取代基对corrole二阶非线性光学性质的影响

在6-31G(d,p)水平上用B3LYP方法对三苯基corrole(TPC)以及氟苯基corrole系列分子进行几何构型优化.用ZINDO/SOS方法计算了这些分子的一阶超极化率.计算结果表明:TPC分子由于其结构非中心对称使其具有大小为2.46×10-50 C3·m3·J-2的一阶超极化率.引入氟苯基后,氟取代苯基corrole系列分子的一阶超极化率均有显著提高,其中5位及10,15位氟苯基取代的corrole分子具有较大的一阶超极化率(3.71×10-49 C3·m3·J-2).氟苯基corrole系列分子一阶超极化率提高主要起源于分子的二能级分量及三能级分量显著增大,且二能级分量与三能级分量大小相当、符号相同.计算表明,二能级分量的增大主要来源于第三激发态(B1)与基态之间的偶极矩的变化.跃迁通道分析表明三能级分量的增大主要通过改变与结构敏感的激发态跃迁通道,即由TPC分子B带与Q带的耦合变成了氟苯基corrole分子B带内2个不同激发态的耦合.     

桥联双卟啉的合成及结构表征

近年来,双卟啉化合物作为主体分子在分子识别领域的研究已成为卟啉化学中的一个重要分支和热点.双卟啉分子中,两个卟啉环之间可以形成一个空腔,而卟啉环间桥连基团不同,则两个卟啉环的相互方位就不同,这就使空腔的大小和空间形态得以控制,从而实现对不同客体分子的选择性识别.基于以上优点,双卟啉可以对多种有机和生物分子进行识别.同时,在卟啉环或者桥链上引入适当的手性中心,就可以对底物进行手性识别.因此,双卟啉的分子识别研究将具有广阔的前景.     

溶剂化变色法测定有机分子β的若干问题

溶剂化变色法是测定有机分子超极化率．的一种半定量方法,已为许多实验室采用并取得了较好的结果．它的理论依据是描述有机分子产值的双能级模型【小式中：P。、11。分别为分子的基态和激发态偶极矩,。e。和11e。则分别为基态和激发态的跃迁频率和跃迁偶极矩．这包括三个方面     

氨基酸桥联手性双卟啉的二阶非线性光学性质研究

采用半经验量子化学PM3方法对系列氨基酸桥联双卟啉1, 2, 3, 4及其锌配合物进行了几何结构优化, 并用TDHF/PM3方法计算了其静态二阶非线性光学系数. 计算结果表明, L型-氨基酸桥联双卟啉及其锌配合物具有右手螺旋结构特征. 在电偶极近似下, 不同手性氨基酸侧链基团R对分子的总体二阶非线性光学系数β和βHRS的影响不大, 但对二阶非线性光学系数的手性分量βxyz却有显著影响. βxyz与螺旋结构参数r2ζ/L4成正比关系, 符合手性分子二阶非线性光学响应的单电子螺旋模型理论. β张量分析表明, 此类分子表现为以八极为主、 偶极为辅的多极分子, 卟啉环与锌离子的配位有利于增加二阶非线性光学响应的偶极分量和手性分量βxyz.     

1,2方酸衍生物非线性光学性质的从头算研究

用CPHF方法在abinitio/4-31G+pd水平上计算了四个1,2方酸衍生物分子的线性极化率,一阶和二阶超极化率.从电荷分布,跃迁偶极矩,前沿轨道性质等方面讨论了其结构与性能的关系.研究表明,四元环作为吸电基团(A),取代基作为供电基团(D),组成了D-A-D结构,取代基的性质对分子的非性光学系数有显著影响.     

