Distinction of the delayed fluorescences S1 → S0 And S2 → S0 of pyrene by selective quenching Of S1 → S0

In the spectrum of the delayed fluorescence (DF) of pyrene, caused by triplet-triplet annihilation T₁ + T₁ → S_n + S_o (n = 1,2), a strong DF S₁ → S_o and a very weak DF S₂ → s₀ are observed. The DF S₁→ S_o is quenched selectively by compounds like N-diethylanine or triethylamine which do not quench T₁ of pyrene.     

Laser excited S2 → S1 and S1 → S0 emission spectra and the S2 → Sn absorption spectrum of azulene in solution

We present the S₁ → S₀ fluorescence spectrum, between 740 and 940 nm, of azulene solutions (10^?3 M in methanol) excited with a Q-switched ruby laser. The nitrogen-laser excited S₂ → S₁ fluorescence spectrum, between 700 and 930 nm, is also reported. The transient S₁ → S_n spectrum between 500 and 650 nm was studied, using synchronous nitrogen laser and dye laser excitation. The S₅ (¹B₁(3)) state of azulene was found to be located at 45500 cm^?1 and the cross section σ₂₅ of the transient absorption S₂ → S₅ is estimated to be 3 × 10^?18 cm²/molecule.     

Investigation of the internal conversion time of the chlorophyll a from S3, S2 to S1

By using femtosecond time-resolved stimulated emission pumping fluorescence depletion (FS-TR-SEP-FD), we present a fluorescence depletion study of chlorophyll a (Chl a) in various solvent environments. Internal conversion times (IC) in different solvents are observed. It is found that all the S₃ and S₂ to S₁ transition processes are extremely fast, and that the time constants of these processes range from 100 to 260 fs. In aprotic solvent, the rate of IC decreases with an increasing of solvent polarity.     

Relative quantum yield of the S2 → S1 fluorescence from azulene

The quantum yield ratio r = φ_{2 → 0}/φ_{2 → 1} of the S₂ → S₀ and S₂ → S₁ fluorescences from azulene has been redetermined. With azulene in isopentane at 190 K, r = 455 ± 100. This value agrees with the lower limit, given by Huppert, Jortner and Rentzepis, but is an order of magnitude lower than that given by Gillispie and Lim.     

Anomalous fluorescence of aceanthrylene: An example of second excited state emission (S2 → S0)

An anomalous fluorescence with a quantum yield of 0.017 near 24000 cm^?1 is detected from hexane solutions of aceanthrylene. Excitation and synchronous scan spectra verify that the second excited state with a lifetime of 4.3 ns is the source of the fluorescence. The absorption spectrum is simulated by PPP SCF CI computations.     

Fluorescence of DPH derivatives. Evidence for emission from S2 and S1 excited states

Absorption, fluorescence excitation and emission spectra, quantum yields, and fluorescence decay times have been measured for several derivatives of all-trans 1,6-diphenyl-1,3,5-hexatriene (DPH) in a number of solvents. Emission occurs from the low-lying ¹Ag^*_g state and the ¹B^*_u which is at slightly higher energy. Accepted models for the photophysics of DPH are shown to be inadequate.     

Picosecond time resolved energy transfer between rhodamine 6G and malachite green

The process of singlet—singlet resonance energy transfer between rhodamine 6G (donor) and malachite green (acceptor) has been studied with a picosecond laser : streak camera system. Unlike previous investigations, the measurements were conducted in a low viscosity solvent (ethanol) at room temperature. The donor fluorescence decay function was found to be in agreement with that predicted by the Förster theory over a tenfold range of acceptor concentrations (10^?3 M to 10^?2 M) and up to a limiting time resolution of 10 ps. An average R₀ value of 52.5 A was obtained from the fluorescence decay curves, in reasonable agreement with the value of 48 A calculated from spectroscopic data.     

