Fluorescence Quenching of Anthracene by N,N-Diethylaniline in the Sodium Dodecyl Sulfate/Benzyl Alcohol/Water System

Photoinduced electron-transfer reaction of anthracene with N,N-diethylaniline (DEA) was studied in the SDS (sodium dodecyl sulfate)/BA (benzyl alcohol)/H₂O system. In an oil/water microemulsion, only the excited anthracene located at the interface can be quenched by DEA. In a water/oil microemulsion, this quenching reaction occurs in the BA continuous phase. Besides being the quencher of the excited anthracene, DEA could also change the system's structure.     

十二烷基硫酸钠/苯甲醇/水微乳液中吩噻嗪对蒽的荧光猝灭

吩噻嗪与蒽之间可以发生光诱导单电子转移反应. 用荧光光谱仪研究了十二烷基硫酸钠(SDS) / 苯甲醇(BA) / 水微乳液中吩噻嗪对蒽的荧光猝灭.结果表明，在W/O微乳液中，蒽位于苯甲醇连续相，吩噻嗪位于膜相，猝灭反应发生于膜相；而在O/W微乳液中，蒽既可位于油核中，也可位于膜相，吩噻嗪位于膜相，猝灭反应亦发生于膜相.     

Fluorescence Quenching of Anthracene by N,N-Diethylaniline and Phenothiazine in CTAB/n-C5H11OH/H2O Microemulsion

Photoinduced electron transfer reactions of anthracene with N,N-diethylaniline (DEA) and phenothiazine (PTZ) occurred in the membrane phase of the CTAB (hexadecyltrimethylammonium bromide)/n-C₅H₁₁OH (1-pentanol)/H₂O micro-emulsion. DEA and PTZ exist in the membrane phase of the microemulsion because the presence of vitamin-C (Vc) can change the quenching constant. The change of the quenching constant for the DEA–anthracene system with the presence of Vc is more obvious than that for the PTZ–anthracene system. Thus, the DEA molecules are much closer to the polar head of the microemulsion than PTZ. Compared with DEA, the distribution of PTZ in the microemulsion tends to follow Poisson statistics.     

Spectroscopy characterization of anthracene in SDS/BA/H2O system

Spectroscopy characterization of anthracene in sodium dodecyl sulfate (SDS)/benzyl alcohol (BA)/water (H(2)O) microemulsion was studied by UV-visible absorption and fluorescence emission spectroscopy. The impact of the composition and structure of the microemulsion on spectroscopy characterization of anthracene were discussed. At the same time, we indicated the location of anthracene in microemulsion. The results indicated that in O/W microemulsion in SDS/BA/H(2)O system, anthracene exists both in the membrane phase and oil core, while in W/O microemulsion, anthracene exists in the oil continuous phase.     

Fluorescence Quenching of Anthracene by N,N-Diethylaniline and Phenothiazine in Triton X-100/n-C10H21OH/H2O Microemulsion

IntroductionDuring the last decade,microemulsions haveplayed important roles in the development of bio-logical,material,environmental and other relatedfields[1— 4] .Although photo- induced electron trans-fer processes are of considerable interest in biologyand chemistry,up to now,most of the studies ofthe photo- induced electron transfer in micelle andinverse micelle have been limited to one- or two-component water/surfactant systems[5] .As theirextensions to microemulsion,only a very limited…     

吩噻嗪在十二烷基硫酸钠/苯甲醇/水微乳液中的定位

采用循环伏安法和荧光猝灭法研究了吩噻嗪（PTZ）在十二烷基硫酸钠（SDS）/苯甲醇（BA ）/ 水（H2O）微乳液中的定位.结果表明,吩噻嗪在十二烷基硫酸钠/苯甲醇/水体系微乳液中位于微乳液膜相中靠近表面活性剂极性头基的一侧,PTZ分子中的S原子和N原子均可朝向表面活性剂的极性头基.     

Ground and excited state isomeric forms of the anthracene-diethylaniline molecular exciplex

The potential energy surfaces for the molecular complex formed between anthracene (the electron acceptor) andN ,N-diethylaniline (DEA) (the electron donor) were computed as the quasi-adiabatic states resulting from the configuration interaction between the ground (AD), locally excited (A^*D) and charge-transfer (A⁻D⁺) excited electronic configurations. The results clearly indicate the existence of three geometrically and energetically different isomeric forms of the complex in the ground state. In the excited state, the potential energy surfaces reveal the existence of five well-defined equilibrium configurations separated by energy barriers and characterized by different admixtures of the (A^*D) and (A⁻D⁺) electronic configurations. Such a variety of equilibrium configurations in the ground and excited states is, in part, accounted for by the existence of two different conformational forms of DEA that can form complexes with anthracene, and are characterized by different balances between steric effects and interactions of electronic charge distributions in the complex components. The energies of transitions between the relevant ground and excited state equilibrium configurations were calculated and compared with spectroscopic data of a jet-cooled complex obtained in supersonic beam experiments. These transitions were successfully assigned to the observed resonance-like and exciplex-like spectra, and this enabled interpretation of observed changes in the fluorescence excitation and fluorescence spectra of the complex upon excess excitation energy.     