以苯等芳香环桥联的1,3-二硫杂环戊二烯衍生物的NLO性质

采用密度泛函理论(DFT)B3LYP/6-31G*优化一系列以芳环为桥联基团,1,3-二硫杂环戊二烯为供电子基团,丙二氰为吸电子基团的D-π-A型分子的几何结构,在此基础上对分子的极化率和第一超极化率进行计算.结果分析表明,桥联苯环数的增加,供电子基团(—OCH3)的引入及共轭桥的增长对分子的几何构型影响很小,但能使分子的二阶非线性光学(NLO)系数增加,且分子的最大吸收波长发生红移.甲氧基的引入或共轭桥的增长,分子的前线分子轨道能级差减小,TD-DFT计算表明分子深层占有轨道与空轨道之间的电子跃迁对二阶NLO效应也有较明显贡献.     

联吖叮氮氧自由基体系及其衍生物NLO性质的密度泛函理论研究

以实验合成的联吖叮氮氧自由基分子为母体, 设计了7个自由基分子. 采用密度泛函理论(DFT) UB3LYP/6-31g(d,p)方法对这些自由基分子不同自旋态的稳定性和非线性光学(NLO)系数进行计算. 结果表明, 联吖叮氮氧自由基分子及其衍生物三重态为稳定基态, 符合自旋极化规则. 引入给吸电子取代基使自由基体系的极化率αs与二阶超极化率γs值有所增大, 且基团的给吸电子能力越强, αs和γs值增加越明显; 对于一阶超极化率βtot, 自由基体系处于单重态时, 取代基的影响较大. 所有自由基分子三重态的NLO系数都小于单重态, 表明可以通过控制体系的自旋多重度来调节体系的NLO性质.     

D-l-A分子修饰罗丹明底环及对其激发态的影响

通过乙基桥把供电子基团1,8-萘酰亚胺与罗丹明底环羧酸基相连,得到了两种以D-l-A(Donor-Acceptor-Line alkanes compounds)分子修饰罗丹明底环的化合物,并就合成中间体D-π-A(Donor-Acceptor-π-conjugated compounds)分子中哌嗪供电子基取代溴对1,8-萘酐母体基态和激发态的影响,以及对D-l-A分子修饰罗丹明底环对罗丹明母体D-π-A分子紫外可见吸收光谱和激发态的影响进行了研究。结果表明:用D-l-A分子修饰罗丹明底环时,D(Donor compound)的给电子能力越强,其吸收强度越大,其吸收紫外光而激发能力越强;在激发态下D-l-A体系发生了分子内能量传递,萘酰亚胺基团发生强烈的荧光猝灭,罗丹明底环接收能量激发罗丹明母体(D-π-A分子)发射特征荧光,D的给电子能力越强,其荧光强度越高。     

D-1-A分子修饰罗丹明底环及对其激发态的影响

通过乙基桥把供电子基团1,8-萘酰亚胺与罗丹明底环羧酸基相连,得到了两种以D-1-A（Donor-Acceptor-Linealkanescompounds）分子修饰罗丹明底环的化合物,并就合成中间体D-π-A（Donor-Acceptor-Tt-conjugatedcompounds）分子中哌嗪供电子基取代溴对1,8-萘酐母体基态和激发态的影响,以及对D-1-A分子修饰罗丹明底环对罗丹明母体D-π-A分子紫外可见吸收光谱和激发态的影响进行了研究。结果表明：用D-1-A分子修饰罗丹明底环时,D（Donorcompound）的给电子能力越强,其吸收强度越大,其吸收紫外光而激发能力越强;在激发态下D-1-A体系发生了分子内能量传递,萘酰亚胺基团发生强烈的荧光猝灭,罗丹明底环接收能量激发罗丹明母体（D-π-A分子）发射特征荧光,D的给电子能力越强,其荧光强度越高。     