Synthesis and characterization of methylpalladium(II) dithiolate complexes of the type [PdMe(SS)(ER3)] (SS = S2CNR 2, S2COEt, S2P(OR)2, S2 PPh2; ER3 = PMePh2, PPh3, AsPh3)

Methylpalladium(II) dithiolate complexes of the type [PdMe(SS)(ER₃] (SS = S₂ CNR₂ (R = Me or Et), S₂COEt, S₂P(OR)₂ (R = Et, ⁿPr, ⁱPr), S₂PPh₂; ER₃ = PMePh₂, PPh₃, AsPh₃) have been synthesized by the reaction of [Pd₂Me₂(μ-Cl)₂(PMePh₂)₂] with sodium/potassium/ammonium salts of the dithio acid or by treatment of [PdMeCl(cod)] with ER₃ followed by sodium/potassium/ammonium salts of the dithio ligand. All the complexes were characterized by elemental analysis, IR and nuclear magnetic resonance (¹H, ³¹P) data.     

Vibrational energy transfer in CH2F2

Infrared fluorescence has been observed from the ν₁, ν₆, 2ν₉, ν₈ and ν₄ levels of CH₂F₂ following excitation by a 9.6 μ Q-switch CO₂ laser. All the observed states exhibit a single exponential decay rate of approximately 44 msec^?1 torr^?1. The rare gas dependence of this rate has also been measured and found to be up to 20 times slower than the rate for the pure gas. Measurements of the risetimes of the observed fluorescence signals yielded an upper limit of 5 μsec at 1 torr for the ν₁, ν₆ and ν₈ levels. The 2ν₉ and ν₄ risetimes were effectively instantaneous under the experimental conditions that prevailed. The relative magnitudes of the measured rate are discussed in terms of existing V-T/R theories and collisional energy transfer processes.     

Inter-sublattice energy transfer in MnF2

The magnetically induced circular emission (MCE) of an exciton—magnon pair from the third nearest neighbour impurity trap [Mgσ(III)] in MnF₂ shows an unusual lineshape. The field dependence of the MCE suggests that this is a consequence of a magnon assisted transfer of excitation between sublattices via the intrinsic exciton band.     

Study of near resonant energy transfer from laser excited CO2 to SO2

Collisional energy transfer from CO₂ to SO₂ was studied subsequent to pumping of CO₂ (ν₃) by a Q-switched laser. The measurements were made in the temperature range 300–800 K and in the pressure range 1–30 Torr. The fluorescence from the ν₃ level of CO₂ was monitored with the help of a Ge:Au detector at 77 K with an estimated response time of ≈2 μs. The probability of the energy transfer was found to be increasing with increasing temperature. The probable kinetic models for the V---V relaxation pathways were discussed and the experimentally measured energy transfer rate is related to the cross-over transfer processes. Theoretical calculations using both a simple SSH-breathing sphere model and the Sharma-Brau theory were carried out to evaluate the probabilities of the involved cross-over energy transfer processes and the results were compared with the experimental rates.     

Comparisons of energy disposal by the reactions of H atoms with Cl2, SCl2, S2Cl2 and SO2Cl2 from observation of HC1 infrared chemiluminescence

Arrested relaxation infrared chemiluminescence studies of the H + Cl₂, SCl₂, S₂Cl₂, SOCl₂ and SO₂-Cl₂ reactions have been made. The mean fraction of vibrational (stational) energy released to HCl is 0.40 (0.10); 0.40 (0.13); 0.38 (? 0.02); 0.33 (?0.02) and 0.36 (?0.02) for the series. Only the H + SCl₂ reaction shows a two component initial rotational distribution. The larger (f_V) and (f_R) from H + SCl₂, relative to the other polyatomic reagents, is consistent with the observation that this is the only reaction that shows forward scattering. The room temperature rate constants also were measured, relative to H + Cl₂, and were found to decline in the series from 0.68 for SCl₂ to 0.02 for SO₂Cl₂. All of these data support the suggestion (first made by Heydtmann and Polanyi) that the unusual rotational energy disposal pattern from H + SCl₂ is a consequence of migration of H from the initially encountered C1 to the second C1, which then forms the HCI product; this pathway augments the direct reactive pathway, which gives HCI in lower J states.     

