F?rster双分子猝灭作用对卟啉侧链聚合物荧光衰变的影响

通过采用时间分辨荧光光谱技术测量了一种卟啉侧链聚合物薄膜：卟啉丙烯酸酯—苯乙烯共聚物poly［porphyrin acrylate-styrene］ (P［(por)A-S］)在高激发密度下的瞬态荧光特性.实验发现,P［(por)A-S］样品的荧光衰减随聚合物分子浓度的增大而加快.利用Frster机制的双分子猝灭理论对其浓度猝灭的原因进行了分析,理论结果与实验结果符合较好.研究表明,在高激发密度的情况下,Frster机制的双分子作用是加快卟啉侧链聚合物初始荧光衰减和降低其发光效率的主要因素. 关键词： 双分子猝灭 Frster机制 瞬态荧光 卟啉侧链聚合物     

激子旋转弛豫对低掺杂卟啉侧链聚合物荧光衰变过程的影响

利用激子旋转扩散理论研究了一类低掺杂卟啉侧链聚合物中卟啉侧链基团的旋转对其发光动力学过程的影响.研究表明,卟啉侧链基团的旋转行为是导致激发态无辐射能量弛豫的重要途径.基团旋转越容易,能量弛豫速度越快,这可导致一个快速的荧光衰变动力学过程.在卟啉低掺杂浓度和聚合物分子链间距离较大的情况下,卟啉侧链基团的旋转成为影响荧光寿命和发光效率的主要因素.对实验测得的两种样品的荧光弛豫过程进行了拟合,理论结果与实验结果符合较好. 关键词： 激子旋转弛豫 瞬态荧光 卟啉侧链聚合物     

分子链间距离对于卟啉侧链聚合物稳态及瞬态发光性能的影响

采用荧光光谱技术,测量了一种卟啉侧链聚合物:卟啉丙烯酸酯-苯乙烯共聚物(P[(por)A-S])的稳态和瞬态的发光性能.通过将聚合物P[(por)A-S]掺杂到有机玻璃(PMMA)中,研究了链间距离对于P[(por)A-S]发光性能的影响.结果表明:随着聚合物分子浓度增大,即链间距离减小,导致卟啉侧链基团之间的相互间作用增加,使其激发态无辐射跃迁几率增加,聚合物荧光强度减弱,激发态寿命缩短.讨论了上述过程产生的原因.     

侧链基团对聚合物薄膜瞬态发光性能的影响

采用飞秒激光光谱技术比较研究了两种卟啉侧链聚合物:卟啉丙烯酸酯-苯乙烯共聚物P[(por)A-S]和卟啉铁(Ⅲ)丙烯酸酯-苯乙烯共聚物P[(por)FeA-S]的瞬态发光性能。并采用纳秒激光光谱技术测量了小分子卟啉(TPP)的荧光动力学过程。结果表明:P[(por)FeA-S]具有比P[(por)A-S]快得多的荧光弛豫过程,而P[(por)A-S]的荧光寿命远小于小分子卟啉的荧光寿命。对上述过程进行了分析,P[(por)A-S]的荧光衰变主要来源于聚合物分子链间的相互作用;而P[(por)FeA-S]的荧光衰变除了来源于聚合物分子链间的相互作用外,中央金属离子与配位体之间的电荷转移也对卟啉发色基团的激发态超快无辐射弛豫具有重要的影响,对上述过程的产生机理进行了讨论。     

一种新型卟啉侧链聚合物的飞秒荧光动力学

研究了一种新型的卟啉侧链聚合物丙烯腈丙烯酸卟啉酯共聚物{poly[porphyrin acrylate-acrylonitrile](p[(por)A-AN]}的链间和链内的卟啉分子的相互作用对聚合物薄膜发光性质的影响。通过采用飞秒荧光光谱技术测量了p[(por)A-AN]薄膜的荧光动力学过程。测量结果表明:纯p[(por)A-AN]薄膜(~450ps)显示出了比混合物薄膜p[(por)A-AN]/polystyrene(PSE)(~1.3 ns)快得多的荧光弛豫过程。而p[(por)A-AN]/PSE混合物薄膜显示出较纯p[(por)A-AN]薄膜增强的荧光效率。增加p[(por)A-AN]分子内卟啉侧链基团的浓度导致纯p[(por)A-AN]薄膜和p[(por)A-AN]/PSE混合物薄膜的荧光效率的增强和寿命(由近26~36 ps)的增加。分子间和分子内卟啉侧链基团之间的无辐射能量转移和分子内卟啉侧链基团的旋转运动在p[(por)A-AN]的荧光动力学过程中起着重要的作用。     

纳米银粒子表面吸附染料分子的荧光增强及荧光猝灭现象

本文通过阴、阳离子型染料分子荧光素钠(FS)及若丹明6G(Rh6G)吸附在银胶体系内纳米银颗粒表面上,首次发现了FS的荧光增强谱及Rh6G的荧光猝灭谱.引起荧光增强及荧光猝灭的因素,除局域场和分子到金属表面能量转移这两个方面外,还与纳米银表面与被吸附分子之间的距离有关.     

