溶剂对N-{4-[(反式)-2-(4-硝基苯基)乙烯基]苯基}-N,N-二苯氨基分子双光子吸收特性的影响

在从头计算的基础上,利用两态模型对溶剂对N-{4-[(反式)-2-(4-硝基苯基)乙烯基]苯基}-N,N-二苯氨基分子双光子吸收特性的影响进行了理论研究.计算结果表明,溶剂对该分子的双光子吸收截面影响较大,双光子吸收截面随着溶剂极性的增加而增加.     

两个新合成化合物EPVPC和OPVPC非线性光学特性的理论研究

在杂化密度泛函理论（DFT/B3LYP）的水平上，研究了最新实验室合成的两个化合物分子9-乙烷基-3-{2-[4-2-吡啶-4-乙烯基苯]-乙烯基}-9氢咔唑（EPVPC）和9-十八烷基-3-{2-[4-2-吡啶-4-乙烯基苯]-乙烯基}-9氢咔唑（OPVPC）的非线性光学特性。理论结果与现有的实验测量结果符合得的较好。利用扩展的少态模型方法计算了分子的双光子吸收截面，结果表明三态模型可以很好地描述它们的最大双光子吸收截面。数值模拟显示这两个化合物都具有较大的双光子吸收截面，并且，在低频范围内，OPVPC分子比EPVPC分子显示出较强的双光子吸收特性。     

新型多共轭链有机分子双光子吸收特性的理论研究

在密度泛函理论水平上,利用解析响应函数方法研究了以（4-{2-［4-（2-吡啶-4-乙烯基）-苯基］-乙烯基}-苯基）-胺为基本结构单元的单支、双支和三支共轭链有机分子的单光子和双光子吸收特性.计算结果表明,这三种有机分子都具有较大的线性和非线性吸收强度.在紫外-可见光区域,它们的单光子吸收谱都存在两个峰,这与实验结果符合较好.在近红外区域,多共轭链有机分子呈现出宽达300 nm的宽带双光子吸收,单支、双支和三支分子的最大双光子吸收截面比约为1.0∶2.3∶4.0,其中三支分子具有最大的双光子吸收截面101.73×10^-48 cm⁴·s.从理论上进一步证实,增加分子的共轭链可有效提高分子的双光子吸收特性.同时还给出了电荷转移态的电荷迁移过程. 关键词： 双光子吸收 响应函数方法 多共轭链有机分子     

一种新型双共轭链分子非线性光学性质的理论研究

对实验室合成的双共轭链分子1,4-二(4-二乙胺基苯乙烯基)-2-［4-(N-甲基-N-羟乙基)氨基-4′-硝基偶氮苯］-5-己烷氧基苯(BSBAB)及合成它的单共轭链分子的单光子和双光子吸收特性在从头计算的基础上利用密度泛函理论进行了研究.分子BSBAB的优化结构显示，组成该分子的横链和纵链除了保持各自的共轭面外，几近相互垂直.因此，分子BSBAB较好地继承了两个单共轭链分子的光学特性.计算结果表明，在低能量范围内，分子BSBAB具有三个双光子吸收峰，分别来自于两个单共轭链分子以及两者的耦合作用.从理论上证明了双共轭链分子BSBAB是一种具有宽带强双光子吸收的分子材料.理论结果和实验结果符合得较好.在HF水平上的响应函数方法进一步证实了有限态求和方法计算结果的可靠性.还给出了电荷转移态的电荷迁移过程. 关键词： 双光子吸收 双共轭链有机分子 非线性光学     

(E,E)-1,4-双{2''-[5''-(B,B-二甲基苯硼)-2-噻吩基]乙烯基}-苯分子双光子吸收特性的理论研究

在密度泛函水平上,利用响应函数方法,研究了分子的单光子和双光子吸收特性.计算出了该分子在低能量范围内的最大双光子吸收截面为6.47×10-47cm4s/photon,与实验符合的较好.研究结果表明该分子具有较强的双光子吸收特性,是较好的双光子吸收材料.     