卟啉-噁二唑二元体系光诱导能量及电子传递研究

以5-对氨基苯基-10,15,20-三苯基卟啉及2-苯基-5-(对氨基苯基)-1,3,4-噁二唑为原料合成了系列卟啉-噁二唑二元化合物, 其结构通过¹H NMR, ESI-MS, IR, UV-Vis确定. 对合成化合物进行光谱性能测定, 结果表明, 在卟啉与噁二唑混合体系中, 存在着卟啉激发态分子向噁二唑基态分子的分子间电子传递过程, 导致卟啉激发态的荧光猝灭; 在卟啉-噁二唑二元体系中, 315 nm激发下发生了由激发态噁二唑基团至卟啉基团的能量传递, 导致噁二唑基团荧光猝灭, 卟啉基团荧光增强. 420 nm激发下不存在分子内卟啉基团向噁二唑基团的电子回传竞争; 电化学性能测定进一步表明从噁二唑基团向卟啉基团的电子传递是可能的. 因此卟啉-噁二唑二元化合物可能作为一种模型, 模拟光合作用中电子给体至叶绿素之间的电子传递过程.     

Theoretical analysis of the porphyrin-porphyrin exciton interaction in circular dichroism spectra of dimeric tetraarylporphyrins

Chiral bis-porphyrins are currently the subject of intense interest as chiral receptors and as probes in the determination of structure and stereochemistry. To provide an improved framework for interpreting the circular dichroism (CD) spectra of bis-porphyrins, we have calculated the CD spectra of chiral bis-porphyrins from three classes: I, where porphyrins can adopt a relatively wide range of orientations relative to each other; II, porphyrins have a fixed relative orientation; III, porphyrins undergo pi-stacking. The calculations primarily utilized the classical polarizability theory of DeVoe, but were supplemented by the quantum mechanical matrix method. Class I was represented by three isomers of the diester of 5alpha-cholestane-3,17-diol with 5-(4'-carboxyphenyl)-10,15,20-triphenylporphin (2-alphabeta, 2-betaalpha, 2-betabeta). Careful analysis of the torsional degrees of freedom led to two to four minimum-energy conformers for each isomer, in each of which the phenyl-porphyrin bonds had torsional angles near 90 degrees. Libration about these bonds is relatively unrestricted over a range of +/-45 degrees. CD spectra in the Soret region were calculated as Boltzmann-weighted averages over the low-energy conformers for each isomer. Three models were used: the effective transition moment model, in which only one of the degenerate Soret components is considered, along the 5-15 direction; the circular oscillator model, in which both Soret components are given equal weight; and the hybrid model, in which the 10-20 oscillator is given half the weight of the 5-15 oscillator, to mimic the effect of extensive librational averaging about the 5-15 direction. All three models predict Soret exciton couplets with signs in agreement with experiment. Quantitatively, the best results are given by the hybrid and circular oscillator models. These results validate the widely used effective transition moment model for qualitative assignments of bis-porphyrin chirality and thus permit application of the exciton chirality model. However, for quantitative studies, the circular oscillator or hybrid models should be used. The simplified effective transition moment and hybrid models are justified by the librational averaging in the class I bis-porphyrins and should only be used with such systems. Two class II bis-porphyrins were also studied by DeVoe method calculations in the circular oscillator model, which yielded good agreement with experiment. Class III bis-porphyrins were represented by 2-alphaalpha, for which the calculations gave qualitative agreement. However, limitations in the conformational analysis with the close contacts and dynamic effects in these pi-stacked systems preclude quantitative results.     

Substituent-control exciton in J-aggregates of protonated water-insoluble porphyrins

A series of protonated porphyrin J-aggregates of various water-insoluble tetraphenylporphyrin derivatives was prepared by aggregation at the liquid-liquid or gas-liquid interface. Using atomic force microscopy, we observed microcrystalline porphyrin J-aggregates. The J-aggregates have two strong exciton bands corresponding to the B (Soret)- and Q-bands of the protonated porphyrin. Interestingly, the excitation energy of the lower exciton (denoted by S1) markedly depends on the meso-substituents, whereas that of the higher exciton (denoted by S2) does not depend on them. These results indicate that the nature of the exciton coupling of the S1 transition dipole moment can be systematically changed by the substituents.     

