铝试剂的荧光光谱与荧光量子产率

首次研究了铝试剂的荧光光谱和荧光量子产率,发现pH3至pH12条件下,用紫外光照射铝试剂溶液可以产生荧光,最大激发波长和最大发射波长分别为297nm和409nm,荧光强度与铝试剂浓度之间存在良好的线性关系,线性范围为0.01～3μg/mL,检测下限为0.01μg/mL,以硫酸奎宁为参比,测得铝试剂的荧光量子产率为0.16。     

Fluorescence quantum yield of the two novel macrocyclic lactams

Fluorescence quantum yield of two novel compounds—dibenzo[c,k]-1,2-dithia-6,9-diazacyclododecane-5,10-dione (1) and dibenzo[c,k]-1,2-dithia-6,9-diaza-7-methylcyclododecane-5,10-dione (2) was studied by Williams method using anthracene as a reference.     

Fluorescence lifetime and quantum yield of diphenylketyl radical at low temperature

The fluorescence lifetimes of the diphenylketyl radical trapped in ethanol and EPA matrices are 16.8 ± 0.5 and 21.1 ± 0.6 ns, respectively in the temperature region of 77–130 K. The fluorescence quantum yield in ethanol matrix is 0.16 ± 0.6. These values are consistent with the radiative lifetime calculated from the absorption spectrum.     

Synthesis and surface photochemistry of graphitized carbon quantum dots

Graphitized carbon quantum dots (CQDs) were synthesized by a simple hydrothermal process with cetyltrimethylammonium bromide (CTAB) as the starting material and nitric acid as surface oxidant. The photoluminescent quantum yield (QY) of CQDs could be greatly enhanced through surface esterification with glycol. Based on the structure characterization, we proposed that the CQDs consisted of the stack of graphene sheets sized several nanometers and their excitation-dependent photoluminescence (PL) should be attributed to the n→π* transition of CO bond of surface carboxylic groups. And the PL of CQDs was obviously enhanced by the esterification of carboxylic groups, possibly due to the increase of the molecular coplanarity or the rigidity.     

Layer-by-layer quantum dot constructs using self-assembly methods

We describe the creation of CdSe/ZnS quantum dot assemblies using layer-by-layer construction strategies, using self-assembly. In the first approach, a dithiol linker was used to make multilayers of CdSe/ZnS quantum dots, while in the second biotin- and streptavidin-conjugated CdSe/ZnS quantum dots were used to make multilayer constructs. Both the chemical bonding nature and fluorescence spectroscopic properties of quantum dot films were characterized using X-ray photoelectron spectroscopy (XPS) and fluorescence spectroscopy.     

Competition between vibrational relaxation and photochemistry: relevance of vibronic quantum effects

Two molecules showing photochemistry but no fluorescence have been investigated at 80 K in a rigid matrix regarding the behavior of the quantum yield for bond fragmentation as a function of the vibrational/vibronic level and electronic excited state. A new equation was developed to determine the photochemical quantum yield under ambient conditions (80 K). The levels/bands involved were those within a given vibrational progression, in different progressions as well as in combination. The yield was low (phi = 0.1) with excitation into the n = 0 level of S1 but very rapidly increased with excitation into higher levels whether they were harmonics or combination levels. A parallel result was observed upon excitation into S2. Vibrational relaxation/deactivation occurs only between levels of the same vibrational progression. Deactivation from the 0 level of S2 does not occur via levels of S1. The photochemically active modes correspond to the vibrational modes present in the region of the molecule where bond breakage occurs. These results add further proof of the complex nature and number of processes that can occur within excited states of photochemically active molecules.     

Cl2O photochemistry: ultraviolet/vis absorption spectrum temperature dependence and O(3P) quantum yield at 193 and 248 nm

The photochemistry of Cl(2)O (dichlorine monoxide) was studied using measurements of its UV/vis absorption spectrum temperature dependence and the O((3)P) atom quantum yield, Φ(Cl(2)O)(O)(λ), in its photolysis at 193 and 248 nm. The Cl(2)O UV/vis absorption spectrum was measured over the temperature range 201-296 K between 200 and 500 nm using diode array spectroscopy. Cl(2)O absorption cross sections, σ(Cl(2)O)(λ,T), at temperatures <296 K were determined relative to its well established room temperature values. A wavelength and temperature dependent parameterization of the Cl(2)O spectrum using the sum of six Gaussian functions, which empirically represent transitions from the ground (1)A(1) electronic state to excited states, is presented. The Gaussian functions are found to correlate well with published theoretically calculated vertical excitation energies. O((3)P) quantum yields in the photolysis of Cl(2)O at 193 and 248 nm were measured using pulsed laser photolysis combined with atomic resonance fluorescence detection of O((3)P) atoms. O((3)P) quantum yields were measured to be 0.85 ± 0.15 for 193 nm photolysis at 296 K and 0.20 ± 0.03 at 248 nm, which was also found to be independent of temperature (220-352 K) and pressure (17 and 28 Torr, N(2)). The quoted uncertainties are at the 2σ (95% confidence) level and include estimated systematic errors. ClO radical temporal profiles obtained following the photolysis of Cl(2)O at 248 nm, as reported previously in Feierabend et al. [J. Phys. Chem. A 114, 12052, (2010)], were interpreted to establish a <5% upper-limit for the O + Cl(2) photodissociation channel, which indicates that O((3)P) is primarily formed in the three-body, O + 2Cl, photodissociation channel at 248 nm. The analysis also indirectly provided a Cl atom quantum yield of 1.2 ± 0.1 at 248 nm. The results from this work are compared with previous studies where possible.     