New Anthracene Derivatives as Triplet Acceptors for Efficient Green‐to‐Blue Low‐Power Upconversion

Three new anthracene derivatives [2‐chloro‐9,10‐dip‐tolylanthracene (DTACl), 9,10‐dip‐tolylanthracene‐2‐carbonitrile (DTACN), and 9,10‐di(naphthalen‐1‐yl)anthracene‐2‐carbonitrile (DNACN)] were synthesized as triplet acceptors for low‐power upconversion. Their linear absorption, single‐photon‐excited fluorescence, and upconversion fluorescence properties were studied. The acceptors exhibit high fluorescence yields in DMF. Selective excitation of the sensitizer Pd^IIoctaethylporphyrin (PdOEP) in solution containing DTACl, DTACN, or DNA‐CN at 532 nm with an ultralow excitation power density of 0.5 W cm^?2 results in anti‐Stokes blue emission. The maximum upconversion quantum yield (Φ_UC=17.4 %) was obtained for the couple PdOEP/DTACl. In addition, the efficiency of the triplet–triplet energy transfer process was quantitatively studied by quenching experiments. Experimental results revealed that a highly effective acceptor for upconversion should combine high fluorescence quantum yields with efficient quenching of the sensitizer triplet.     

蒽在SDS/BA/H2O体系中的光谱特征

用紫外-可见吸收光谱和荧光发射光谱研究了蒽在不同组成和结构的十二烷基硫酸钠(SDS)/苯甲醇(BA)/H20微乳液中的光谱特征,探讨了微乳液组成和结构对蒽光谱特征的影响,阐述了蒽在微乳液中的定位。结果表明,蒽位于O/W微乳液的膜相和油核;在SDS/BA/H2O W/O微乳液中,蒽定位于油连续相。     

Influence of the solvent on the quenching of the fluorescence of anthracene by aromatic amines

The influence of the solvent on the quenching of the fluorescence of anthracene by diethylaniline (DEA) and aniline has been investigated. Fluorescence quenching in these systems obeys the equation of Stern and Volmer. A transition from kinetics-controlled to diffusion-controlled processes takes place with the increase in viscosity () in nonpolar solvents. In polar solvents the quenching rate is limited by diffusion over the whole viscosity range investigated. These peculiar effects of the solvent can be explained by the traditional three-stage quenching scheme of the singlet-excited anthracene by electron donors. It is also possible that the increase in the quenching constant () in polar as compared to nonpolar solvents with the same is related to an increase in the rate constant of non-emitting deactivation in polar media, induced by the quenching agent. In the case of the quenching of fluorescence of anthracene by aniline the process is diffusion-controlled, regardless of the nature of the solvent.Translated from Teoreticheskaya i Éksperimental'naya Khimiya, Vol. 21, No. 3, pp. 370–374, May–June, 1985.     

DEA与SDS/n-C5H11OH/H2O微乳液的相互作用

以循环伏安法研究了N,N-二乙基苯胺（DEA）与十二烷基硫酸钠（SDS）/正戊醇（n-C5H11OH）/H2O体系O/W和W/O结构微乳液的相互作用.结果表明,DEA在SDS/n-C5H11OH/H2O体系微乳液中有两种定位方式:其一,DEA分子在微乳液液滴膜相中定位于表面活性剂和助表面活性剂的极性基团附近;其二,DEA分子在微乳液液滴膜相中定位于表面活性剂疏水基团一侧.两种定位的分布与微乳液的结构和组成相关.     

