法研究其光物理性质和PET机理.结果表明, 在激发态, 荧光母体发生最高占有分子轨道(HOMO)到最低非占有分子轨道(LUMO)的电子跃迁, 识别基团上的HOMO轨道能级提高到荧光母体的单电子占据的HOMO轨道能级之上, 并向其转移一个电子, 使激发态电子回落过程受阻而导致荧光部分淬灭. 硒被氧化后, 识别基团上的HOMO轨道能级降低, PET过程被阻断, 荧光发射恢复. 研究进一步证明, PET效应来自于识别基团上苯胺N原子的p电子, 它的电子转移能力受到其对位苯硒基的氧化-还原状态的影响, 产生了荧光信号的“开-关”作用.     

环状聚茚并茚及其取代衍生物电子结构和磁性研究

采用半经验的AM1法，对环状聚茚并茚及其取代物的电子结构进行了计算研究 ，探讨了其磁性和取代基效应．计算得到，环状聚茚并茚及其取代物皆表现半导体 性质且发现其中一种异构体可能具有磁性．取代基效应表明，吸电子基团的取代使 聚合物的电子亲合势增大，而给电子基团的取代则导致电离势减少，但取代基效应 不能改变聚合物的半导体性质．此外，无论吸电子基团还是给电子基团的取代都不 能改变聚合物的磁性特征．     

氟硼二吡咯类pH荧光探针PET光谱特性的理论计算

氟硼二吡咯(BODIPY)类pH荧光探针分子是基于光诱导电子转移(PET)的荧光探针分子, 识别基团氮原子上引入不同取代基可呈现不同的光学灵敏度. 本文应用密度泛函理论(DFT)及含时密度泛函理论(TD-DFT)方法对六种含不同取代基的探针分子进行了几何构型优化及激发态计算, 探讨了不同取代基对PET效应影响. 计算结果表明: 基态时这些探针分子的最高占有分子轨道(HOMO)和最低未占有分子轨道(LUMO)都在荧光母体BODIPY的π, π^*轨道, 而识别基团上氮原子孤对电子所在的轨道为HOMO-1轨道. 但是在激发态, 当氮原子上有两个取代基时, HOMO-1→LUMO跃迁的激发能都小于荧光团的HOMO→LUMO跃迁, 这将有可能产生PET效应并导致荧光熄灭, 而当氮原子上有一个取代基时不会出现这种现象. 通过激发态结构优化可以发现, 无论识别基团氮原子上有一个还是两个取代基, N原子的轨道对称性都发生变化, 由sp³→sp², 孤对电子占据在p轨道上, 其轨道能级升高至荧光团的HOMO和LUMO轨道之间, 将导致不同程度的PET效应, 与实验结果一致.     

4-(1,2-二苯基)乙烯基-4’-(N,N-二苯基-4-乙烯基苯胺基)联苯及其二氟取代衍生物的电子结构与光谱性质

分别采用B3LYP/6-31G(d)和CIS/6-31G(d)方法对4-(1,2-二苯基)乙烯基-4’-(N,N-二苯基-4-乙烯基苯胺基)联苯(A)及其二氟取代衍生物(B-F)的基态(S0)和单重激发态(S1)的几何构型进行了全优化, 计算获得了电离势IP、电子亲和势EA等相关数据, 并采用含时密度泛函(TD-DFT)方法计算了上述化合物的电子吸收和荧光发射光谱. 研究结果表明, 化合物A及二氟取代衍生物B-F在469-474 nm蓝光区域主发射峰的强度远远大于372-387 nm范围的次发射峰, 说明此类化合物具有纯度较高的发射光谱; 主链苯环上的二氟取代(B, C和D)使最低空轨道(LUMO)能级明显降低, 有利于提高电子注入; 芳胺基苯环上的二氟取代(D和E)使分子最高占据轨道(HOMO)能级明显降低, 电离势增加, 能隙变大, 有利于抑制空穴越过发光层向电子传输层输运, 减少界面处激基复合物的形成, 同时起到光谱蓝移的效果; 既是主链苯环上也是芳胺基苯环上的二氟取代衍生物D更有利于平衡电子-空穴的注入, 应该具有更加优良的发光性质.     

