Kinetics of long-lived luminescence of eosin in Langmuir-Blodgett films

The spectral and kinetic properties of photoluminescence of mixed Langmuir-Blodgett (LB) films of eosin decyl ether and palmitic acid on a solid substrate are studied. The electronic absorption and fluorescence spectra of the films are identical to the spectra of the dye in ethanol. An increase in the dye concentration in a monolayer results in the appearance of a dimer absorption band, quenching of fluorescence of monomers, and the red shift of the spectral bands. At 90 K, the distinct phosphorescence and delayed fluorescence bands of LB films were observed. The decay kinetics of phosphorescence and delayed fluorescence is nonexponential. It is shown that the decay curve of delayed fluorescence is determined by triplet-triplet annihilation (TTA) and T ₁→S₁ triplet-singlet intersystem crossing (IS). The initial nonexponential phosphorescence decay is caused the dominant contribution of TTA to the decay of triplet molecules. The experimental data are interpreted based on the mechanisms of exchange-resonance and inductive-resonance annihilation.     

Delayed observation of laser-induced fluorescence for imaging of tumors

We report on a technique to improve fluorescence images of superficially growing tumors marked with photosensitizers. Exploiting the longer fluorescence decay times of porphyrin-based photosensitizers compared to average decay times of tissue autofluorescence, delayed detection of laser-induced fluorescence allows to suppress the autofluorescence background. The feasibility of delayed fluorescence imaging of tumors has been demonstrated in-vitro. It follows from an analysis of delayed fluorescence spectra that autofluorescence background falling into the photosensitizer fluorescence band can be reduced by up to one order of magnitude.     

Fluorescence and Time-Resolved Delayed Luminescence of Porphyrins in Organic Solvents and Polymer Matrices

Porphyrin dyes fulfill an essential function in photosynthesis and are important in photodynamic therapy and in a range of electronic devices. Their spectroscopic characteristics may play a crucial role in these processes. The spectral properties of two porphyrin dyes: tetraphenylporphyrin and tetraphenysulfporphyrin in organic solvents (acetone, chloroform, methyl alcohol, and dimethyl-sulfoxide) and in polyvinyl alcohol and poly(methylmethacrylate) films have been investigated. Absorption, fluorescence, and microsecond time-resolved delayed luminescence spectra have been measured at room temperature. The existence of different aggregated dye forms in the ground and excited states has been demonstrated. The manifold of dye species depends on the solvent/polymer. In the case of the polymers, it also depends on the solvent used to coat the polymer film. Delayed luminescence spectra and decay times of the two porphyrins in the different solutions and in polymeric matrices suggest that different mechanisms of deexcitation of the singlet excited states may be responsible for their generation in these and other porphyrin dyes.     

Spectral Properties of Y-Shaped Donor-Acceptor Push-Pull Imidazole-based Fluorophores: Comparison between Solution and Polymer Matrices

The spectral properties of a novel type of Y-shaped fluorophores consisting of an imidazole ring end-capped with two electron-donating N,N-dimethylaminophenyl groups at positions C4 and C5 and one electron-withdrawing cyano group on the imidazole moiety at position C2 were examined. The π-linker separating the 4,5-bis[4-(N,N-dimethylamino)phenyl]-1H-imidazole donor moiety and the cyano group comprises 1,4-phenylene (1), (E)-phenylethenyl (2), (E)-phenylbuta-1,3-dienyl (3), biphenyl (4), (E)-phenylethenylphenyl (5) and phenylethynylphenyl (6) conjugated paths. The absorption and fluorescence spectra were obtained in toluene, dichloromethane, acetonitrile and methanol and in polymer matrices such as polystyrene (PS), poly(methyl methacrylate) (PMMA) and poly(vinylchloride) (PVC). The most intense absorption bands of fluorophores 1-6 were observed within the range of 283 to 330?nm. Less intense but longer-wavelength absorption bands designated as charge-transfer bands were observed at approximately 380-430?nm depending on the medium. The fluorophores exhibited strong fluorescence in the visible region with a Stokes shift of approximately 4300-5800?cm(-1) in non-polar toluene and polystyrene, whereas very low intensity of fluorescence was observed with a Stokes shift in the 6500-7800?cm(-1) region in polar methanol and acetonitrile. The large Stokes shift indicates a large difference in the spatial arrangement of the chromophore in the absorbing and emitting states. A relatively intense fluorescence (quantum yields of 0.12-0.69) was observed only for derivative 1 in all media except methanol. The fluorophores doped in matrices yielded more intense fluorescence compared with the fluorescence in liquid media. The use of solid polymer matrices lowers the probability of forming non-emissive excited states. The fluorescence lifetimes were short (1-4?ns) for all of the fluorophores in solvents and in polymer matrices.     

