偶氮苯侧链结构对聚丙烯酸酯三阶非线性光学性能影响

设计合成了一系列含偶氮苯非线性生色团的丙烯酸酯,并采用溶液聚合法合成了功能化的聚丙烯酸酯,利用FTIR、NMR、UV等对化合物的结构进行了表征,证实得到了指定结构的化合物.利用Z扫描技术对合成的聚丙烯酸酯的非线性光学性能进行了研究,通过对聚合物的非线性光学吸收拟合,计算得到非线性吸收系数β和三阶非线性系数χ(3),并探讨了取代基生色团分子结构与高分子三阶非线性光学性能的关系,结果显示增大侧链生色团π电子离域长度或强DπA(推拉基团)结构均可有效提高聚合物的三阶非线性光学性能.     

聚酰胺酸及其接枝衍生物的三阶非线性光学性能研究

设计合成了苯代三聚氰胺与均苯四酸二酐缩聚物, 及不同侧链的p-π共轭缩聚物, 并以量子化学PM3/CIS方法为基础, 利用完全态求和(SOS)公式, 对不同侧链取代的聚酰胺酸的分子进行了几何构型优化, 并计算了其三阶非线性光学系数γ. 研究了不同侧链对聚合物三阶非线性性能的影响. 这些结果对合成具有优良加工性能的三阶非线性光学材料是有一定的指导作用.     

苯并[b]萘并[2'''',3'''':5,6][1,4]二噻英并[2,3-i]噻蒽-5,7,9,14,16,18-六酮的合成及其三阶非线性光学性能

以1,4-萘醌为原料,合成了含硫的醌构稠杂环化合物苯并[b]萘并[2',3':5,6][1,4]二噻英并[2,3-i]噻蒽-5,7,9,14,16,18-六酮(4),其结构经1H NMR和IR确证.采用波长为800 nm,脉宽为80 fs的Ti:Sapphire飞秒激光,运用双光束简并四波混频法测定了4的三阶非线性光学性能,结果表明,4的三阶非线性光学极化率χ(3),非线性折射率n2,分子二阶超极化率γ和响应时间分别为2.89×10-13 esu, 5.31×10-12 esu, 3.14×10-31 esu和101 fs.并分析了4的分子结构对其三阶非线性光学性能的影响.     

苯并[b]萘并[2′,3′∶5,6][1,4]二噻英并[2,3-i]噻蒽-5,7,9,14,16,18-六酮的合成及其三阶非线性光学性能

以1,4-萘醌为原料,合成了含硫的醌构稠杂环化合物苯并[b]萘并[2′,3′∶5,6][1,4]二噻英并[2,3-i]噻蒽-5,7,9,14,16,18-六酮(4),其结构经1HNMR和IR确证。采用波长为800nm,脉宽为80fs的Ti∶Sapphire飞秒激光,运用双光束简并四波混频法测定了4的三阶非线性光学性能,结果表明,4的三阶非线性光学极化率χ(3),非线性折射率n2,分子二阶超极化率γ和响应时间分别为2.89×10-13esu,5.31×10-12esu,3.14×10-31esu和101fs。并分析了4的分子结构对其三阶非线性光学性能的影响。     

不同类型二苯乙烯衍生物双光子吸收截面的理论研究

用AM1和INDO/CI理论方法,系统研究不同类型二苯乙烯衍生物(D-π-D,A-π-A,D-π-A)的结构和电子光谱。在正确的UV-vis光谱基础上,预测了双光子吸收峰的位置,用SOS公式计算了三阶非线性光学系数及双光子吸收截面,并从微观上探讨了不同取代基对双光子吸收截面的影响。     

含噻吩环的新推-拉型多环电光聚合物中间体的三阶非线性光学系数的理论研究

以INDO/SCI方法为基础,利用完全态求和(SOS)公式,计算了一系列新推-拉型多环电光聚合物中间体的三阶非线性光学系数γ(一ω;ω,-ω,ω)和γ(0;0,0,0),研究了γ与分子骨架、给受取代基和噻吩环数目(共轭分子链长的关系)及其与外场频率的关系,表明在链不十分长时,γ与链长的2.69次方成正比。     

六元环硼氮烷对称取代方酸的电子光谱和非线性光学性质的DFT研究

用量子化学密度泛函理论B3LYP方法,在6-31G(d)水平上对环硼氮烷和苯基对称取代方酸进行几何构型优化.以此为基础,利用TD-DFT方法得到方酸衍生物的UV-Vis吸收光谱.进一步引入外电场,用有限场(FF/DFT-B3LYP)方法探讨了各体系的三阶非线性光学性质(NLO).计算结果显示,对称环硼氮烷取代的方酸衍生物性质不同于苯环取代,取代位置对电荷分布、分子轨道特征和非线性光学性质的影响很大.氮原子与方酸相连时对提高方酸体系的三阶非线性光学性质十分有效,其NLO系数可达2.3808×10^-24C·m.     

