A-B2型含二苯甲酮的对硝基二苯乙烯类染料的合成、双光子性质与电化学

报道了3',4'-二(对苯甲酰基苯甲氧)基-4-硝基二苯乙烯(C1)的合成与表征. 研究了在不同溶剂中分子的吸收与荧光发射. 分子在可见光区的吸收可以归于生色团对硝基二苯乙烯部分的贡献, 而其在短波长区的吸收主要由二苯甲酮部分提供. 分子在中等极性溶剂中表现出较强的荧光发射. 系统研究了3',4'-二(对苯甲酰基苯甲氧)基-4-硝基二苯乙烯与2',4'-二(对苯甲酰基苯甲氧)基-4-硝基二苯乙烯(C2)两种A-B2型分子的双光子性质与电化学行为. 结果表明, 在800 nm波长的飞秒激光激发下, 两个分子皆表现出明显的上转换荧光发射, 其双光子吸收横截面的大小与二苯甲酮取代位置表现出一定的相关性. 分子结构优化与电化学的研究表明, 两个分子的电子密度分布与前线轨道能量亦与二苯甲酮取代位置表现出一定的相关性.     

二噻吩衍生物的合成及其线性、非线性光谱性质

合成了一系列二噻吩衍生物类有机合物：5，5'-二（对－N，N－二甲胺基苯乙 烯基）－2，2'－二噻吩（BMSBT）与5，5'－二（对－N，N－二乙胺基苯乙烯基）- 2,2'-二噻吩（BESBT），5,5'-二（对N－环丁胺基苯乙烯基）－2,2'－二噻吩（ BBSBT），5,5－二（对－N－咔唑基苯乙烯基）2-2'－二噻吩（BCSBT），并测定了 其吸收光谱、单光子荧光光谱和双光子荧光光谱。BMSBT，BESBT和BBSBT的单光子 荧光参数存在的很强的、规则的溶剂效应，表明其激发态的分子可能有较大的极性 。在800nm fs激光下测得BMSBT与BESBT在560nm附近（与单光子荧光发射峰波长接 近的位置）有较强的上转换荧光发射，上转换荧光强度与激发能量之间较好的平方 关系表明了双光子激发的机理，这种上转换荧光被称为双光子荧光。用以光子荧光 法测得BMSBT和BESBT的双光子吸收截面分别为54*10~(-50)(cm~4·s)/photon和 102*10~(-50)(cm~4·s)/photon。     

1,3,4-噁二唑衍生物的双光子吸收和双光子泵浦荧光

依据“推电子基-共轭中心-拉电子基-共轭中心-推电子基”的模型将电荷传输型1,3,4-噁二唑环嵌入芳香共轭体中, 通过Wittig-Horner反应合成了2种对称型强双光子吸收和双光子诱导荧光分子2,5-二[4-(2-芳基乙烯基)苯基]-1,3,4-噁二唑. 它们的氯仿溶液在锁模Nd: YAG激光器800 nm激光照射下, 发射出很强的双光子上转换荧光, 其最强荧光分别在波长507和475 nm. 采用非线性透过率法测得其双光子吸收截面分别为1.07×10^－46和6.6×10^－47 cm⁴•s•photon^－1. 这2个对称型D-π-A-π-D生色分子从激发端基到π共轭桥的有效能量传输, 对双光子吸收和双光子荧光发射能力贡献较大.     

