FLUORESCENCE OF THYMINE IN AQUEOUS SOLUTION AT 300° K

Abstract— –Fluorescence of thymine in neutral aqueous solution at room temperature has been detected using the multiscaling operation of a multichannel analyzer. The emission maximum (2.96 μm^-1) and 0-0 transition energy (3.37-3.45 μm^-1) are close to those determined at liquid nitrogen temperature in mixed solvents. The quantum efficiency of fluorescence excited at 3.77 μm^-1 is calculated to be 1.04 × 10^-4.
The corrected relative excitation spectrum shows significant differences from the absorption spectrum when both are determined under identical conditions of concentration and spectral bandwidth on the same instrument. The quantum yield of fluorescence decreases about 2-fold as the energy of excitation is increased beyond the 0-0' transition and follows the relation 1/φ°α E _excit..
This behavior is discussed in terms of (a) n π* and ππ* states, (b) emission from a minor tautomer and (c) kinetics of competing deactivation processes.     

PHOTOPHYSICAL PROPERTIES OF NUCLEIC ACID COMPONENTS—1. THE PYRIMIDINES: THYMINE, URACIL, N, N-DIMETHYL DERIVATIVES AND THYMIDINE

Abstract— Low-temperature (and some room temperature) absorption and emission, fluorescence and phosphorescence, data including quantum yields and lifetimes have been obtained from the title pyrimidine bases as a function of the nature of the solvent environment. Modest vibrational resolution has been observed for the first time in the absorption spectra, particularly for thymine and uracil. The excitation spectra also show structure. The quantum yields of fluorescence (φ_F) and phosphorescence are independent of the excitation wavelength. Thymine, thymidine and uracil have profoundly different photophysical properties in polar-aprotic vs polar-protic solvents. The N, N-dimethyl substitution of thymine and uracil produces photophysical changes comparable to the solvent change for the unsubsti-tuted bases. The species involved in the emission processes is the keto (lactam) form. It is probable that ^1,3(n,π*) state(s) has(have) changed order relative to a lowest ¹(π,π*) state as a consequence of both the solvent change and N, N-dimethyl substitution. The lowest triplet state is assigned as ³(n π*). We propose that an important factor contributing to the previously reported excitation wavelength dependence of φ_F and φ_T1 (φ_isc) for nucleic-acid components is the equilibrium coexistence of H-bonded and non-H-bonded forms each having different photophysical properties. Consideration is given of the impact of the significantly different photophysical properties of nucleic-acid bases as a function of the nature of the solvent upon the photochemical properties.     

PHOTO-DIMERIZATION AND PHTO-REDUCTION OF ALPHA-NAPTHOQUINONE IN DIFFERENT SOVENT MEDIA

Abstract -Violet and ultravioet radiation are equally efficient in phot-dimerizing aplhanathoquinone in benzene. The reactants yielding the dimeric photo-product are moelcules in the ground state and excited ones. The photo-reduction in 2-propanol occurs with the same effciency for excitation in the n→* and →π* absorption bands. It is concluded that either reaction occurs via an n,π* excited state molecule, by direct excitation or after 100 per cent effucient internal conversion from the π,π* to the n,π* state.     

Photoinduced ultrafast processes in phenyl-substituted poly(phenylenevinylene) s studied by picosecond absorption,fluorescence and conductivity measurements

Transient absorption, fluorescence and conductivity were measured on phenylated poly(phenylenevinylene)s (P-PPV) in solution and in film after UV pulse excitation in picosecond region. Transient absorption bands of distinguishable rise and decay kinetics were observed. The fluorescence shows two exponential decay times in ps- and ns-region, resp, Transient photoconductivity also exhibits a ps- and a ns-time component. The mobility of carriers was estimated.     

DEPENDENCY OF APPARENT RELATIVE QUANTUM YIELD OF ISORHODOPSIN TO RHODOPSIN ON THE PHOTON DENSITY OF PICOSECOND LASER PULSE

Abstract— The quantum yield of bleaching of isorhodopsin relative to that of rhodopsin was measured by irradiation of both pigments with a steady light source or a picosecond laser pulse. The each pigment was prepared by incubation of 11- cis or 9 -cis retinal with opsin, respectively. The ratio of isorhodopsin to rhodopsin in the quantum yield was estimated to be 0.37 using irradiation with a steady light, while with a weak picosecond laser pulse (excitation photon density: below 20 μ.J/1.8 mmφ), it was estimated to be 0.39. Both values are in good agreement with each other. On the other hand, excitation with a strong picosecond laser pulse (above 20 μ.J/1.8 mmφ) produced a larger ratio than 0.39, indicating that saturation effects can be easily observed by irradiation with strong picosecond laser pulses.     