一种锌希夫碱配合物的表征及发光性能研究

合成并通过真空升华提纯得到了一种高纯度的希夫碱有机金属配合物水杨醛缩邻苯二胺合锌。通过元素分析、红外光谱、热重-差热曲线、紫外-可见光吸收光谱、荧光发射光谱和光致发光光谱表征了其结构、热稳定性以及能带结构。实验结果表明：水杨醛缩邻苯二胺合锌的玻璃化温度(T_g)高达183 ℃,分解温度为449 ℃; 水杨醛缩邻苯二胺合锌是一种多晶粉末状的发光材料,在紫外光的激发下,在四氢呋喃溶液体系中的荧光发射峰在508 nm处,为蓝绿色荧光,色纯度高,荧光量子效率高,禁带宽度2.62 eV; 利用真空热蒸镀很容易制备高质量薄膜,其发射峰在562 nm处,半高宽为48.5 nm的黄绿光发射。利用水杨醛缩邻苯二胺合锌为发光层制备了黄光有机电致发光器件。     

Dynamics of long-wavelength fluctuations in a fluid layer heated from above

We report an experimental study of the dynamics of thermal fluctuations in a 4.86 mm thick layer of CS2 heated from above. Stabilizing gradients ranged from 10.3 to 61.7 K/cm. Power spectral measurements were made over the wave vector range 9 cm(-1)相似文献   

Collision-induced vibrational energy transfer: K2[1(1) sigmau+ (nu'=2)]+He, H2-->K2[1(1) sigmau+(nu'=1,3)]+He, H2

Collisional energy transfer processes K2[1(1) sigmau+ (nu'=2)]+He, H2-->K2[1(1) sigmau+(nu'=1,3)]+He, H2 were studied by laser induced fluorescence under gas cell conditions. During the experiments, the cell temperature was kept constant at 420K. The buffer gas pressure was varied over the range from 40 to 250 Pa, Kz molecules were irradiated with pulses of radiation from an OPO laser, populating K2[1(1) sigmau+ (nu'=2)] by photon absorption. The resulting fluorescence included the direct component emitted in the decay of the optically excited state and the sensitized components arising from collisionally populated states. The decay signal of time-resolved fluorescence from 1(1) sigmau+ (nu'=2)]-->1(1) sigmag+(nu"=0) transition was monitored. In the early period after excitation, only very little population in states v'= 1 or 3 had yet accumulated, the rate of collisional activation to the state nu'=2 was negligible. The decay curve of the nu' = 2-->nu" = 0 was treated as a single exponential function. From the measurement of the time-resolved fluorescence, the semilog plot was shown. The slope yielded the effective lifetime of the nu' = 2--> nu' = 0 transition. Based on the Stern-Volmer equation, the radiative lifetime (36 +/- 7) ns was obtained. The total cross sections for deactivation of 1(1) sigmau1 (nu'=2) state by means of collisions with He and H2 are (3.0 +/- 0.5) x 10(-16) cm2 and (6.4 +/- 1.2) x 10(-15) cm2, respectively. The radiative lifetimes of 1(1) sigmau+(nu' = 1,3) states can also be determined through time-resolved fluorescence in pure K vapor. The time-integrated intensities of 1(1)sigmau+(nu' = 1,2,3)-->1(1) sigmag+(nu"=0) transition at different He or Hz pressure were measured. The ratio of fluorescence intensities versus 1/P(He, H2) can be fitted by a straight line. The slopes yield the cross sections sigma(nu'=2-->nu'=1) = (1.4 +/- 0.5) x 10(-16) cm2 and (3.2 +/- 1.0) x 10(-15) cm2; sigma(nu'=2-->nu'=3)= (1.2 +/- 0.4) x 10(-16) cm2 and (2.6 +/- 0.9) x 10(-15) cm2 for He and H2, respectively. Cross sections for the effective quenching of the nu' = 1,2,3 states were also determined. To our knowledge, the cross-sections for these processes are reported for first time.     