新型树枝分子的宽带多光子荧光发射

用飞秒Ti∶sapphire激光研究了3个树枝分子1,2,4,5-四(4-N,N-二苯氨基苯乙烯基)苯(TPAB)、1,2,4,5-四[4-N,N-二(4-溴苯基)氨基苯乙烯基]苯(TPAB-Br)和1,2,4,5-四{4-{N,N-双{4-{4-[5-(4-叔丁基苯基)-1,3,4-噁二唑-2]苯乙烯基}苯基}氨基}苯乙烯基}苯(TPAB-OXA)的多光子吸收及上转换荧光性质.在二氯甲烷溶液中3个生色团分子TPAB,TPAB-Br和TPAB-OXA在800 nm飞秒光激发的双光子荧光发射波长分别为569,535和621 nm,在1300 nm飞秒光激发的三光子频率上转换荧光发射波长分别为566,534和610 nm,采用非线性透过率法测得在四氢呋喃(THF)溶液中TPAB,TPAB-Br和TPAB-OXA在800 nm和150fs激光激发下双光子吸收截面分别为61.86×10-50,6.19×10-50和65.98×10-50 cm4.s/photon;在1300 nm和80 fs激光激发下三光子吸收截面分别为3.88×10-79,7.76×10-79和27.17×10-79 cm6.s2.树枝分子具有很强的多光子吸收和上转换荧光发射能力,多光子荧光发射波长位于500～600 nm.     

双氰基二苯代乙烯型双光子荧光铅离子探针

以4-甲基-2,5-二氰基-4'-氨基二苯代乙烯(DCS)和双[2-(2-氨基苯基硫基)乙基]胺(BSA)分别作为双光子荧光团和铅离子配体,构建了1个新型的双光子荧光Pb2+探针(DPb),并对其结构和性能进行了表征.结果表明,该探针具有分子尺寸小、双光子吸收截面大(δ_(TPA),1020 GM)、长波长发射(λmax=609 nm)、斯托克斯位移大(209 nm)、光稳定性好、水溶性适宜、细胞渗透性优良、无细胞毒性及在生理环境下对p H不依赖等优点.该探针能选择性地检测细胞与组织中的Pb2+,猝灭常数K~(TP)_(sv)=7.58×10~5L/mol.     

1,2,3,4-四氢喹啉-4-酮衍生物的线性及非线性光学性质

合成了一系列具有刚性结构的推拉型1,2,3,4-四氢喹啉-4-酮衍生物: 1-苄基-1,2,3,4-四氢喹啉-4-酮(BTHQ)、2-(1,2,3,4-四氢喹啉-4-叶立德)丙二腈(THQM)、1,6-二羰基久洛尼定(DOJ)和1,6-二(二氰甲烯基叶立德)久洛尼定(BDCJ).测定了其吸收光谱、单光子荧光光谱和双光子上转换荧光光谱. 这类化合物的单双光子荧光参数都存在着很强的、规则的溶剂效应, 表明分子激发态可能存在较大的极性. 它们的二氯甲烷溶液在800 nm飞秒激光(150 fs)照射下, 能够发射出很强的双光子上转换荧光. 采用非线性透过率法测得四个化合物的双光子吸收截面在0.83～23.95×10－50 cm4•s•photon－1之间. 这类化合物的激发态存在有效的分子内电荷转移, 对双光子吸收和双光子荧光发射有较大贡献.     

D-π-A型三联吡啶衍生物的合成及光学性质

以4'-(4-甲苯基)-2,2'∶6',2″-三联吡啶为电子受体(A)基元,通过Wittig反应引入电子给体(D)基元,合成了2个新的D-π-A型三联吡啶衍生物;研究了其单、双光子吸收荧光特性,并通过量子化学计算从结构角度进行了解释.目标产物的荧光量子产率(Ф)最高达到0.45,双光子吸收截面(δ2)最大达406 GM.     

几个荧光蛋白发色团双光子吸收性质的理论研究

实验测得的荧光蛋白的单、双光子吸收光谱在低频和高频区域都表现出明显不同的特征。为了揭示这些不同点的起源和研究荧光蛋白的构–效关系,我们详细研究了三种荧光蛋白发色团(一种增强型蓝绿色荧光蛋白的中性发色团和两种红色荧光蛋白的阴离子发色团)的单、双光子吸收特性,分别计算了纯的和振动分辨的电子谱。计算结果表明：光谱线形与计算采用的交换相关密度泛函及谱截面计算所采用的近似关系密切;如果在计算光谱截面时,我们利用长程修正的交换相关泛函CAM-B3LYP来计算几何和电子结构参数,然后把Franck-Condon (FC)效应和包含Herzberg-Teller (HT)效果的电-声耦合效应都考虑进去,理论计算的光谱与实验测定的光谱可以很好地符合;对于两种离子态的发色团,HT电-声耦合效应使得对应于基态到第一激发态跃迁的双光子吸收最强峰相对于单光子吸收的最强峰发生了蓝移,但HT电-声耦合效应对高频的双光子吸收谱没有太大的影响;分子内电荷转移是导致高频区的双光子吸收明显强于单光子吸收的主要原因。     