Measurements of intersystem crossing kinetics using 3545 Å picosecond pulses: nitronaphthalenes and benzophenone

The build-up of triplet-triplet absorption following singlet excitation was measured for 1- and 2-nitronaphthalene and benzophenone on a picosecond time scale in the condensed phase. A single, picosecond pulse from a mode-locked Nd³⁺/glass laser was used to produce excitation at the laser third harmonic, 3545 Å, while the second harmonic at 5300 Å was used to probe the known triplet-triplet absorption in the nitronaphthalenes and benzophenone. Solvent effects on the build-up rates in these molecules are exposed. In the case of benzophenone, we discuss solvent assisted vibrational relaxation and intersystem crossing contributions to these rates. The anomaly of intersystem crossing at a rate of ca. 10¹¹ s^-1 with a triplet yield of less than 1 for the nitronaphthalenes is discussed.     

LASER PULSE EXCITATION STUDIES OF THE FLUORESCENCE OF CHLOROPLASTS

Abstract. The fluorescence yield, φ, as a function of single picosecond laser pulse intensity was experimentally studied in spinach chloroplasts and for chlorophyll a in ethyl ether solution. The progressive decrease in φ with increasing incident intensity for in vivo chlorophyll was found to be adequately explained within the context of continuum bimolecular kinetics with a singlet-singlet fusion rate constant of γ=5×^-9cm^-3s^-1 at room temperature. We discuss qualitatively how the fluorescence quantum yield depends on the duration and intensity of the incident pulse. The identity of φ vs l (the number of absorbed quanta) curves at the emission maxima of 685 nm and 735 nm for single picosecond pulse mode of excitation is explained within the context of Butler's tripartite model of the fluorescence of chloroplasts at 77 K. Various models relating γ to the singlet exciton diffusion coefficient and the Förster energy transfer rate are used to infer lower bounds to these physical parameters. Predictions and supporting experimental evidence for the tripartite model are discussed.     

Investigation of the excited-state absorption of a Ru dioxolene complex by the Z-scan technique

We investigated nonlinear absorption of picosecond laser pulses in a Ru complex [{Ru(bipy)2}2L][PF6] using the open-aperture Z-scan technique. Experiments were performed in a spectral region of moderate linear absorption (lambda=532 nm, sigmag=0.65 x 10(-16) cm(-2)). We observed a transition from reverse saturable absorption to saturable absorption when the excitation intensity was higher than 50 GW/cm2. To determine the population level kinetics, a model based on three- and four-level systems was considered, and the rate equations solved taking into account the propagation equation of the laser pulse inside the sample. Fitting of the experimental data allows extraction of the excited-states absorption cross sections and lifetimes.     

FLUORESCENCE QUANTUM YIELDS OF 124-kDa PHYTOCHROME FROM OAT UPON EXCITATION WITHIN DIFFERENT ABSORPTION BANDS

Abstract— A fluorescence quantum yield (emission at650–850 nm) of π= (2.3 ± 0.3)10⁻³ was measured for the red-absorbing form (Pr) of 124-kDa phytochrome from etiolated oat seedlings ( Avena sativa ) upon excitation in the Soret band at Λ^exc= 380 nm. The small difference between this value and the previously determined quantum yield with Λ^exc= 640 nm, π= (3.5 ± 0.4)10⁻³is attributed to a blue-absorbing emitter responsible for the "anomalous" or "blue" emission of the chromoprotein in the region from ca. 400 to 550 nm. The absorption of Pr at 380 nm is consequently somewhat lower than that measured directly from the spectrum. Processes from upper excited states of the Pr phytochromobilin-derived chromophore other than rapid relaxation to the emitting state are not important. A quantum yield of Φ ' 1.2 times 10⁻³ is estimated for the blue fluorescence. The proportion of the blue emitters relative to Pr appears to be relatively high.     

Transient absorption induced by a picosecond electron pulse in the fused silica windows of an optical cell

The transient absorption induced by picosecond pulse radiolysis in the windows of a fused silica optical cell is investigated with pump probe techniques in the UV and the visible range. After excitation with an electron pulse of 7 MeV and an effective duration of around 10 ps the absorbance changes during relaxation are recorded up to nanoseconds with a supercontinuum and a single wavelength probe at 263 nm. The complex spectral signatures and kinetics of the empty cell are set into relation with the transient absorption of water radiolysis. Special care is taken to assure equal irradiation conditions for the comparative measurements over the large spectral range. The results reveal clearly that the transient absorption induced in the fused silica cell is not negligible. The transient signals due to the cell should be considered in picosecond pulse radiolysis of solutions in order to avoid important errors on the time dependent yield of transient species, particularly of those absorbing in the UV.     