An anthracene-appended beta-cyclodextrin-based dyad: study of self-assembly and photoinduced electron-transfer processes

The self-assembly of a beta-cyclodextrin (beta-CD)-based supramolecular dyad is reported, in which the donor anthracene moiety is covalently linked to the smaller rim of the beta-CD and the acceptor pyromellitic diimide (PMDI) is encapsulated within the beta-CD cavity. Encapsulation of the PMDI into the beta-CD cavity was studied by a variety of techniques, which suggested that PMDI is encapsulated so as to position the aromatic part at the centre of the cavity with the 2-propyl end at the narrower rim among the overhanging primary OH groups and the N-ethylpyridinium end situated at the wider rim exposed to water. Photoinduced electron transfer (PET) in the system was studied by fluorescence quenching and laser flash photolysis techniques. At [PMDI]<10(-4) M, the equilibrium is in favour of the free molecules, and under these conditions fluorescence quenching is negligible and diffusion-mediated electron transfer involving the triplet excited state of anthracene predominates. At higher concentrations of PMDI, the equilibrium is largely in favour of the supramolecular dyad and intra-ensemble PET processes predominate. The experimentally determined electron-transfer rate constant agrees very well with that calculated by using the Marcus equation. It was observed that a fraction of the ion pairs survived for more than 200 micros.     

Preparation and spectral characteristics of anthracene/tetracene mixed crystals

A series of tetracene-doped anthracene crystals with different doping concentrations (the highest molar ratio 100 1) are grown from solution. Crystal structures and optical characteristics of the above mixed crystals are investigated at room temperature. By changing the doping concentrations, the fluorescence can be adjusted from blue-green to green and even to yellow-green. The emission spectra of anthracene/tetracene (An/Te) mixed crystals reveal the sensitized fluorescence of tetracene and the partial quenching of anthracene emission. The data of transient photoluminescence (PL) decays illustrate that in An/Te mixed crystals, the decay of anthracene becomes faster, while the PL lifetime of tetracene is longer than that of the tetracene single crystals. All above experimental results suggest that there is excitation energy transfer from anthracene to tetracene in the mixed crystals. Supported by the National Natural Science Foundation of China (Grant No. 5057 3039) and the National Key Basic Research and Development Program of China (Grant No. 2006CB806200)     

CdTe量子点与蛋白质相互作用的荧光猝灭效应

本文在水热法合成水溶性CdTe及核壳结构CdTe/CdS量子点的基础上,分别研究了细胞色素c对CdTe量子点及CdTe/CdS核壳量子点荧光的猝灭效应和CdTe量子点对牛血清白蛋白荧光的猝灭效应,并阐述了猝灭机理。结果显示,细胞色素c对CdTe量子点的荧光猝灭效应具有一定的粒径依赖性,粒径越小,猝灭效应越强;细胞色素c对CdTe/CdS核壳量子点的猝灭效应比对CdTe量子点的更强,揭示了受激电子的表面传递机理。CdTe量子点通过松散牛血清白蛋白的螺旋结构而猝灭其荧光。     

竞争吸收在含金属稳定剂的猝灭机理中的作用

<正> 含重金属原子的光稳定剂的稳定效果常和其光猝灭能力相联系。钱钦文等指出,Ni、Cr、Yb及Eu的整合物能猝灭二乙酮的三重态。Briggs等发现,镍的一系列不同配位体的螯合物可以强烈的猝灭蒽的三重态。有些报告还指出,许多不同配位体的金属螯合物是二苯酮激发态的最佳猝灭剂。但也存在一些相反的结果,如Carlsson等未观     

Anthracene as a sensitiser for near-infrared luminescence in complexes of Nd(III), Er(III) and Yb(III): an unexpected sensitisation mechanism based on electron transfer

The ligand L(1), which contains a chelating 2-(2-pyridyl)benzimidazole (PB) unit with a pendant anthacenyl group An connected via a methylene spacer, (L(1) = PB-An), was used to prepare the 8-coordinate lanthanide(III) complexes [Ln(hfac)(3)(L(1))] (Ln = Nd, Gd, Er, Yb) which have been structurally characterised and all have a square antiprismatic N(2)O(6) coordination geometry. Whereas free L(1) displays typical anthracene-based fluorescence, this fluorescence is completely quenched in its complexes. The An group in L(1) acts as an antenna unit: in the complexes [Ln(hfac)(3)(L(1))] (Ln = Nd, Er, Yb) selective excitation of the anthracene results in sensitised near-infrared luminescence from the lanthanide centres with concomitant quenching of An fluorescence. Surprisingly, the anthracene fluorescence is also quenched even in the Gd(III) complex and in its Zn(II) adduct in which quenching via energy transfer to the metal centre is not possible. It is proposed that the quenching of anthracene fluorescence in coordinated L(1) arises due to intra-ligand photoinduced electron-transfer from the excited anthracene chromophore (1)An* to the coordinated PB unit generating a short-lived charge-separated state [An(.+)-PB(.-)] which collapses by back electron-transfer to give (3)An*. This electron-transfer step is only possible upon coordination of L(1) to the metal centre, which strongly increases the electron acceptor capability of the PB unit, such that (1)An* --> PB PET is endoergonic in free L(1) but exergonic in its complexes. Thus, rather than a conventional set of steps ((1)An* -->(3)An* --> Ln), the sensitization mechanism now includes (1)An* --> PB photoinduced electron transfer to generate charge-separated [An(.+)-PB(.-)], then back electron-transfer to generate (3)An* which finally sensitises the Ln(III) centre via energy transfer. The presence of (3)An* in L(1) and its complexes is confirmed by nanosecond transient absorption studies, which have also shown that the (3)An* lifetime in the Nd(III) complex matches the rise time of Nd-centred near-infrared emission, confirming that the final step of the sequence is (3)An* --> Ln(III) energy-transfer.     