具有双光子吸收特性的咪唑类衍生物的合成及其光物理性能研究

分子在强激光作用下能同时吸收两个光子的现象称为双光子吸收(TPA),具有大的双光子吸收截面(σ2)的分子有多种用途,是目前光电子材料研究领域的热点之一.双光子吸收材料可应用于上转换激射[1]、光限幅[2]、光稳幅、三维光存储[3]、三维微加工[4,5]以及光动力疗法[6]等.但由于一般材料的双光子吸收截面很小,大大限制和束缚了双光子吸收材料的发展应用.     

荧光素卟啉分子间分子内能量及电子转移反应

合成了以共价键相连的荧光素-卟啉二元分子.研究了荧光素酯与卟啉分子间和分子内的能量及电子转移过程.分子间的荧光猝灭实验表明,当激发荧光素时,荧光素的单重态能量有效地传给卟啉,动态荧光猝灭速度常数(k_d)为1.3×10~(12)s~(-1)·mol~(-1)L.吸收光谱和NMR谱结果表明荧光素与卟啉间有基态相互作用,其静态荧光猝灭速度常数(k_s)为3.6×10~(12)s~(-1)·mol~(-1)·L.在二元分子中,当激发荧光素时,从荧光素到卟啉的单重态能量传递效率在0.90以上,速度常数为 1.2×10~(10)S~(-1)·mol~(-1)·L,溶剂极性对其影响不大.当激发卟啉时,在极性溶剂中发生了电子转移,其转移效率为0.51,速度常数为2.3×10~8s~(-1)·mol~(-1)·L.     

Synthesis and Nonlinear Optical Properties of a New A-π-A Two-Photon Compound Utilizing Dibenzothiophene as Center

A new two‐photon material, 3E,6E‐bis(2‐pyrid‐4′‐ylvinyl)dibenzothiophene (BPVDBT), has been firstly synthesized by an efficient Pd‐catalyzed Heck coupling route. The single‐ and two‐photon fluorescence, quantum yields, lifetimes, solvent effects of the chromophore were studied in detail and the compound exhibited solvent‐sensitivity. The fluorescence intensity (I_out) and input excitation intensity (I_in) can fit in well with the quadratic parabolas, which indicates that the up‐converted fluorescence was induced by the two‐photon absorption (TPA). TPA cross‐section of BPVDBT has been measured using the two‐photon‐induced fluorescence method, whose value is 14.24×10^?50 cm⁴·s·photon^?1·molecule^?1 at 750 nm. The experimental results confirm that BPVDBT is a good two‐photon absorbing chromophore with an A‐π‐A type.     

一个新的具有大的吸收截面的双光子引发剂的合成和非线性光学性质

E,E-1,4-Bis（4＇-N,N-diphenylaminostyryl）-2,5-dimethoxybenzene （DPAMOB） has been synthesized by a simple and effective solid phase Wittig reaction and characterized by 1^H NMR spectra and elemental analysis, Linear absorption, single-photon induced fluorescence and two-photon induced fluorescence spectra were experimentally studied. The new dye has a large two-photon absorption （TPA） cross-section of σr= 1007,2 GM [1 GM= 1 × 10^-50 cm^4·s/（photon molecule）] at 800 nm measured by the two-photon induced fluorescence method. The experimental results confirm that DPAMOB is a good TPA chromophore and can successfully initiate two-photon photopolymerization of ethoxylated trimethylolpropane triacrylate esters （SR454）. Finally, a microstructure has been fabricated by use of DPAMOB as initiator.     