硫堇同步荧光猝灭法测定痕量铁(Ⅲ)

研究了硫堇（TH）的同步荧光光谱（△λ=10nm）,消除了瑞利散射的干扰,并确定λ_ex=624nm,λ_em=634nm。进一步观察了Fe³⁺对硫堇同步荧光的猝灭作用,并在同步荧光猝灭度（△F）与Fe³⁺质量浓度(pFe³⁺)之间建立了良好的线性关系（△F=536.3p、r=0.9986）。Fe³⁺的线性范围0.0283—0.890μg·mL^-1,检出限为0.0085μg·mol^-1,加标回收率为96.7%—104.6%。该方法选择性高,稳定性好,用于3种不同啤酒样品中的痕量铁的测定,结果满意。     

荧光猝灭法对超支化聚合物囊泡温敏性翻转的研究

本文利用稳态瞬态荧光光谱法对硝酸铊猝灭芘标记超支化聚合物囊泡的机理进行了探讨,并将猝灭实验应用于超支化聚合物囊泡温敏性翻转的研究。结果发现,硝酸铊对芘标记超支化聚合物囊泡的猝灭属于动态过程,并且有选择性地猝灭囊泡双分子层的外层;聚合物链段温敏性的转变,引起该链段在囊泡双分子层间的再分布,从而导致超支化聚合物囊泡翻转。     

烷烃类分子对NCO(A2∑+)自由基的猝灭

采用激光光解 激光诱导荧光 (LP LIF)的方法 ,用 2 6 6nm激光光解CHBr3 分子产生CH自由基 ,再与N2 O继续反应作为NCO自由基的产生源 ,用 4 38.6nm激光将电子基态X 2 Πi(0 0 10 )的NCO激励到激发态A2 Σ+ (0 0 0 0 )上 ,通过检测激发态NCO时间分辨荧光信号 ,测得室温 (2 98K)下NCO(A2Σ+ )被烷烃类分子猝灭的实验结果 ,获得了A 2Σ+ (0 0 0 0 )态猝灭速率常数 .实验发现 ,随着烷烃分子中C -H键数增加 ,其猝灭截面也近线性增加 ,但随着分子体积增大 ,这种增加趋缓 .     

银纳米粒子对抗生素诺氟沙星的荧光猝灭效应

以β-环糊精(β-CD)为稳定剂,葡萄糖为还原剂,采用"绿色化学方法"合成了平均粒径约为31nm的类球形银纳米粒子。研究了其对水溶液中痕量诺氟沙星荧光行为的影响,实验结果表明,制得的银纳米粒子对诺氟沙星具有较强的荧光猝灭效应,且随着加入银纳米粒子量的增加荧光猝灭效果逐渐增强。初步探讨了银纳米粒子对诺氟沙星的荧光猝灭机理。     

The effect of intermolecular interactions on photoluminescence of a porphyrin side-chain polymer

Photoluminescence properties and exciton decay dynamics in a porphyrin side-chain polymer, poly[porphyrin acrylate- acrylonitrile (abbreviated p[(por)A-AN]), have been investigated by femtosecond time-resolved photoluminescence spectroscopy. All the luminescences of p[(por)A-AN] films are due to the emissive decay of the photoexcited singlet excitons in the porphyrins. The luminescence efficiencies and lifetimes are increased for samples from pure films to dilute blend films. However, they are increased as the intrachain concentration of the porphyrin sidechain groups is decreased. The intrachain rotation motions of porphyrin sidechain groups result in the initial ultrafast luminescence decays, which are much faster than those due to the interchain interactions. All the samples show no significant red-shift and broadening of the transient luminescence spectra. The interchain and intrachain nonradiative exciton relaxation processes may play an important role in the luminescence dynamics in the p[(por)A-AN] films. The possible origin of different intrachain and interchain dynamic behaviours in p[(por)A-AN] films is discussed.     

Kinetics of annihilation of triplet excitationsand decay of delayed fluorescence for isolated 1,12-benzoperylene pairs

We studied the annihilation kinetics for triplet excitations in isolated pairs of organic molecules and their delayed fluorescence decay using a new mathematical model for the process. According to this model, the intensity of delayed annihilation fluorescence (DAF) for isolated pairs is directly proportional to the number of pairs in which both molecules are found in the excited triplet state. We show that the decrease in such pairs and the decay of their delayed annihilation fluorescence occur according to an exponential law in the absence of random scatter in the deactivation rate constants for the triplet excitations. The results of an experimental study of the DAF decay kinetics for 1,12-benzoperylene in n-hexane at 77 K, where triplet–triplet annihilation occurs in isolated pairs, confirm the validity of the theoretical conclusions.     