Effect of Temperature on the Rate of Triplet–Triplet Annihilation of 1,2-Benzanthracene in a Polymer Matrix

The process of triplet–triplet annihilation (TTA) of 1,2-benzanthracene (1,2-BA) incorporated into polymer films of polyvinyl butyral has been investigated in the temperature interval 80–360 K. An analysis of the kinetics of the decay of delayed annihilation fluorescence (DAF) of 1,2-BA has shown that the process of the triplet excitation energy transfer in a disperse medium of the polymer at distant times of the DAF decay can be described using the approximation of random walks of the triplet energy in the inhomogeneous medium of the polymer. At low temperatures, at the initial times of DAF decay the TTA process is described with the aid of a model of static annihilation.     

基于电荷转移过程的PAN-C60共聚物薄膜的时间分辨荧光研究

利用吸收光谱和皮秒时间分辨荧光研究PAN－C60星状共聚物的电荷转移过程。PAN－C60共聚物的吸收和荧光光谱结果显示共聚物中存在着电荷转移过程。时间分辨荧光结果表明PAN的荧光衰减遵循双指数衰减规律（一快过程160ps和一慢过程1500ps)，快衰减过程主要来源于聚合物中主链间相互作用产生的空间间接极化子对的影响，慢变过程主要来源于单重态激子的辐射跃迁弛豫。在共聚物中，C60分子的存在除导致PAN激发态寿命缩短外，还影响聚合物链间的相互作用，C60分子对PAN荧光猝 灭作用主要通过慢变过程影响的，而对PAN的空间极化子对的影响主要与其快衰减过程有关。     

Preparation and Spectral Characterization of Fluorescence Probes Based on 4-N,N-Dimethylamino Benzoic Acid and Sterically Hindered Amines

The adducts of simple chromophore 4-N,N-dimethylamino benzoic acid with 2,2,6,6-tetrametyl-4-hydroxy- or 4-amino-piperidine were examined as fluorescence probes (spin double sensors) to monitor radical processes. The links in the adducts were either an ester or amide group, and the sterically hindered amines were in the form of -NH, -NO? and -NOR. The spectral properties of the three related derivatives (esters or amides) were quite similar. The maxima of the absorption spectra were in the range of 295-315?nm, and the maximum of fluorescence was located in the range of 330-360?nm, depending on the polarity of the solvent. In polar solvents, a red-shifted fluorescence band at 460-475?nm was observed. The fluorescence of these derivatives was rather weak as compared to anthracene under the same conditions. The Stokes shift was large, as high as 6,000?cm(-1), indicating the formation of a twisted intra-molecular charge transfer (TICT) state. No large differences in Stokes shifts were observed in polymer matrices of poly(methyl methacrylate), polystyrene and poly(vinyl chloride). The extent of intramolecular quenching was expressed as Φ(NX)/Φ(NO) (X?=?H, NOR) and was in the range of 1-3 in solution and as high as 8 in polymer matrices. The low efficiency of intramolecular quenching limits the application of these new adducts as fluorescence probes for the monitoring of radical processes in solution but favors their application in polymer matrices.     