4-(1,2-二苯基)乙烯基-4''-(NSV-二苯基-4-乙烯基苯胺基)联苯及其二氟取代衍生物的电子结构与光谱性质

分别采用B3LYP/6-31G(d)和CIS/6-31G(d)方法对4-(1,2-二苯基)乙烯基-4'-(N,N-二苯基-4-乙烯基苯胺基)联苯(A)及其二氟取代衍生物(B-F)的基态(S0)和单重激发态(S1)的几何构型进行了全优化,计算获得了电离势IP、电子亲和势EA等相关数据,并采用含时密度泛函(TD-DFT)方法计算了上述化合物的电子吸收和荧光发射光谱.研究结果表明,化合物A及二氟取代衍生物B-F在469-474 nm蓝光区域主发射峰的强度远远大于372-387 nm范围的次发射峰,说明此类化合物具有纯度较高的发射光谱;主链苯环上的二氟取代(B,C和D)使最低空轨道(LUMO)能级明显降低,有利于提高电子注入;芳胺基笨环上的二氟取代(D和E)使分子最高占据轨道(HOMO)能级明显降低,电离势增加,能隙变大,有利于抑制空穴越过发光层向电子传输层输运,减少界面处激基复合物的形成,同时起到光谱蓝移的效果;既是主链苯环上也是芳胺基苯环上的二氟取代衍生物D更有利于平衡电子-空穴的注入,应该具有更加优良的发光性质.     

三-(2-苯基吡啶)-铱及其衍生物电子结构、电子光谱及取代基效应的密度泛函理论研究

采用密度泛函理论(DFT)B3LYP/LanL2dz方法,对一类重要的磷光材料三-(2-苯基吡啶)-铱[Ir(ppy)₃]及其衍生物的电子结构与电子光谱进行了研究,讨论了取代基对配合物的能级和LUMO-HOMO能隙的影响,发现吸电子基(-CN)使能级降低,HOMO-LUMO之间能隙减小,而推电子基(-OCH₃)使能级升高,HOMO-LUMO之间能隙变化不大.     

Computational study of the structure, dynamics, and photophysical properties of conjugated polymers and oligomers under nanoscale confinement

Computational simulations were used to investigate the dynamics and resulting structures of several para-phenylenevinylene (PPV) based polymers and oligomers (PPV, 2-methoxy-5-(2'-ethyl-hexyloxy)-p-phenylenevinylene --> MEH-PPV and 2,5,2',5'-tetrahexyloxy-7,8'-dicyano-p-phenylenevinylene --> CN-PPV). The results show how the morphology and structure are controlled to a large extent by the nature of the solute-solvent interactions in the initial solution-phase preparation. Secondary structural organization is induced by using the solution-phase structures to generate solvent-free single molecule nanoparticles. Isolation of these single molecule nanostructures from microdroplets of dilute solution results in the formation of electrostatically oriented nanostructures at a glass surface. Our structural modeling suggests that these oriented nanostructures consist of folded PPV conjugated segments with folds occurring at tetrahedral defects (sp3 C-C bonds) within the polymer chain. This picture is supported by detailed experimental fluorescence and scanning probe microscopy studies. We also present results from a fully quantum theoretical treatment of these systems which support the general conclusion of structure-mediated photophysical properties.     

Control of pi-stacking for highly emissive poly(p-phenylenevinylene)s: synthesis and photoluminescence of new tricyclodecane substituted bulky poly(p-phenylenevinylene)s and its copolymers