一种新型偶氮化合物的纳秒光限幅特性研究

研究了反式—4—{[p—(N,N—二羟乙基胺基)偶氮苯]乙烯基}吡啶在N,N—二甲基甲酰胺(DMF)中的光限幅性能。实验结果表明,该偶氮化合物的DMF溶液对波长为532nm,脉冲宽度为8ns的激光脉冲具有很强的光限幅特性。理论分析表明,光限幅效应主要起源于材料的双光子吸收。利用双光子吸收模型拟合光限幅实验数据得到材料的双光子吸收系数β=1.6×10-9cm/W。     

(E,E)-1,4-双{2''-[5''-(B,B-二甲基苯硼)-2-噻吩基]乙烯基}-苯分子双光子吸收特性的理论研究

在密度泛函水平上,利用响应函数方法,研究了分子的单光子和双光子吸收特性.计算出了该分子在低能量范围内的最大双光子吸收截面为6.47×10-47 cm4 s/photon,与实验符合的较好.研究结果表明该分子具有较强的双光子吸收特性,是较好的双光子吸收材料.     

多维树枝状有机分子的双光子吸收特性

利用响应理论方法,研究了新近合成的以二-(苯乙烯基)苯为主干的多分枝有机物的双光子吸收特性.结果表明这些多维有机分子显示了较好的双光子吸收特性,其中A-π-A型的有机分子具有较大的双光子吸收截面,进一步说明了到底是对称型的还是不对称型的有机分子具有大的双光子吸收截面还与分子的π中心有关.     

多维树枝状有机分子的双光子吸收特性

利用响应理论方法，研究了新近合成的以二-(苯乙烯基)苯为主干的多分枝有机物的双光子吸收特性。结果表明这些多维有机分子显示了较好的双光子吸收特性，其中A-π-A型的有机分子具有较大的双光子吸收截面，进一步说明了到底是对称型的还是不对称型的有机分子具有大的双光子吸收截面还与分子的π中心有关。     

1，4-二甲氧基-2，5-二乙烯基苯系列衍生物的双光子吸收截面

在HF水平上，利用解析响应函数方法，研究了1，4_二甲氧基_2，5_二乙烯基苯系列衍生物 分子的单光子和双光子吸收特性. 实验测量了反，反_2，5_双(4′_N,N_二丁胺基苯乙烯)_1 ，4_二甲氧基苯分子的单光子和双光子荧光谱. 研究结果表明该系列分子具有较强的双光子 吸收特性. 在低能量范围内，对于D_π-A型分子，分子的单光子吸收强度和双光子吸收截面 最大值都发生在分子的第一激发态. 对于D_π_D型分子，单光子吸收强度最大值出现在分子 的第一激发态，而最大双光子吸收值则对应于分子的第二激发态. 分子的单和双光子吸收强 度和分子官能团的电性有关. 对于由该类π中心部分构成的分子，其对称型不一定比不对称型更有利于提高双光子吸收截面. 分子基态与电荷转移态的电荷转移过程定性地解释了双光 子聚合反应的聚合机理. 关键词： 双光子吸收 响应函数方法 非线性光学     

Solvent effects on optical properties of a newly synthesized two-photon polymerization initiator： BPYPA

Time-dependent hybrid density functional theory in combination with polarized continuum model is applied to study the solvent effects on the geometrical and electronic structures as well as one- and two-photon absorption processes, of a newly synthesized asymmetrical charge-transfer organic molecule bis-（4-bromo-phenyl）-[4-（2-pyridin-4-yl-vinyl）phenyl]-amine （BPYPA）. There exist two charge-transfer states for the compound in visible region. The two-photon absorption cross section calculated by a three-state model and solvatochromic shift of the charge-transfer states are found to be solvent-dependent, where a nonmonotonic behaviour with respect to the polarity of the solvents is observed. The numerical results show that the organic molecule exhibits a rather large two-photon absorption cross section as compared with the compound 4-trans-[p-（N, N-Di-n-butylamino）-p-stilbenyl vinyl] pyridine （DBASVP） reported previously, and is predicted to be a good two-photon polymerization initiator. The hydrogen-bond effect is analysed. The computational results are in good agreement with the measurements.     