Growth and Spectroscopic Characteristics of Yb3＋：LiGd（WO4）2 Crystal

The Yb3+:LiGd(WO4)2 crystal with the dimension of Φ15×35 mm3 was grown by Czochralski technique. The spectroscopic characterization and fluorescence dynamics of Yb3+ in Yb3+:LiGd(WO4)2 crystal were investigated. The Yb3+:LiGd(WO4)2 crystal exhibits a broad absorption band centered near 975 nm with the linewidths of 16 and 11 nm and maximal absorption cross-section of 3.60 × 10-20 and 2.90 × 10-20 cm2 for π- and σ-polarization, respectively. The emission broadband has an FWHM of 47 and 45 nm with the emission cross sections of 3.92 × 10-20 and 3.34 × 10-20 cm2 at 1020 nm for π- and σ-polarization, respectively. The measured fluorescence lifetime is 398 μs. The blue light emission around 480 nm through cooperative upconversion from the de-excitation of excited Yb3+-Yb3+ pairs at 4 K was observed under 932-nm excitation and demonstrated.     

Synthesis and Properties of a New Two—Photon—absorbed Material DMAEAS

IntroductionSubstitutedstilbeneshavesignificantpotentialapplica tionssuchasfluorescencemicroscopy ,two photonphotody namictherapy ,opticalpowerlimiting ,three dimensionalstorage,andthree dimensionalmicrofabrication .1 4 Thesedyeshavestrongtendencyofintra molecularchargetransferundertheexcitedstate.Asaresult,theyusuallyexhibitlargetwo photonabsorption (TPA) ,inthemeanwhileemitstrongup convertedfluorescence .Ontheotherhand ,theirsolutionsgenerallydisplaylineartransmissionof >90 %atwavelengthof…     

亚甲基蒽苯乙烯吡啶盐的合成、结构及双光子吸收性质

以氯化4-甲基-N-9-亚甲基蒽吡啶盐为原料,合成了一种新型的苯乙烯吡啶盐,通过红外、核磁共振氢谱、碳谱、电喷雾质谱、单晶X射线衍射等测试技术对化合物的结构进行了表征。单晶X射线衍射结果表明,该化合物属于单斜晶系,空间群为P21/c,晶胞参数a=1.255 7(1)nm,b=1.539(1)nm,c=2.220 2(8)nm,β=101.099(1)°,V=4.210 5(4)nm3,Z=4,Dc=1.159 g/cm3。用1 064 nm皮秒脉冲激光研究其三阶非线性光学特性,双光子吸收系数β=0.028 cm/GW,吸收截面为σ=8.68×10-48cm4.s.photon-1,表明目标化合物具有良好的三阶非线性光学性质。     

Measurement of strong nonlinear absorption in stilbene-chloroform solutions,explained by the superposition of two-photon absorption and one-photon absorption from the excited state

A strong nonlinear absorption is measured when ruby laser light passes through a solution of stilbene in chloroform. The experimental results are interpreted by the use of the following model: two-photon absorption (TPA) is followed by one-photon absorption (OPA) by the excited molecules. The solution of the corresponding system of rate equations and fitting of parameters to the experimental curve give the TPA cross section σ⁽²⁾ = 8 × 10^?49 cm⁴ sec/photon and the product σ⁽¹⁾ τ₁₀ = 3 × 10^?26 cm² sec. Measurements at other frequencies are in agreement with this model.     

Alternating copolymers of 2,6‐bis(p‐dihexylaminostyryl)anthracene‐9,10‐diyl and N‐octylcarbazole with large two‐photon cross sections