水杨醛缩乙二胺双席夫碱及其Ni(Ⅱ) 配合物的电子结构和非线性光学性质的INDO/CI研究

采用量子化学ab initio HF方法, 在6.31G(d)基组水平上， 对水杨醛缩乙二胺类双席夫碱及其Ni配合物体系进行几何构型优化. 以优化的稳定构型为基础, 利用INDO/CI方法计算体系的电子光谱, 同时用ZINDO.SOS方法给出该系列分子二阶(βijk)和三阶(γijkl)非线性光学系数. 计算结果表明, 共轭性增强有助于增大分子的二阶及三阶非线性光学系数, 双席夫碱化合物1的β和γ值分别为35.54×10-30和-1.20×10-34 esu, 而共轭桥为萘环的化合物4的β和γ值分别为54.22×10-30和2.00×10-34 esu, 端部引入苯并环的化合物5的β和γ值增加幅度更大. 对应的金属Ni(Ⅱ)配合物的β值增加较明显, 为配体的1.7~10.8倍, γ值也有不同程度的增加.     

可溶性聚(2-甲氧基-5-辛氧基)对苯乙炔的合成及其导电和三阶非线性光学性能

聚对苯乙炔;电导率;三阶非线性极化率;简并四波混频;可溶性聚(2-甲氧基-5-辛氧基)对苯乙炔的合成及其导电和三阶非线性光学性能     

基于吡咯并四硫富瓦烯结构的D-π-A型化合物的合成及其非线性光学性质的理论计算

以吡咯并四硫富瓦烯衍生物(1)为原料,经过Vilsmeier甲酰化、Wittig反应或交叉偶联反应得到D-π-A型化合物(6a,7a),为了比较N-甲基的影响,以N-甲基吡咯并四硫富瓦烯衍生物(2)出发,用同样的方法合成了N-甲基化的D-π-A型化合物(6b,7b). 用循环伏安法(CV)和UV-Vis研究了目标化合物的电化学和光物理性质,并进行了非线性光学性质的理论计算. 结果表明,目标化合物的紫外最大吸收波长在325～383 nm之间,具有较长共轭结构的化合物7a和7b显示出较好的三阶非线性光学性质, 它们在λ=1 064 nm基频下的三阶非线性系数γ值达5×10-33 esu.     

Theoretical studies of third-order nonlinear optical response for B12N12, B24N24 and B36N36 clusters

In this paper, we have calculated the third-order nonlinear optical polarizabilities corresponding to three optical processes: third-harmonic generation (THG), electric-field-induced second-harmonic generation (EFISHG) and degenerate four-wave mixing (DFWM) for B₁₂N₁₂, B₂₄N₂₄ and B₃₆N₃₆ clusters. The calculations have been performed by employing ab initio time-dependent density functional theory combined with sum-over-states method (SOS//TDDFT). We obtained the similar dynamic behavior of third-order NLO polarizabilities for three BN clusters. At input photon energy below 1.25 eV, the resonance enhancements of response haven't occurred. This is due to the fact that the calculated BN clusters have the large transition energy. B₂₄N₂₄ cluster has the larger transition dipole moments and the third-order polarizabilities of B₂₄N₂₄ are much larger than those of B₁₂N₁₂ and B₃₆N₃₆. We also estimate the static third-order optical susceptibility χ⁽³⁾ for BN fullerene materials from the average static third-order polarizability <γ>. The static χ⁽³⁾ of B₂₄N₂₄ fullerene materials are 1.36×10⁻¹⁴ esu for three NLO processes.     