The theoretical studies on the two-photon absorption properties of symmetric 1,4-bis{2-[4-（2- aryl） phenyl] vinyl }- 2,5-bisdialkoxyb enzenes

On the level of the time-dependent hybrid density functional theory, the one- and two-photon absorption properties of a series of symmetric 4-bis 2-[4-(2-ary12) phenyl]vinyl-2,5-bisdialkoxybenzenes are studied respectively utilizing the analytic response theory and the few-state model methods. The calculated results show that the planarity of the geometrical structure plays a great role in enhancing the linear and nonlinear optical abilities of the molecule. However the effect of the length of the chain linked to the π-centre on the optical property is very little. For the investigated compounds, the A–π–A type charge-transfer molecules display more superior one- and two-photon absorption characteristics than the D–π–D type ones. Furthermore, the two-photon absorption results by use of few-state model are generally consistent with those by analytic response theory, demonstrating the reliability of the few-state model for evaluating the two-photon absorption cross section. The numerical simulations are in good agreement in tendency with the available experimental measurements.     

Static and Ultrafast Transient Photophysics of Mono- and Dual-Branched Triarylamines

Mono- and dual-branched molecules, { 4-[2-（4-benzothiazol-2-yl-phenyl）-vinyl]-phenyl}-（4-methoxy-phenyl）-phenyl- amine （BS1） and bis-{4-[2- （4-benzothiazol-2-yl-phenyl）-vinyI]-phenyl}-（4-methoxy-phenyI）-phenyl-amine （BS2）, are investigated with one- and two-photon static spectroscopy, and the femtosecond fluorescence up-conversion technique. The molecules show branch-based fluorescence emission at low quantum yield. U1trafast non-radiative decay on a picosecond time scale is found and is attributed to intramolecular charge-transfer bridged by the central triphenylamine. The two-photon absorption cross-sections of BS1 and BS2 are 19.1 and 19.4 GM, respectively.     

Resonant propagation of femtosecond laser pulse in DBASVP molecule：one-dimensional asymmetric organic molecule

We have investigated the resonant propagation of femtosecond laser pulse in 4-trans-[p-（N, N-Di-n-butylamino）- p-stilbenyl vinyl] pyridine medium with permanent dipole moments. The electronic structures and parameters for the compound have been calculated by using density functional theory. In the optical regime, there is one charge-transfer state, and the molecule can thus be simplified as a two-level system. Both the one- and two-photon transitions occur between the ground and charge-transfer states. The numerical results show that the permanent dipole moments have an obvious effect on the propagation of the ultrashort pulse laser. The ideal self-induced transparency disappears for 2π pulse, and second harmonic spectral components occur significantly due to the two-photon absorption process. For the 6π pulse, continuum frequency generation is produced and a shorter duration pulse in time domain with 465 as is obtained.     

Synthesis, characterization and studies on the nonlinear optical parameters of hydrazones

Three hydrazones, 2-(4-methylphenoxy)-N′-[(1E)-(4-nitrophenyl)methylene]acetohydrazide (compound-1), 2-(4-methylphenoxy)-N′-[(1E)-(4-methylphenyl)methylene]acetohydrazide ((compound-2) and N′-{(1E)-[4-(dimethylamino)phenyl]methylene}-2-(4-ethylphenoxy) acetohydrazide(compound-3) were synthesized and their third order nonlinear optical properties were investigated using a single beam z-scan technique with nanosecond laser pulses at 532 nm. Open aperture data obtained from the three compounds indicates two photon absorption at this wavelength. The nonlinear refractive index n₂, the nonlinear absorption coefficient β, the magnitude of the effective third order susceptibility χ⁽³⁾, the second order hyperpolarizability γ_h and the coupling factor ρ have been estimated. The values obtained are comparable with the values obtained for 4-methoxy chalcone derivatives and dibenzylidene acetone derivatives. Among the compounds studied, compounds-1 and 3 exhibited the better optical power limiting behaviour at 532 nm. Our studies suggest that compounds-1, 2 and 3 are potential candidates for optical device applications such as optical limiters and optical switches.     