Excited state absorption dynamics in metal cluster polymer [WS4Cu3I(4-bpy)3]n solution

The nonlinear absorptive property of a novel metal cluster [WS(4)Cu(3)I(4-bpy)3]n in DMF solution is studied by using an open-aperture Z-scan technique with picosecond and nanosecond laser pulses at the wavelength of 532 nm. The experimental results show that the cluster has strong nonlinear absorption under the 8 ns pulse excitation and a relatively weak nonlinear absorptive property under the picosecond pulse excitation. The picosecond pump-probe response of the metal cluster is similar to that of C60 solution, which implies that the nonlinear mechanisms are the same for the two materials. By using the rate-equation model, the experimental data are theoretically simulated; several optical parameters of the cluster, especially the lifetime of the higher excited singlet state of the cluster, are obtained.     

Chemically Initiated Electron Exchange Luminescence of Silyloxyaryl-Substituted Spiroadamantyl Dioxetanes: Kinetics and Excited State Yields

Abstract— The kinetics of the fluoride-induced decomposition of the thermally stable silyloxyaryl-substituted spiroadamantyl dioxetanes 1a,b and the excited state formation of this chemically initiated electron exchange luminescence (CIEEL) have been investigated. Two limiting kinetic regimes flash and glow have been identified, which depend on the fluoride concentration, the first at high, the second at low [F^-] triggering, whose detailed kinetic analysis affords the rate constants for the deprotected dioxetanes 2a,b cleavage in acetonitrile and dimethyl sulfoxide and chemiluminescence measurements the CIEEL and phen-olate 4 (CIEEL emitter) excitation yields. Chloro-substi-tution in the spiroadamantyl dioxetane does not affect the deprotection step k ₂ but leads to a ca five-fold faster cleavage of the deprotected dioxetane 2, while the chemiexcitation yield is the same for both dioxetanes. The energies of the first excited singlet and triplet states of the emitting phenolate 4 were estimated by AM1 configuration interaction calculations with explicit consideration of acetonitrile as solvent (self-consistent reaction field approach). The first excited singlet and triplet state of the CIEEL emitter phenolate 4 possess π,π* character, as suggested by the π-type molecular orbitals and the large singlet-triplet energy gap. The chemiexcitation of both singlet and triplet states of the excited phenolate 4 is feasible during the dioxetanes 1a,b cleavage, but the experimentally determined high singlet excitation yields suggest that preferentially the phenolate 4 singlet state is populated in the fluoride ion-triggered CIEEL process.     

LUMINESCENCE AND PHOTOCHEMISTRY OF 4-THIOURIDINE IN AQUEOUS SOLUTION

Abstract— In bidistilled water, 4-thiouridine (4TU) exhibits a weak unusual luminescence, the quantum yield of which is 3 × 10^-4 at 25°C. The excitation spectrum corresponds well to the 4TU absorption spectrum. The emission lies at longer wavelengths (Λ_max 550 nm) than the 4TU phosphorescence observed at 77 K (Λ_max, 470–480 nm). From the emission signal obtained after an excitation flash of 3 ns half-width, an "apparent" rate constant for the radiative deactivation process, shorter than 5 × 10⁶ s, can be inferred. The 300 K emission is efficiently quenched by halides and by oxygen: quenching involves a long-lived intermediate (⋍ 200 ns).
Clearly the emissive state X is populated through the S₀-S₁ electronic transition π→π* of 4TU. The nature of X cannot be unambiguously determined: it cannot be an excimer but can be either the 4TU triplet state or another chemical state distinct from the 4TU excited singlet or triplet states.
An interesting finding is that the 300 K emission and the ability of 4TU to photoreact are related: they are quenched with the same efficiency by halide anions. This indicates that quenching occurs at the same long-lived intermediate species , which is either a precursor of the emitter or the emitter itself.     

PICOSECOND ABSORPTION SPECTROSCOPY OF CHLOROPHYLL A DIHYDRATE

Abstract— The solution of chlorophyll a in hexane with more than 70% of chlorophyll molecules in the form of the dihydrate (CHl-a.2H₂O)_n is investigated at room temperature by picosecond absorption technique. The transient difference spectra and the kinetic dependences of the absorption changes are measured for several excitation and probe wavelengths. Creation of a new state with blue-shifted absorption band is observed in the system after excitation. A model of the behaviour of the system after excitation is proposed and checked by comparison of the computer-simulated spectral and time dependences with the experimental data. According to the model, about 30% of excited molecules are in the state with the 0.046 eV shift of the absorption band in comparison with the ground state absorption. The lifetime of this state has 170-ps component. The rest of the excited molecules are in the first excited state with the decay time component of 37 ps.     

Real-time picosecond measurements of electronic energy transfer from DODCI to malachite green and DQOCI

Singlet-singlet resonance energy transfers from DODCI (donor) to malachite green and to DQOCI in ethanolic solutions have been investigated with a real-time picosecond streak-camera (time-resolution 3–5 ps) operating at a repetition rate of 140 MHz, in synchronism with the pulse train from a mode-locked cw dye laser used as excitation source. Acceptor concentrations from 10^?5 M to 7.5 × 10^?3 M were studied and average R_o values of 45.6 Å for malachite green and 61.8 Å for DQOCI are obtained from the directly measured fluorescence decay curves. Departure from Förster kinetics is seen at the lower acceptor concentrations employed.     