Characterisation and theoretical investigation of the electronic properties and second-order nonlinearity of some three dentate salicylaldiminato Schiff base ligands

A series of asymmetric three dentate salicylaldiminato Schiff base ligands 1-4 (Scheme 1) has been synthesized and their structures, electronic properties and second order nonlinearities are investigated using the AM1 Hamiltonian SCF-MO methods. The analysis of MOs indicates that the O(2) atom could be the coordination site if the ligands were monodentate. In addition, the atomic orbitals on the O(9) atom have no contributions to the frontier MOs of the anionic form of these three dentate ligands. The Mulliken populations reveal that the coordination sites N(6) and O(9) possess different character in generation of the Schiff base complexes. The molecular first-order hyperpolarizability value of ligands was calculated using finite field method. Generally the presence of the methoxy group as third dentate play a major role in increasing the second harmonic generation (SHG) responses of three dentate ligands. Comparison of the NLO properties of two dentate with three dentate salicylaldiminine-based ligands reveals that the presence of -NO2 and -OCH3 groups as R1 and R2 substituents enhance the second-order nonlinear optic properties of these type ligands.     

13顶点金属碳硼烷结构和非线性光学性质的DFT研究

采用量子化学密度泛函理论(DFT)B3LYP/6-31G(d)方法,对4,1,6-MC2B10H1213顶点金属碳硼烷几何构型进行优化,结合有限场(FF)方法计算了它们的极化率和二阶非线性光学(NLO)系数.结果表明,十个13顶点金属碳硼烷分子中1a～6a的二阶NLO系数与其构型纵向扩张呈现相同的规律.分子的前线分子轨道能级差越小,其二阶NLO系数越大.对于不同自旋态的同种金属碳硼烷分子,其偶极矩值为高自旋态大于相应的低自旋态,极化率和二阶NLO系数与自旋多重度没有一致的对应规律,自旋多重度对NLO性质影响不大.     

A sum-over-state scheme of analysis of hyperpolarizabilities and its application to spiroconjugated molecular system

The static first and second hyperpolarizabilities of a number of spiromolecules with varying degree of polarity have been calculated at the HF and MP2 level using the 6-31+G* basis set and the B3LYP/6-31+G* optimized geometry. The variation of mean second hyperpolarizability in these molecular systems has been explained in terms of the ground state dipole moment, mean linear polarizability and second-order polarizability. A number of relationships among these quantities have been derived in the framework of the sum-over-state scheme and the generalized Thomas–Kuhn sum rule. The spiroconjugation results in the significant increase of the mean polarizability. The appreciable enhancement of first hyperpolarizability due to the spiroconjugation between two dipolar monomer units has been accounted for the rather significant increase of the mean polarizability tensor and the ground state dipole moment. The relatively larger value of the average second hyperpolarizability of the spiroconjugated molecules compared to that of the corresponding monomers arises from the rather significant increase of the nonaxial component γ _xxyy . The replacement of spirocarbon by spirosilicon results in the enhancement of the cubic polarizability manifold. The donor–acceptor substituted spirocompounds are predicted to be the superior third-order nonlinear optical (NLO) phores. The nature of π-conjugation in the monomer units around the spirocenter shows a strong modulation of the NLO properties of spirocompounds. The influence of electron correlation on the NLO properties at the MP2 level has been found to be rather significant.     

Novel ruthenium(II) complexes with substituted 1,10-phenanthroline or 4,5-diazafluorene linked to a fullerene as highly active second order NLO chromophores

Various Ru(II) complexes with substituted 1,10-phenanthroline or 4,5-diazafluorene are characterized by a good to very large second order NLO response, as determined by EFISH. Among these complexes, [Ru(9-fulleriden-4,5-diazafluorene)(PPh(3))(2)Cl(2)] is particularly appealing due to its huge second-order NLO response and its transparency to the second harmonic generation. The structure of cis-Cl,trans-PPh(3)-[Ru(5-NO(2)-1,10-phen)(PPh(3))(2)Cl(2))] was determined by single-crystal X-ray diffraction.     

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.     