In the present work, we have demonstrated a facile approach to increase the luminescence of the poly (p-phenylenevinylene)s via controlling the molecular aggregates induced by pi-stacking. We have synthesized new bulky tricyclodecane (TCD) substituted PPVs: poly(2-methoxy-5-tricyclodecanemethyleneoxy-1,4-phenylenevinylene) (MTCD-PPV), poly(bis-2,5-tricyclodecanemethyleneoxy-1,4-phenylenevinylene) (BTCD-PPV), and a series of symmetrically substituted bulky PPV copolymers (P-1-P-7) covering the entire composition range from 0 to 100 mol %. The structures of the monomers and polymers were confirmed by 1H NMR and FTIR, and the molecular weights were determined by gel permeation chromatography. The composition analysis by NMR revealed that the bulky monomer was highly reactive and the incorporation of bulky units in MEH-PPV increased irrespective of the feed ratio. The polymers possess good solubility, high molecular weights, good thermal stability, and so forth. The molecular weights of the PPV copolymers were also significantly affected by the bulky substitution: the higher the incorporation of bulky units, the lower the molecular weight. The absorption and emission studies revealed that there was no influence on the MEH-PPV by TCD substitution in solution whereas in the solid state the photoluminescence intensity of PPV increased more than 10 times. The luminescence increase in PPV was observed throughout the entire bulk and was not confined to any particular domain in the polymer. The bulky PPV copolymers showed that both the luminescence intensity (in film) and quantum yields (in solution) increased with an increase in the extent of BTCD incorporation in the MEH-PPV and attained a maximum for 50% BTCD. The TCD unit has thus proved to be an efficient bulky susbstituent for PPV as it controls the pi-stack-induced molecular aggregates in the polymer chains by increasing the interchain distances. The new bulky PPV copolymers are highly soluble, thermally stable, and highly luminescent besides being economically cheap compared to the other materials reported so far for the bulkier approach in pi-conjugated materials.     

Enhancing electroluminescence performance of MEH-PPV based polymer light emitting device via blending with organosoluble polyhedral oligomeric silsesquioxanes

Organosoluble polyhedral oligomeric silsesquioxanes (POSS) blending effect on electroluminescence properties of MEH-PPV based polymer light emitting device was investigated. Excellent compatibility and surface morphology of organosoluble POSS and MEH-PPV based composite films were observed using AFM spectroscopy. The surface roughness of POSS:MEH-PPV composite film increased with increasing POSS content. Interfacial area between the light-emitting layer and cathode was favorably enhanced for cathode electron-injection. MEH-PPV blended with POSS would create a better balance between the electron and hole fluxes for POSS:MEH-PPV composite film based devices. This led to greater current efficiency of the POSS:MEH-PPV composite film based device as compared to one with a light emitting layer of MEH-PPV. Organosoluble POSS concentration effects on the PL spectra and EL performances were also studied for the POSS:MEH-PPV composite film based polymer light emitting devices.     

聚合物发光电化学池的研究——中国科学院有机固体重点实验室导电聚合物电化学研究工作简介(Ⅱ)

简要介绍本研究组 1997年以来在聚合物发光电化学池 (LEC)研究中取得的一些成果,包括发光聚合物的电化学性质及其HOMO和LUMO能级的电化学测量,LECp i n结的交流阻抗分析,双功能嵌段共聚物LEC,以及咪唑盐离子液体掺杂的室温准冷冻p i n结LEC等.     

含二唑的聚(间亚苯乙烯)电致发光二极管

含二唑的聚（间亚苯乙烯）电致发光二极管印寿根李晨曦黄文强何炳林（南开大学吸附分离功能高分子材料国家重点实验室高分子化学研究所天津３０００７１）彭俊彪刘星元李文连（中国科学院长春物理研究所长春１３００２１）关键词电致发光，光电子能谱，聚（间亚苯...     

Enhanced Photostability and Red-NIR Photosensitivity of Conjugated Polymer Charge-Transfer Complexes

A promising route to photostable and low-bandgap polymer materials for optoelectronic and photonic applications could be utilization of donor-acceptor ground-state charge-transfer complexes (CTCs) of wide-bandgap conjugated polymers. In this work, we report our results on photostability and photoelectric studies of CTC between an archetypical conjugated polymer MEH-PPV and low-molecular-weight acceptor 2,4,7-trinitrofluorenone (TNF). By using the pump-probe laser photobleaching technique, we show that the photodegradation rate of MEH-PPV:TNF blend films decreases up to four orders of magnitude as compared with pristine MEH-PPV. By using photocurrent and surface photovoltage spectroscopies, we demonstrate that the photoelectric sensitivity of the MEH-PPV:TNF CTC can be deeply extended in the polymer optical gap down to 1 µm. However, the main drawback of the CTC studied is their low charge collection efficiency, and an approach to increasing it is discussed.     