Spin-chemical approach to photochemistry: reaction control by spin quantum operation

In this review, the contribution of spin chemistry (in particular, magnetic resonance-related chemistry) to the photochemical field is briefly introduced. First, the development of a time-resolved EPR method and its significant application to radical-related physical phenomena and chemical reactions are presented. Second, a reaction-control method by means of electron spin operations is introduced, and several reaction yield-detected magnetic resonance (RYDMR) methods are presented as applications of this concept. One of the most important physical conclusions is the introduction of the concept of “spin phase relaxation” termed singlet–triplet (S–T) and triplet–triplet (T–T) dephasing, instead of the traditional concepts of longitudinal (T₁) and transversal relaxations (T₂). The effects of strong microwave power on the RYDMR spectrum and time-domain data are analyzed according to this concept. Furthermore, a new detection method is introduced, termed “photoconductivity detected magnetic resonance” (PCDMR), which is applicable exclusively to the system of charge transfer reactions.     

Time-dependent quantum wave-packet description of the 1pi sigma* photochemistry of phenol

The photoinduced hydrogen elimination reaction in phenol via the conical intersections of the dissociative 1pi sigma* state with the 1pi pi* state and the electronic ground state has been investigated by time-dependent quantum wave-packet calculations. A model including three intersecting electronic potential-energy surfaces (S0, 1pi sigma*, and 1pi pi*) and two nuclear degrees of freedom (OH stretching and OH torsion) has been constructed on the basis of accurate ab initio multireference electronic-structure data. The electronic population transfer processes at the conical intersections, the branching ratio between the two dissociation channels, and their dependence on the initial vibrational levels have been investigated by photoexciting phenol from different vibrational levels of its ground electronic state. The nonadiabatic transitions between the excited states and the ground state occur on a time scale of a few tens of femtoseconds if the 1pi pi*-1pi sigma* conical intersection is directly accessible, which requires the excitation of at least one quantum of the OH stretching mode in the 1pi pi* state. It is shown that the node structure, which is imposed on the nuclear wave packet by the initial preparation as well as by the transition through the first conical intersection (1pi pi*-1pi sigma*), has a profound effect on the nonadiabatic dynamics at the second conical intersection (1pi sigma*-S0). These findings suggest that laser control of the photodissociation of phenol via IR mode-specific excitation of vibrational levels in the electronic ground state should be possible.     

高量子产率水溶性CdTe量子点的制备与表征

以巯基乙酸(HSCH2 COOH,TGA)为稳定剂,在水相中合成高量子产率CdTe量子点(QDs),产率达68%.用紫外.可见分光光度计、荧光分光光度计、红外光谱仪、透射电子显微镜等对制备的样品进行表征.结果表明:CdTe Ods紫外吸收峰及荧光发射峰均随回流时间延长而红移,即粒径在不断增大;荧光发射峰窄而对称,表明QDs分散性好、大小较均一,半峰宽随回流时间延长而逐渐变宽,表明粒径在增大的同时粒径分布范围也变宽;从TEM及紫外.可见光谱推算,可知其粒径约为3 nm;红外光谱图说明作为稳定剂的巯基乙酸对QDs表面起到修饰作用.     

Influence of quantum dot's quantum yield to chemiluminescent resonance energy transfer

The resonance energy transfer between chemiluminescence donor (luminol-H₂O₂ system) and quantum dots (QDs, emission at 593 nm) acceptors (CRET) was investigated. The resonance energy transfer efficiencies were compared while the oil soluble QDs, water soluble QDs (modified with thioglycolate) and QD-HRP conjugates were used as acceptor. The fluorescence of QD can be observed in the three cases, indicating that the CRET occurs while QD acceptor in different status was used. The highest CRET efficiency (10.7%) was obtained in the case of oil soluble QDs, and the lowest CRET efficiency (2.7%) was observed in the QD-HRP conjugates case. This result is coincident with the quantum yields of the acceptors (18.3% and 0.4%). The same result was observed in another similar set of experiment, in which the amphiphilic polymer modified QDs (emission at 675 nm) were used. It suggests that the quantum yield of the QD in different status is the crucial factor to the CRET efficiency. Furthermore, the multiplexed CRET between luminol donor and three different sizes QD acceptors was observed simultaneously. This work will offer useful support for improving the CRET studies based on quantum dots.     