Theoretical study on a novel series of fullerene-containing organometallics Fe(eta5-C55X5)2 (X = CH, N, B) and their large third-order nonlinear optical properties

Geometry structures, electronic spectra, and third-order nonlinear optical (NLO) properties of Fe(eta (5)-C 55X 5) 2 (X = CH, N, B) have first been investigated by time-dependent density functional theory. We analyzed the intramolecular interactions between ferrocene and the C 50 moiety. The calculated electronic absorption spectrum indicates that the short wavelength transitions are ascribed to the C 50 moiety mixed charge transfer transition of ferrocene itself, while the low energy excitation transitions are ascribed to the unique charge transfer transition from ferrocene to C 50 moiety in these systems. The third-order polarizability gamma values based on sum of states (SOS) method show that this class of ferrocene/fullerene hybrid molecule possesses a remarkably large third-order NLO response, especially for Fe(eta (5)-C 55B 5) 2 with the static third-order polarizability (gamma av) computed to be -10410 x 10 (-36) esu and the intrinsic second hypepolarizability to be 0.250. Thus, these complexes have the potential to be used for excellent third-order nonlinear optical materials. Analysis of the major contributions to the gamma av value suggest that the charge transfer from ferrocene to C 50 moiety along the z-axis (through Fe atom and the centers of two hybrid fullerenes) play the key role in the NLO response. Furthermore, boron substitution is an effective way of enhancing the optical nonlinearity compared to CH and N substitution, owing to smaller energy gap and better conjugation through the whole molecule.     

Reversible redox-switchable second-order optical nonlinearity in polyoxometalate: a quantum chemical study of [PW11O39(ReN)]n- (n = 3-7)

In this paper, the relationship between the reversible redox properties and the second-order nonlinear optical (NLO) responses for the title series of complexes has been systematically investigated by using the time-dependent density functional theory (TDDFT) method combined with the sum-over-states (SOS) formalism. The results reveal that the successive reduction processes of five PW11ReN redox states should be PW11ReVII (1) --> PW11ReVI (2) --> PW11ReV (3) --> PW11ReV1e ( 4) --> PW 11ReV2e (5). Furthermore, their electrochemical properties have been reproduced successfully. It is noteworthy that the second-order NLO behaviors can be switched by reversible redox for the present studied complexes. Full oxidation constitutes a convenient way to switch off the second-order polarizability (system 1). The incorporation of extra electrons causes significant enhancement in the second-order NLO activity, especially for the third reduced state (system 4), whose static second-order polarizability (betavec) is about 144 times larger than that of fully oxidized 1. The characteristic of the charge-transfer transition corresponding to the dominant contributions to the betavec values indicates that metal-centered redox processes influence the intramolecular donor or acceptor character. Therefore, these kinds of complexes with the facile and reversible redox states could become excellent switchable NLO materials.     

Prediction of second-order optical nonlinearity of trisorganotin-substituted beta-Keggin polyoxotungstate

The dipole polarizabilities, second-order polarizabilities, and origin of second-order nonlinear optical (NLO) properties of trisorganotin-substituted beta-Keggin polyoxotungstate [XW9O37(SnR)3](11-n)- (X = P, Si, Ge, R = Ph; X = Si, R = PhNO2, PhCCPh) have been investigated by using time-dependent density functional response theory. This class of organic-inorganic hybrid complexes possesses a remarkably large molecular second-order NLO response, especially for [SiW9O37(SnPhCCPh)3]7- (system 5) with the static second-order polarizability (beta(vec)) computed to be 1569.66 x 10(-30) esu. Thus, these complexes have the possibility to be excellent second-order nonlinear optical materials. Analysis of the major contributions to the beta(vec) value suggests that the charge transfer from the heteropolyanion to the organic segment along the z-axis plays the key role in the NLO response of [XW9O37(SnR)3](11-n)-. The computed beta(vec) values increase as a heavy central heteroatom changes in the order Ge > Si > P. Furthermore, nitro substitution on the aryl segment and the lengthening of organostannic pi-conjugation are more important in enhancing the optical nonlinearity, especially for the latter factor. The present investigation provides important insight into the origin of the NLO properties of trisorganotin-substituted heteropolyoxotungstate.     

Inorganic supramolecular compounds with 3-D chiral frameworks show potential as both mid-IR second-order nonlinear optical and piezoelectric materials

Two inorganic supramolecular compounds, (Hg(6)P(3))(In(2)Cl(9)) (1) and (Hg(8)As(4))(Bi(3)Cl(13)) (2), which have chiral 3-D host frameworks with guest moieties filling the helical tunnels, have been synthesized. They both have large second-harmonic generation efficiencies, and compound 2 also exhibits obvious single-crystal piezoelectric performance. Theoretical studies from first-principles calculations were performed on their nonlinear optical (NLO) and piezoelectric properties, and results indicate that good NLO and piezoelectric materials can be obtained by designing both complicated polycations and polyanions with large molecular polarizability as functional components rather than traditional single polyanions.