钠分子B^1∏u与2^1∑g^＋间的碰撞激发转移

The B 1pi(u) electronic state of Na2 was excited by the 441.6 nm He-Cd laser line. The Na atomic transitions and the A 1sigma(u)+ --> X 1sigma(g)+ band of Na2 were recorded. From the intensities and spectra of the Na and Na2 fluorescence several collisional processes in the excited sodium atom-dimer system were identified. The Na atomic lines are the result of collisional energy transfer from Na2 (B 1pi(u)) to Na(3P). Predissociation process may also contribute to atomic fluorescence. The A 1sigma(u)+ --> X 1sigma(g)+ band is interpreted through a populating mechanism involving collisional transfer from B 1pi(u) to 2 1sigma(g)+ followed by a radiative transfer to the A 1sigma(u)+ state. From the decay constants and fluorescence intensities, the rate coefficient at 360 degrees C for collisional energy transfer from Na2 (B 1pi(u)) to Na2 (2 1sigma(g)+) was found to be 5.7 x 10(-10) cm3 x s(-1). The predissociation rate of the B 1pi(u) is 2.7 x 10(6) s(-1).     

NO分子双光子诱导荧光的自吸收现象

以皮秒Nd:YAG激光器抽运的光学参量发生/放大器为激发光源,获得了在452.4 nm波长激光激发下,NO分子的双光子激光诱导色散荧光光谱(LIDFS)。并由此得到了NO分子基电子态的振动基频和振动非谐性系数分别为ω″_e=(1 904.7±7.3) cm-1, ω″_eχ″_e=(14.2±1.2) cm-1, ω″ey″_e=-(0.021 8±0.009 1) cm-1。在NO分子双光子LIDFS实验研究中,首次观测到了NO分子强烈的自吸收现象,在较高样品气压条件下,色散荧光光谱图中对应A 2Σ(v′＝0)→X 2Π(v″＝0)跃迁的谱线消失。实验结果表明,自吸收现象导致的该跃迁谱线强度的变化,随样品气压、激光场和样品作用区到荧光接收窗口距离的减小而减小。     

Analysis of branched oligophenylene by absorption and fluorescence spectra

A branched oligophenylene has been synthesized based on 1,3,5-tri(4′-bromophenyl)benzene. Absorption and fluorescence spectra were studied and fluorescence quantum yields and lifetimes were measured for the compound in solution. It is demonstrated that the absorption spectrum is a superposition of p-quaterphenyl, p-terphenyl, and biphenyl chromophore absorption bands in a 1:2:1 ratio. The oligomer fluorescence spectrum is found to depend on the excitation wavelength. It is shown that the oligomer fluorescence is determined by two fluorochromic groups, namely fragments with branched p-terphenyl and p-quaterphenyl units. The main fluorescence maxima for these fluorochromic groups coincide with each other and lie in the vicinity of λ = 360 nm. A very weak fluorescence band found in the region 380–440 nm is excited by light with a wavelength lying beyond the oligomer self-absorption region. The reasons for a decrease in fluorescence quantum yields of branched models and the studied oligophenylene as compared with those of linear p-polyphenylene chromophores are discussed.     

Influence of OH groups on 1.5-μm emission of Yb3+/Er3+ co-doped tungsten-tellurite glasses

The Yb3+/Er3+ co-doped TeO2-WO3-ZnO glasses bubbling with different times were prepared. The infrared (IR) transmission spectra, emission spectra and fluorescence lifetime of Er3+ at 1.5μm were measured. The quench effects of OH groups on emission intensity of Er3+ at 1.5μm as well as the relationships between fluorescence decay rate and OH group content were investigated. The constant kOH-Er, which represents the strength of the interactions between Er3+ ions and OH groups, is approximately 17.0 × 10-20cm4/s, and is comparable to that for Er3+ in Yb3+/Er3+ co-doped phosphate glasses.     