We report the synthesis, thermal, one‐ and two‐photon properties of poly(2,6‐bis(p‐dihexylaminostyryl)anthracene‐9,10‐diyl‐alt‐N‐octylcarbazole‐3,6‐/2,7‐diyl) ( P1/P2 ). The as‐synthesized polymers exhibit number‐average molecular weights of 1.7 × 10⁴ for P1 and 2.1 × 10⁴ g/mol for P2 . They emit strong one‐ and two‐photon excitation fluorescence with the peak around 502 nm, and the fluorescence quantum yields around 0.76 in chloroform. In film state, P1 and P2 show different red‐shift emission with the peaks at 512 nm and 523 nm, respectively. The DSC measurement reveals that as‐synthesized polymers are all amorphous aggregates with the glass transition temperatures of 131 °C for P1 and 152 °C for P2 . The solution two‐photon absorption (TPA) properties of P1 and P2 in chloroform are measured by the two‐photon‐induced fluorescence method using femtosecond laser pulses (120 fs). The TPA cross sections (δ) are measured over the range of 700–900 nm. The maximal δ of P1 and P2 all appear at ～800 nm and are 1010 GM and 940 GM per repeating unit, respectively. This suggests that no notable interactions among structure units that impair their fluorescence and TPA properties, and the polymers with large δ can be obtained by using the high TPA‐active units as building blocks. © 2010 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem, 2010     

Ultrafast dynamics in multibranched structures with enhanced two-photon absorption

The understanding of the mechanism of the enhanced two-photon absorption (TPA) in multibranched chromophore systems is of importance to the design of materials with the large TPA cross-sections and for future applications. In this communication, the mechanism of enhanced TPA properties is investigated. For a dendritic model system, the excited-state dynamics for both population (T1-process) and phase relaxation (T2-process) processes involved are investigated by a combination of time-resolved spectroscopic techniques. The results of time-resolved fluorescence anisotropy are compared with previous results obtained from other branched chromophore systems. It is found that the PRL-701 trimer system, which possesses the large enhancement of two-photon absorption cross-section, gives a faster anisotropy decay (fluorescence upconversion and transient absorption), a longer population relaxation time (fluorescence lifetime), and a weaker coupling to the solvent (a larger photon echo peak shift initial value). New strategies for rational design of large TPA materials can be achieved based on a better understanding of the mechanism of the enhancement.     

以N为耦合中心多枝分子的双光子上转换荧光

采用非线性透过率法研究了以N为耦合中心的多枝化合物N-[4-{2-(3,5-二-[5-(4-叔丁基苯基)-1,3,4-噁二唑-2-]苯基}-1-乙烯基}苯基}-N,N-二苯胺(BPODPA), N,N-双[4-{2-(3,5-二-[5-(4-叔丁基苯基)-1,3,4-噁二唑-2-]苯基}-1-乙烯基}苯基}-N-苯胺(BBPOPA)和N,N,N-三[4-{2-(3,5-二-[5-(4-叔丁基苯基)-1,3,4-噁二唑-2]苯基}-1-乙烯基}苯基}胺(TBPOA)的双光子吸收性质, 测定了化合物的单光子荧光光谱和双光子上转换荧光光谱, 研究了多枝化对三苯胺分子双光子吸收和双光子激发荧光性质的影响.在800 nm波长的激光激发下,化合物BPODPA、BBPOPA和TBPOA在二氯甲烷溶液中发出很强的蓝绿色双光子上转换荧光, 荧光峰分别位于502、515 和518 nm. 这些多枝结构化合物的双光子吸收截面较大, 双光子吸收增强来源于多枝分子中扩展的π共轭体系和重复单元的协同效应.     

Conformationally tuned large two-photon absorption cross sections in simple molecular chromophores

We investigate here the relationship between molecular architecture and two-photon absorption (TPA) processes in a class of alkyl-substituted 4-quinopyran chromophores. We find that TPA cross sections diverge as the one-photon gap energy nears one-half of the two-photon gap. The molecular strategy proposed here to tune these two-excitation gaps for maximizing TPA cross sections is to twist the molecule about the bond connecting the chromophore donor and acceptor phenylene fragments. Extremely large TPA cross sections, determined by the absorption bandwidth, can then be realized (imaginary part of the third-order polarizability approximately 2.6 x 10(5) x 10(-36) esu) for fundamental photon energies near 1.0 eV, when the torsional angle approaches 104 degrees. The required torsional angle is achieved by introduction of sterically encumbered 2,2',2' ',2' " tertiary alkyl substituents.