Photochemical processes in doped argon-neon core-shell clusters: the effect of cage size on the dissociation of molecular oxygen

The caging effect of the host environment on photochemical reactions of molecular oxygen is investigated using monochromatic synchrotron radiation and spectrally resolved fluorescence. Oxygen doped clusters are formed by coexpansion of argon and oxygen, by pickup of molecular oxygen or by multiple pickup of argon and oxygen by neon clusters. Sequential pickup provides radially ordered core-shell structures in which a central oxygen molecule is surrounded by argon layers of variable thickness inside large neon clusters. Pure argon and core-shell argon-neon clusters excited with approximately 12 eV monochromatic synchrotron radiation show strong fluorescence in the vacuum ultraviolet (vuv) spectral range. When the clusters are doped with O2, fluorescence in the visible (vis) spectral range is observed and the vuv radiation is found to be quenched. Energy-resolved vis fluorescence spectra show the 2 1Sigma+-->1 1Sigma+(ArO(1S)-->ArO(1D)) transition from argon oxide as well as the vibrational progression A '3Delta u(nu'=0)-->X 3Sigmag*(nu") of O2 indicating that molecular oxygen dissociates and occasionally recombines depending on the experimental conditions. Both the emission from ArO and O2 as well the vuv quenching by oxygen are found to depend on the excitation energy, providing evidence that the energy transfer from the photoexcited cluster to the embedded oxygen proceeds via the O2+ ground state. The O2+ decays via dissociative recombination and either reacts with Ar resulting in electronically excited ArO or it recombines to O2 within the Ar cage. Variation of the Ar layer thickness in O2-Ar-Ne core-shell clusters shows that a stable cage is formed by two solvation layers.     

Mechanistic Insights into the Fluorescence Quenching of Rhodamine 6G by Graphene Oxide

The fluorescence quenching of Rhodamine 6G (R6G) by graphene oxide (GO) was interrogated by R6G fluorescence measurements using a set of controlled GO samples with varied C/O ratios as the quencher.The carbonyl groups on the GO nanosheet turned to play a dominant role in quenching the R6G fluorescence.The quenching in the static regime can be described by the "sphere of action" model.The significant absorption of the R6G fluorescence by the ground-state complex formed between R6G and GO was identified to be responsible for the static quenching.This work offers helpful insights into the fluorescence quenching mechanisms in the R6G/GO system.     

核酸前体及其修饰结构的电子转移机理研究

应用荧光淬灭和激光光解瞬态吸收光谱技术研究了一系列核酸前体(核酸碱基、核苷及其结构修饰物)、小牛胸腺ctDNA与各种荧光探针及蛋白酶之间的瞬态、稳态电子转移作用机理。测定结果表明,它们的稳态、静态荧光淬灭作用很强,很好地符合Stern-Volmer线性方程,淬灭速率常数,k~q(s)和k~q(d),达10^10.M^-^1S^-^1,属于扩散控制,表明核酸前体的基态可作为电子受体或给体而分别与含色氨酸残基的蛋白酶、受电子型荧光探针之间发生具有电子转移性质的相互作用。对鸟嘌呤的结构修饰物进行了激光光解的瞬态吸收光谱研究,检测了几类活性中间体,论证了激发态的光致电子转移和能量转移机理。     

Singlet exciton migration in a random organic two-component system containing physical and chemical traps

Steady-state as well as time-dependent fluorescence studies have been carried out near 80 K on glassy mixed layers of anthracene and phenanthrene doped with tetracene and containing incipient anthracene dimers as physical traps. The efficiency of energy transfer from initially excited anthracene (“donor”) sites to tetracene (“supertrap”) has been measured as a function of donor concentration c_D. The results are interpreted in terms of a superposition of two transfer pathways: (i) Random walk of excitons across the donor ensemble to either tetracene or anthracene dimers and (ii) single step Förster transfer from the excited dimers (excimers) to tetracene. The efficiency of process (i) is in quantitative accord with the predictions of the 3D version of the Loring, Anderson and Fayer theory assuming dipole-dipole coupling.