新型含氟聚苯撑乙烯的合成及电致发光性能

设计并合成了两个不同烷氧基增溶的结构新颖的含氟聚苯撑乙烯Pa, Pb和共聚物Pc. 通过核磁共振和元素分析对其结构进行了表征, 通过热重分析、凝胶色谱测定了其热分解温度和分子量及分布; 紫外-可见吸收光谱仪和荧光分光光度计测得其吸收-发射光谱. 测量发现热失重曲线拐点温度超过400 ℃. 由2-乙基己基增溶的Pa和Pc具有优异的溶解性, 固态荧光发射波长分别为499和585 nm, 相应比PPV和MEH-PPV稍有蓝移. 应用旋转涂膜的方法制作Pa和Pc的双层器件(ITO/PEDOT/Polymer/Ba/Al), 电致发光波长分别为494和604 nm, 器件均具有较低的启动电压(4 V左右), 分别在24和15 V时达到最大亮度598和203 cd•m^－2, 而此时电流密度分别为100和80 mA•cm^－2.     

可溶性聚合物电致发光材料PDHPV的合成及单、双层发光二极管器件的发光性能比较

可溶性聚合物电致发光材料ＰＤＨＰＶ的合成及单、双层发光二极管器件的发光性能比较李晨曦，尹春，黄文强，印寿根，张会旗，何炳林，郑军，华玉林（南开大学高分子化学研究所，天津，３０００７１）（天津理工学院材料物理研究所）关键词ＰＤＨＰＶ共轭聚合物；电致发光...     

Ultrafast charge photogeneration dynamics in ground-state charge-transfer complexes based on conjugated polymers

The charge photogeneration and early recombination in MEH-PPV-based charge-transfer complexes (CTCs) and in MEH-PPV/PCBM blend as a reference are studied by ultrafast visible-pump-IR-probe spectroscopy. After excitation of the CTC band, an immediate (<100 fs) electron transfer is observed from the polymer chain to the acceptor with the same yield as in the MEH-PPV/PCBM blend. The forward charge transfer in the CTCs is followed by an efficient (approximately 95%) and fast (<30 ps) geminate recombination. For comparison, the recombination efficiency obtained in the MEH-PPV/PCBM blend does not exceed a mere 50%. Polarization-sensitive experiments demonstrate high (approximately 0.3) values of transient anisotropy for the CTCs polaron band. In contrast, in the MEH-PPV/PCBM blend the dipole moment orientation of the charge-induced transition is less correlated with the polarization of the excitation photon. According to these data, photogeneration and recombination of charges in the CTCs take place locally (i.e., within a single pair of a polymer conjugation segment and an acceptor) while in the MEH-PPV/PCBM blend exciton migration precedes the separation of charges. Results of the ultrafast experiments are supported by photocurrent measurements on the corresponding MEH-PPV/acceptor photodiodes.     

The effect of broken conjugation on the excited state: ether linkage in the cyano-substituted poly(p-phenylene vinylene) conjugated polymer poly(2,5,2',5'-tetrahexyloxy-8,7'-dicyano-di-p-phenylene vinylene)

We investigate the effect of broken conjugation on the excited state dynamics of excimers in cyano-substituted phenylene-vinylene polymers. We compare previous studies on the well-characterized poly(2,5,2',5'-tetrahexyloxy-8,7'-dicyano-di-p-phenylene vinylene) (CN-PPV) with poly[oxa-1,4-phenylene-1,2-(1-cyano)-ethenylene-2,5-dioctyloxy-1,4-phenylene-1,2-(2-cyano)-ethenylene-1,4-phenylene] (CN-ether-PPV), in which the conjugation is disrupted by the insertion of an oxygen atom within the polymer backbone. Despite the broken conjugation, the spectroscopic behavior of the two materials is similar, indicating that the cyano group dominates the photophysics in these materials. The emission in CN-ether-PPV is due to a single-chain exciton in solution and due to an interchain excimer in thin film, as previously reported for CN-PPV; however, the excimer absorption and emission in thin film are blueshifted by approximately 0.2 eV relative to CN-PPV, implying that the excimer in CN-ether-PPV is less stable. Furthermore, substitution of an ether group along the chain results in decay times in both solution and film that are twice as long than in CN-PPV due to the broken conjugation which restricts the exciton within a conjugation segment and reduces its access to internal quenching sites. These properties result in a decay time of 14 ns for CN-ether-PPV film, one of the longest decay times observed in a conjugated polymer film. The long lifetime indicates a large exciton diffusion length, making these species particularly vulnerable to quenching by other materials. This work has implications for the design of conjugated polymers for efficient optoelectronic devices, such as photovoltaics.