Asymptotic quantum yield of triplet sensitized decomposition

The asymptotic quantum yield of triplet energy transfer is found by calculating the fraction of acceptor molecules with energy above the minimum energy for decomposition. This is done by allowing for a statistical energy distribution among the internal modes in the collision complex. It is found that for a monatomic triplet donor most of the triplet energy is transferred to the acceptor molecule, while for a polyatomic donor molecule only a fraction of it is available for future decomposition of the acceptor.     

栀子甙对碲化镉量子点的荧光淬灭作用

以3-巯基丙酸作为稳定剂,在水溶液中合成了CdTe量子点;采用荧光光谱法初步研究了栀子甙对巯基丙酸稳定的CdTe量子点的荧光淬灭作用,考察了量子点浓度、pH、反应时间等多种因素对量子点-栀子甙体系荧光强度的影响,确定了测定栀子甙的最佳实验条件;并初步探讨了栀子甙与该量子点相互作用的可能反应机理.结果表明,在最佳实验条件下,巯基丙酸稳定的CdTe量子点对栀子甙检测的线性范围为2×10-7~4×10-6 mol/L,检出限为1.4×10-7 mol/L,相对标准偏差为0.355%;且常见的金属阳离子、糖类和氨基酸对栀子甙的测定无显著影响.总体而言,该方法可用于人体体液中栀子甙的检测,且两者的作用过程可初步推断为动态淬灭过程.     

Fluorescence quantum efficiencies of halogen-substituted benzoic acid isomers

The fluorescence of halogen-substituted benzoic acid isomers is enhanced by the addition of an aliphatic acid to chloroform as the solvent. The molar absorptivities of these isomers ar the wavelength of maximum absorbance are reported. The fluorescence quantum efficiencies of the fluorescent species from these isomers in 5% acetic acid/ chloroform are also reported.     

UV laser photochemistry and diborane at 193 nm: Quantum yield for BH3 production

The quantum yield ø_BH3 for BH₃ production from ArF-laser-excited B₂H₆ was determined to be 2.00 ± 0.25 by trapping with PF₃. The former postulate of BH₃ as a chain carrier in ArF-laser-induced B₂H₆-D₂ exchange is confirmed.     

A quantum yield map for synthetic eumelanin

The quantum yield of synthetic eumelanin is known to be extremely low and it has recently been reported to be dependent on excitation wavelength. In this paper, we present quantum yield as a function of excitation wavelength between 250 and 500 nm, showing it to be a factor of 4 higher at 250 nm than at 500 nm. In addition, we present a definitive map of the steady-state fluorescence as a function of excitation and emission wavelengths, and significantly, a three-dimensional map of the "specific quantum yield": the fraction of photons absorbed at each wavelength that are subsequently radiated at each emission wavelength. This map contains clear features, which we attribute to certain structural models, and shows that radiative emission and specific quantum yield are negligible at emission wavelengths outside the range of 585 and 385 nm (2.2 and 3.2 eV), regardless of excitation wavelength. This information is important in the context of understanding melanin biofunctionality, and the quantum molecular biophysics therein.     

Fluorescence probe for microenvironments: anomalous viscosity dependence of the fluorescence quantum yield of p-N,N-dialkylaminobenzylidenemalononitrile in 1-alkanols

The effect of solvent viscosity on the fluorescence quantum yield of p-N,N-dialkylaminobenzylidenemalononitrile has been studied in alcoholic solvents with viscosities ranging from 0.55 to 115 cP. The observed effect is shown to be a direct consequence of the molecular rotation of surrounding solvent molecules.     

Mechanisms in the quantum yield of Cypridina bioluminescence

Abstract— –The influence of temperature, pH, salts, and reactant concentrations on the biolumin-escent oxidation of Cypridina luciferin catalyzed by Cypridina luciferase indicates a highest quantum yield φ (einsteins per mole of luciferin oxidized) of 0.31 in H₂O, or 0.33 in 99% D₂O. With the aid of data on fluorescence of the light-emitting oxyluciferin-luciferase complex, and of oxyluciferin in diglyme, partial explanations are suggested for the observed variations in φ, including the relatively low φ, of 0.03 for chemiluminescence of luciferin in organic solvents, wherein a different pathway of luciferin degradation, as indicated by chromatographic evidence, results in much less population of the excited state.