Hydrogen‐Bonding Induced Cooperative Effect on the Energy Transfer in Helical Polynorbornenes Appended with Porphyrin‐Containing Amidic Alanine Linkers

Polynorbornenes appended with porphyrins containing a range of different linkers are synthesized. The use of bisamidic chiral alanine linkers between the pending porphyrins and the polymeric backbone has been shown to bring the adjacent porphyrin chromophores to more suitable orientation for exciton coupling owing to hydrogen bonding between the adjacent linkers. The hydrogen bonding between the adjacent pendants in these polymers may induce a cooperative effect and therefore render single‐handed helical structures for these polymers. Such a cooperative effect is reflected in the enhancement of FRET efficiencies between zinc–porphyrin and free base porphyrin in random copolymers.     

Photophysical properties of long rodlike meso-meso-linked zinc(II) porphyrins investigated by time-resolved laser spectroscopic methods

The molecular design of directly meso-meso-linked porphyrin arrays as a new model of light-harvesting antenna as well as a molecular photonic wire was envisaged to bring the porphyrin units closer for rapid energy transfer. For this purpose, zinc(II) 5,15-bis(3,5-bis(octyloxy)phenyl)porphyrin (Z1) and its directly meso-meso-linked porphyrin arrays up to Z128 (Zn, n represents the number of porphyrins) were synthesized. The absorption spectra of these porphyrin arrays change in a systematic manner with an increase in the number of porphyrins; the high-energy Soret bands remain at nearly the same wavelength (413-414 nm), while the low-energy exciton split Soret bands are gradually red-shifted, resulting in a progressive increase in the exciton splitting energy. The exciton splitting is nicely correlated with the values of cos[pi/(N + 1)] according to Kasha's exciton coupling theory, providing a value of 4250 cm(-1) for the exciton coupling energy in the S(2) state. The increasing red-shifts for the Q-bands are rather modest. The fluorescence excitation anisotropy spectra of the porphyrin arrays show that the photoexcitation of the high-energy Soret bands exhibits a large angle difference between absorption and emission dipoles in contrast with the photoexcitation of the low-energy exciton split Soret and Q-bands. This result indicates that the high-energy Soret bands are characteristic of the summation of the individual monomeric transitions with its overall dipole moment deviated from the array chain direction, while the low-energy Soret bands result from the exciton splitting between the monomeric transition dipoles in line with the array chain direction. From the fluorescence quantum yields and fluorescence lifetime measurements, the radiative coherent length was estimated to be 6-8 porphyrin units in the porphyrin arrays. Ultrafast fluorescence decay measurements show that the S(2) --> S(1) internal conversion process occurs in less than 1 ps in the porphyrin arrays due to the existence of exciton split band as a ladder-type deactivation channel, while this process is relatively slow in Z1 (approximately 1.6 ps). The rate of this process seems to follow the energy gap law, which is mainly determined by the energy gap between the two Soret bands of the porphyrin arrays.     

5,10-A2B2-type meso-substituted porphyrins--a unique class of porphyrins with a realigned dipole moment

Current applications in porphyrin chemistry require the use of unsymmetrically substituted porphyrins. Many current industrial interests in optics and biomedicine require systems with either push-pull (electron-donating and -withdrawing groups) or amphiphilic systems (hydrophobic and hydrophilic groups). In this context we present the class of 5,10-A(2)B(2)-type porphyrins for which two different substituents are positioned in diagonally opposite meso positions. Thus, the intramolecular dipole moment in these tetrapyrroles is positioned along a β-β vector passing through two pyrrole rings. This is opposite to the situation of the frequently used 5,15-A(2)BC porphyrins for which the dipole moment is oriented along a meso-meso axis. We have elaborated syntheses of the 5,10-A(2)B(2) porphyrins by using transition-metal-catalyzed transformations of 5,10-A(2) porphyrins or direct substitutions reactions thereof; this gives the target molecules in 22-77% overall yields. The compounds exhibit interesting structural, spectroscopic, and optical features and can serve as building blocks for new porphyrin arrays and applications.     