Observation and characterization of the fluorescence decay of the 2s2p(6)np 1P(o) excited states of Ne

Fluorescence decay of the 2s2p(6)np (1)P(o) excited states of neon has been observed directly for the first time. This process has also been observed indirectly by threshold photoelectron spectroscopy and in electron/photon coincidences. The measurements have allowed this weak decay channel to be characterized and branching ratios derived. The fluorescence excitation spectrum is well described by a simple Rydberg model that highlights the interplay and competition between the decay channels of autoionization and fluorescence.     

QCD prediction for the non-DD[over ] annihilation decay of psi(3770)

To clarify the marked difference between BES and CLEO measurements on the non-DD[over ] decays of the psi(3770), a 1(3)D1-dominated charmonium, we calculate the annihilation decay of psi(3770) in nonrelativistic QCD. By introducing the color-octet contributions, the results are free from infrared divergences. The color-octet matrix elements are estimated by solving the evolution equations. The S-D mixing effect is found to be very small. With m_{c}=1.5+/-0.1 GeV, our result is Gamma(psi(3770)-->light hadrons)=467(+338);(-187) keV. For mc=1.4 GeV, together with the observed hadronic transitions and E1 transitions, the non-DD[over ] decay branching ratio of psi(3770) could reach about 5%. Our results do not favor the results of either the BES or the CLEO Collaborations, and further experimental tests are urged.     

有机混合薄膜中的F(o)rster能量转移

通过掺杂不同的染料有机电致发光器件可以得到不同颜色的光发射。掺杂小分子有机材料?p酸四甲酯perylene-3,4,9,10-tetracarboxylicacid(TMEP)到蓝色发光聚合物poly(N-vinyl-carbazole)聚乙烯基咔唑(PVK),得到了很好的绿光发射。TEMP掺杂质量分数为0.01时,295. 5nm激发波长的荧光光谱可以明显观察到在420 nm处PVK和530 nm处TEMP的发射峰值;当TMEP掺杂质量分数达到0.05～0.10之间,器件的电致发光光谱和荧光光谱发射峰几乎完全被TEMP的绿光所占据。光谱的转移归因于从聚合物PVK到小分子有机材料TMEP的Forster能量转移。荧光光谱中随着TMEP掺杂浓度的的增大发射峰值有明显的红移,这种现象被归因于在TMEP高浓度掺杂情况下激基缔合物的形成。激基缔合物的形成从TMEP在薄膜状态下与溶液状态下的荧光光谱的比较中得到证实。     

Study off o (995) resonance in the π0π0 decay channel

A high-statistics study of the π⁰π⁰-system produced in the π^- p→π⁰π⁰ n reaction at 38GeV/c has been carried out at the IHEP accelerator using the GAMS-2000 multiphoton spectrometer. A partial-wave analysis which includesS, D ₀, D_? andD ₊ waves has been performed in the |t|-range up to 1 (GeV/c)². TheS ^*/f ₀(980) resonance is seen as a dip in theS-wave amplitude at small |t|. A distinct peak with a mass of 997±5MeV and a width of 48±10MeV is observed in theS-wave at |t|>0.3 (GeV/c)². The production cross sections are measured.     

Picosecond time resolved fluorescence spectroscopy study of aggregation of porphyrin derivative Mn(3,4,5-OMeTPP)Cl

The picosecond time-resolved fluorescence spectrum I(, t) of the porphyrin derivative Mn(3,4,5-OMeTPP)Cl is measured. Experiments show that the fluorescence relaxation of the concentrated sample solution is composed of a fast (ps), a moderately fast (100 ps) and a slow (ns) decay process. Furthermore, the fluorescence spectra for various times after excitation have different shapes. Detailed analysis shows that the fluorescence is composed of three components with different relaxation times and spectrum shapes. The three components are attributed to monomers, dimers, and aggregates respectively.     

CTAB对四-(4-N-甲基吡啶)卟啉SERS谱的影响

研究了阳离子表面活性剂十六烷基三甲基溴化铵 (CTAB)对四 ( 4 N 甲基吡啶 )卟啉 (H2 TMPyP)及其银配合物 (AgTMPyP)在Ag胶中的表面增强拉曼散射 (SERS)谱的影响 .SERS光谱表明 ,吸附于Ag胶粒的H2 TMPyP与衬底银原子结合形成AgTMPyP ,加入CTAB后 ,部分AgTMPyP表面络合物还原为H2 TMPyP .相似的去金属化反应也出现在AgTMPyP/Ag胶 /CTAB体系中 .CTAB的加入使SERS谱带强度明显增加 .AgTMPyP的去金属化被认为是由于CTAB的存在使Ag胶颗粒表面附近微环境发生改变