Synthesis and Characterization of New Y-shaped Fluorophores with an Imidazole Core

Four new y-shaped fluorophores of 4- {4,5-[2,2'-Bis(2,4,6-trimethoxyphenyl)vinyl]-1-H-imidazole-2-yl}benzonitrile 1a, 2-phenyl-{4,5-[2,2'-Bis(2,4,6-trimethoxyphenyl)vinyl]-1-H-imidazole} 1b, 2- (9-anthryl)-{4,5-[2,2'-Bis(2,4,6-trimethoxyphenyl)vinyl] }-1-H-imidazole 1c and 2- (4-nitrophenyl) - {4,5-[2,2'-Bis(2,4,6-trimethoxyphenyl)vinyl] -1-H-imidazole 1d which bear an imidazole core, were synthesized for the first time via intermediate 1,6-Bis(2,4,6-trimethoxyphenyl)hexa-1,5-diene-3,4-dion with different aldehydes. The structures of the new derivatives were confirmed by (1)H NMR, (13)C NMR and FT-IR. The optical properties such as absorption and emission maxima, Stokes' shift and quantum yield values were investigated in solvents of toluene, tetrahydrofuran and acetonitrile. The products show intense emission maxima in the range of 440-630?nm. The imidazole derivatives exhibited excellent photostabilities.     

Two-photon absorption properties of aggregation systems on the basis of (E)-4-(2-nitrovinyl) benzenamine molecules

Aggregation effect caused by the intermolecular hydrogen-bonding interactions on two-photon absorption properties of (E)-4-(2-nitrovinyl) benzenamine molecules is studied at a hybrid density functional level. The geometry optimization studies indicate that there exist two probable conformations for the dimers and three for the trimers. A strong red-shift of the charge-transfer states is shown. The two-photon absorption cross sections of the molecule for certain conformations are greatly enhanced by the aggregation effect, from which a ratio of 1.0:2.6:3.6 is found for the molecule and its dimer and trimer with nearly planar structures. Namely, a 30 or 20 percent increase of the two-photon absorption cross section is observed.     

White organic light-emitting device with\ both phosphorescent and fluorescent emissive layers

This paper reports the fabrication of novel white organic light-emitting device（WOLED） by using a high efficiency blue fluorescent dye N-（4-（（E）-2-（6-（（E）-4-（diphenylamino）styryl）naphthalen-2-yl）vinyl）phenyl）oN- phenylbenzenamine （N-BDAVBi） and a red phosphoresecent dye bis （1-（phenyl） isoquinoline） iridium （III） acetylanetonate （Ir（piq）2（acac））. The configuration of the device was ITO/PVK：TPD/CBP： N-BDAVBi /CBP/ BALq： Ir（piq）2（acac）/BCP/Alq3/LiF：AL. By adjusting the proportion of the dopants （N-BDAVBi, Ir（piq）2（acac）） in the light-emitting layer, white light with Commission Internationale de l＇Eclairage （CIE） coordinates of （0.35, 0.35） and a maximum luminance of 25350cd/m2 were obtained external quantum and current efficiency of 6.78% and between the two light-emitting layers and using BCP at an applied voltage of 22V. The WOLED exhibits maximum 12cd/A respectively. By placing an undoped spacer CBP layer as hole blocking layer, the colour stabilization slightly changed when the driving voltage increased from 6 to 22 V.