时间分辨拉曼光谱研究一氧化氮与肌红蛋白的结合过程

纳秒瞬态拉曼光谱技术是研究分子结构变化超快动态过程的重要实验手段之一.而肌红蛋白(Mb)与小分子配体的结合过程一直是人们研究的焦点.本文旨在利用纳秒瞬态拉曼光谱技术研究小分子配体NO与肌红蛋白结合的动力学过程.通过考察MbNO光解后产物脱氧肌红蛋白(DeoxyMb)与反应物MbNO的ν4特征振动峰的强度比值随激光激发功率的变化,阐述了利用纳秒瞬态拉曼光谱技术研究MbNO体系中NO与DeoxyMb结合过程的可行性.利用纳秒瞬态拉曼光谱技术,获得了与皮秒时间分辨拉曼和皮秒时间分辨吸收相一致的结合动力学实验结果.为研究其它复杂体系的超快结合动力学过程提供了一种新的思路.     

ENERGY TRANSFER AMONG THE CHROMOPHORES OF C-PHYCOCYANIN FROM Anabaena variabilis USING STEADY STATE AND TIME-RESOLVED FLUORESCENCE SPECTROSCOPY

Abstract We have investigated the model of energy transfer between sensitizing (s) and fluorescing (f) chromophores for the αβ monomer and for the separated α and β subunits of C-phycocyanin from Anabaena variabilis using fluorescence emission spectroscopy, fluorescence excitation polarization, and picosecond-resolved fluorescence decay kinetics. The fluorescence emission maximum occurs at 640 nm for all samples. The fluorescence excitation polarization is constant ( P = 0.40) across the absorption hand for the α subunit, but it increases across the absorption band towards longer wavelength for the β subunit and the αβ monomer. The fluorescence decay kinetics exhibit two exponential lifetimes of 1.3-1.5 ns and 340-500 ps for the αβ monomer and for the α and β subunit preparations.
We attribute the change in polarization across the absorption band to energy transfer among the three chromophores in the αβ monomer and among the two chromophores in the separated β subunit. The constant, relatively high polarization in the separated a subunit, having only one chromophore, is consistent with the absence of both energy transfer and chromophore rotation. The concentration of the α subunit did not affect the decay kinetics, suggesting that the short lifetime component does not arise from aggregation of the α subunits. The biexponential decay kinetics of the α subunit cannot be explained using the sensitizing-fluorescing model. The possibility of conformational interactions is under investigation.     

The Electronic Structure of Transient Species in the Photochemical Reduction of Porphyrins

Studies on the electronic structure of -radical anions and -dianions of Zn porphyrins, Zn chlorins, -anions of Zn phlorins, and porphodimethenes by electronic absorption spectroscopy, luminescence, picosecond spectroscopy, ESR, NMR, IR, and Raman spectroscopy are briefly surveyed. The experimental data are compared with the results of quantum-chemical calculations. The electronic structure of M-anions with an excess charge on the central ion of a transition metal (Fe, Ni, Co, and Pd) is discussed.     

Dynamics and mechanisms of the multiphoton gated photochromic reaction of diarylethene derivatives

The cycloreversion (ring-opening) process of one of the photochromic diarylethene derivatives, bis(2-methyl-5-phenylthiophen-3-yl)perfluorocyclopentene, was investigated by means of picosecond and femtosecond laser photolysis methods. The drastic enhancement of the reaction yield was observed only by the picosecond laser exposure. The excitation intensity effect of the reaction profiles revealed that the successive multiphoton absorption process leading to higher excited states opened the efficient cycloreversion process with a reaction yield of (50 +/- 10)%, while the one-photon absorption directly pumped to a higher excited state did not lead to the efficient cycloreversion reaction. These results indicate that not the energy of the excitation but the character of the electronic state takes an important role in the enhancement of the cycloreversion reaction.     

Formation of photochemical π-cation radicals

We have monitored the spectra and kinetics of μ-oxo iron (III) tetraphenyl porphyrin. The spectral changes between 460 nm and 770 nm were observed after excitation with 25 ps fwhm, 355 nm pulse. Kinetic studies from — 100 ps to 4 ns suggest that after the immediate formation of the excited states a transient species is formed which we assign to the π-caion radical-ferrous porphyrin pair. This pair decays with a time constant of 600 ps ± 100 ps leaving a small amount of disproportionation reaction photoproducts. The spectra and kinetics of the transients, were not altered by concentration (0.15 OD – 1.0 OD at 571 nm), solvent or addition of oxygen.