光学活性金属卟啉的磁手性效应研究

磁光学活性与自然光学活性均可用介质对左右圆偏振光的吸收之差来表示 .但自然光学活性和磁光学活性的物理机制是截然不同的 ,前者源于镜象不能互相重叠介质的非定域光学响应 ( nonlocaloptical response) ,而后者则是由于介质的时间反演对称性 ( time- reversal symmetry)被磁场打破所致 .理论分析表明 ,当介质的两种光学活性同时存在时 ,将会出现一个新的附加光学效应 ,这种磁光学活性与自然光学活性之间的交叉效应称为磁手性效应 ( magneto- chiral effect)或磁手二色性 ( magneto-chiral dichroism) [1,2 ] .磁手性效应通常很弱 ,直到 1…     

Efficient exciton transport in layers of self-assembled porphyrin derivatives

The photosynthetic apparatus of green sulfur bacteria, the chlorosome, is generally considered as a highly efficient natural light-harvesting system. The efficient exciton transport through chlorosomes toward the reaction centers originates from self-assembly of the bacteriochlorophyll molecules. The aim of the present work is to realize a long exciton diffusion length in an artificial light-harvesting system using the concept of self-assembled natural chlorosomal chromophores. The ability to transport excitons is studied for porphyrin derivatives with different tendencies to form molecular stacks by self-assembly. A porphyrin derivative denoted as ZnOP, containing methoxymethyl substituents ({meso-tetrakis[3,5-bis(methoxymethyl)phenyl]porphyrinato}zinc(II)) is found to form self-assembled stacks, in contrast to a derivative with tert-butyl substituents, ZnBuP ({meso-tetrakis[3,5-bis(tert-butyl)phenyl]porphyrinato}zinc(II)). Exciton transport and dissociation in a bilayer of these porphyrin derivatives and TiO2 are studied using the time-resolved microwave conductivity (TRMC) method. For ZnOP layers it is found that excitons undergo diffusive motion between the self-assembled stacks, with the exciton diffusion length being as long as 15 +/- 1 nm, which is comparable to that in natural chlorosomes. For ZnBuP a considerably shorter exciton diffusion length of 3 +/- 1 nm is found. Combining these exciton diffusion lengths with exciton lifetimes of 160 ps for ZnOP and 74 ps for ZnBuP yields exciton diffusion coefficients equal to 1.4 x 10(-6) m2/s and 1 x 10(-7) m2/s, respectively. The larger exciton diffusion coefficient for ZnOP originates from a strong excitonic coupling for interstack energy transfer. The findings show that energy transfer is strongly affected by the molecular organization. The efficient interstack energy transfer shows promising prospects for application of such self-assembled porphyrins in optoelectronics.     

Exciton coupling of tetra(p-hydroxyphenyl)porphyrin controlled by substituents of counterions in Triton X-100 micellar solution

The interactions of nonionic meso-tetra(p-hydroxyphenyl)porphyrin (THPP) with CX3COOH (X = F, Cl, Br) in Triton X-100 (TX) micellar solution have been investigated by optical absorption, resonance light-scattering, and fluorescence spectroscopies. The double red-shifted absorption bands and strong resonance light scattering (RLS) signal imply that the assemblies induced by trihalo acetic acids belong to J-aggregates. The fluorescence of porphyrin is quenched due to the aggregate formation. The kinetics of assemblies trigged by CBr3COOH is studied via stopped-flow techniques. No characteristics of autocatalyzed reactions are observed, and there is only a log phase. The nature of the exciton coupling of transition dipole moment can be systematically changed by the haloid substituents of the organic counteranion.