DMANS——一种新型荧光闪烁体染料的寿命与能量转移的研究

本工作对一种新型荧光闪烁体染料——4-二甲胺基—4''硝基芪(DMANS)在不同介质中的光谱行为和能量转移进行了研究,发现介质的极性大小以及介质和染料间的能量转移对该闪烁体染料的荧光量子产率和闪烁发光延迟具有重大影响。研究对选择基体材料和合理组成闪烁材料配方有一定的参考价值。     

芪盐LB多层膜的三维荧光谱分析

采用稳态、时间分辨荧光和三维荧光光谱技术研究了芪盐有机分子在溶液和芪盐/花生酸交替LB多层膜中的激发态的动力学特性.研究表明,芪盐分子在LB膜中形成H-聚集体,使得其荧光光谱发生蓝移.由于偶极间的相互作用使得聚集体的能级发生分裂,荧光衰减曲线可用双指数函数进行拟合.三维荧光谱发现随着衰减时间的推移,荧光峰逐渐向长波方向移动,不同波段具有不同的衰减驰豫时间.     

2(水杨醛缩苯胺)-(1,10-邻菲罗啉)合钙的光谱特性

合成了一种新型的蓝光发射材料2(水杨醛缩苯胺)-(1,10-邻菲罗啉)合钙,并利用红外光谱、X射线衍射谱、DSC热分析、UV-vis吸收谱、荧光激发光谱和荧光发射光谱研究了其结构、晶态、热稳定性以及光学特性,分析了它的能态结构和发光机理。结果表明,2(水杨醛缩苯胺)-(1,10-邻菲罗啉)合钙的热稳定性较高,是一种多晶粉末发光材料,禁带宽度2.93eV,在紫外光的激发下,固态荧光发射峰在449.7nm处,在乙醇溶液体系中的荧光发射峰在491nm处,均为蓝色荧光,色纯度高,荧光量子效率高,其荧光发射主要来源于长波吸收带,最大波长吸收带对荧光发射贡献最大。     

Transient color centers in GGG crystals

Electron pulse induced absorption and their decay kinetics have been investigated in samples of GGG crystals with different starting absorption spectra. It is shown that for all samples there appears a wide transient absorption (TA) band with two maxima in the region 14,000-17,000 v cm m 1 and 22,000-26,000 v cm m 1 . TA decay kinetics measurements in 14,000 v cm m 1 and 22,000 v cm m 1 are two-exponential (with half-time order several tens and several hundreds ns). Analyzing the obtained results, we can suppose that low and high energy TA bands are connected with the F + (or O m ) and F transient color centers (TCC) respectively.     

NO2分子在550～740 nm范围内的激光诱导荧光光谱

以皮秒Nd：YAG激光器的二倍频输出(532nm)作为激发源,在室温下,对NO2分子在低气压和较高气压情况下进行了激光诱导荧光研究。在低气压条件下获得了在550～740nm范围内的振动序列,将其归属为由第一电子激发态A^2B2态向基电子态X^2A1态不同振动态的跃迁,由此得到对称振动模式和弯曲振动模式的谐振频率,分别为ω1=1300．72cm^-1和ω2=744．14cm^-1.并在此基础上对较高气压下荧光光谱产生的明显红移现象进行了解释,得到了有意义的结果。     

Proposal for Fourier-Transform Phase-Modulation Fluorometer

I propose a concept of a novel Fourier-transform phase-modulation fluorometer by which a fluorescence decay waveform can be obtained. In the fluorometer, the modulation frequency of the excitation light source is swept continuously from a start frequency f_min to an end frequency f_max with a time duration T. The resultant fluorescence signal waveform is Fourier-transformed to obtain amplitude and phase spectra. The ratio of the amplitude spectrum and the difference of the phase spectrum over those of the reference spectra that are obtained from a non-fluorescent material are calculated, respectively, and the pair of both spectral data is inverse-Fourier-transformed again to obtain the fluorescence decay waveform. To verify and demonstrate the effectiveness of the concept, I carried out (1) numerical simulations, (2) determination of a time constant of a passive resistor-capacitor (RC) differential circuit, and (3) measurement of a fluorescent decay waveform of YAG materials packed in Nichia’s white LED.