Ultrafast Decay Dynamics of 2-Hydroxypyridine Excited to S1 Electronic State

The S\begin{document}$_1$\end{document} state decay dynamics of 2-hydroxypyridine following UV excitation at a wavelength range of 276.9\begin{document}$-$\end{document}250.0 nm is investigated using femtosecond time-resolved photoelectron imaging technique. Based on pump wavelength dependence of the decay dynamics, a refined decay picture is proposed. At pump wavelength of 276.9 nm, the S\begin{document}$_1$\end{document} state is depopulated through intersystem crossing to lower triplet state(s). At 264.0 nm, both intersystem crossing to lower triplet state(s) and internal conversion to the ground state are in operation. At 250.0 nm, internal conversion to the ground state becomes dominated.     

Structures of 1,2,3-trihydroxybenzene in the S0 and S1 states

In this paper we report on the structure and vibrations of gaseous pyrogallol (1,2,3-trihydroxybenzene) in the electronic ground state (S₀) and its first electronically excited state (S₁). Both ab initio CASSCF/CASMP2 calculations as well as R2PI spectroscopy have been performed. From the ab initio calculations three minimum energy structures are obtained and the vibrations of two structures are observed in the R2PI spectra. The minimum energy structures differ by their OH torsional angles. The full three-dimensional potential energy surface of the coupled torsional motions is investigated and the three-dimensional eigenvalues are calculated. The most stable structure of pyrogallol contains two intramolecular hydrogen bonds and turns out to be planar in the S₀ state. In the S₁ state the free OH group is rotated out of the plane of the aromatic ring by about 40°. The strong change in geometry of this structure is predicted by the CASSCF calculations and confirmed by the R2PI spectra of pyrogallol and its deuterated species. The low frequency region of the R2PI spectra can be explained by a torsional motion and the out of plane vibration 17b.     

Resonant raman scattering from the S2 ion in NaI

The S₂⁻ molecule ion in NaI crystals exhibits multiple-order resonance Raman scattering at 80 K with little background luminescence. Relative scattering efficiencies measured for up to nine Raman overtones are compared with the theory of Hizhnyakov and Tehver.     

S2 → S0 fluorescence in an aromatic thioketone, xanthione

In addition to the red phosphorescence (T₁(³ A₂n, π^*) → S₀) xanthione exhibits in solution an emission with a maximum at ≈ 23 000 cm⁻¹ and φ_f(298°) = 5 × 10⁻³. It is shown that this emission is fluorescence from the second excited singlet state (S₂ (¹A₁ π, π^*) → S₀).     

Comparative sensibility of S1 ←S0 and S2 ←S0 indole electronic transitions to environment perturbations. The positions of the 0—0 bands in polar media

The modifications under environmental perturbations of the well separated two first electronic systems of carbazole are used to demonstrate the possibility of including solute-ether complexes in polyethylene films. The application of this technique to indole allows to differentiate the overlapping ¹L_a and ¹L_b transitions in the spectrum of hydrogen bonded indole. The ground state interactions of indole, 5-methoxyindole and 3-methylindole in several well defined environment conditions (hydrogen bond in a polar cage, hydrogen bond in a nonpolar cage) are investigated through UV absorption spectroscopy between 293 and 88 K. A strong red shift of the ¹L_a bands under the hydrogen bonding occurs with all the indoles investigated. The comparative analysis of the spectra in three types of environment, allows to give the accurate location of the first bands for the two overlapping vibronic systems of these molecules in polar media. Particularly, it is unambiguously shown that the first ¹L_a band and the first ¹L_b band of indole in alcohols are superposed at 288 nm. These results offer reliable new bases for the study of the emission properties of indole and its derivatives.     

Theory of the S0 → S1 two-photon transition in benzene

The symmetry forbidden two-photon excitation spectrum recently observed in benzene vapour gave intensities inverted from those expected by current predictions based on the Herzberg-Teller theory for vibronic induced processes. We show that an extension of the HT approximation which allows us to correlate the movement of electrons and nuclei leads to an agreement with the experimental results.     

Dual fluorescence (S1, S2) in chrysene and 3,4-benzophenanthrene

S₂ and S₁ fluorescence of chrysene and 3,4 benzophenanthrene has been observed in the vapour phase under collision free conditions. It is shown that the intermediate strong couplinng model can be applied to these molecules. The efficiency of the transfer of the excess energy to collision partners is given for different gases.