Enhanced triplet formation by twisted intramolecular charge-transfer excited states in conjugated oligomers and polymers

The triplet yield and intersystem crossing rate of a set of conjugated oligomers and polymers that, in polar solvents, form a charge-transfer state with a twisted conformation has been investigated. It was observed that in these dibenzothiophene-fluorene oligomers a greater than 10-fold increase on the triplet yield is achieved by simply changing the medium polarity to favor the formation of the twisted charge-transfer state, while the fluorescence lifetime is only slightly increased. The increase in the intersystem crossing rate is attributed to the improved mixing between the singlet and triplet states in the twisted excited state. In analogous polymers, the intersystem crossing rate does not show the same increase, most likely because of the greater energetic and conformational disorder increasing the intersystem crossing rate at all times, regardless of the formation of the twisted charge-transfer state or not.     

Photodissociation of N2O: triplet states and triplet channel

The role of triplet states in the UV photodissociation of N(2)O is investigated by means of quantum mechanical wave packet calculations. Global potential energy surfaces are calculated for the lowest two (3)A' and the lowest two (3)A' states at the multi-reference configuration interaction level of electronic structure theory using the augmented valence quadruple zeta atomic basis set. Because of extremely small transition dipole moments with the ground electronic state, excitation of the triplet states has only a marginal effect on the far red tail of the absorption cross section. The calculations do not show any hint of an increased absorption around 280 nm as claimed by early experimental studies. The peak observed in several electron energy loss spectra at 5.4 eV is unambiguously attributed to the lowest triplet state 1(3)A'. Excitation of the 2(1)A' state and subsequent transition to the repulsive branch of the 2(3)A' state at intermediate NN-O separations, promoted by spin-orbit coupling, is identified as the main pathway to the N(2)((1)Σ(g)(+))+O((3)P) triplet channel. The yield, determined in two-state wave packet calculations employing calculated spin-orbit matrix elements, is 0.002 as compared to 0.005 ± 0.002 measured by Nishida et al. [J. Phys. Chem. A 108, 2451 (2004)].     

Zero-field splittings in aromatic triplet states

The zero-field splitting parametersD andE have been calculated for naphthalene using T.B.M. and I. R. M. wave functions, and accurate values of all significant two, three and four centre dipolar interaction integrals. Agreement with experiment is improved in the case ofE, but is less satisfactory forD.     

Exciplexes in highly excited triplet states

A mechanism of energy transfer from highly excited triplet aromatic molecules has been developed, which involves a stage of formation of an exciplex between a highly excited energy-donor molecule and an unexcited energy-acceptor molecule. Interpretation of the experimental data on the shape and the intensity of triplet-triplet absorption bands and the energy transfer probability is presented. In this interpretation, the results of quantum-chemical calculations of the energies of highly excited triplet states of toluene and benzene molecules are used.     

New excited state intramolecular proton transfer (ESIPT) dyes based on naphthalimide and observation of long-lived triplet excited states

A new excited state intramolecular proton transfer chromophore of naphthalimide (NI) conjugated 2-(2-hydroxyphenyl) benzothiazole () was prepared which shows red shifted absorption and long-lived triplet excited states.     

Semiempirical calculations on triplet and doublet states

Restricted open-shell SCF calculations are carried out on triplet states of electron systems and doublet states of some of their ions. The results are compared with the ones obtained by limited configuration interaction and by the use of Koopman's theorem. For some examples open-shell SCF wavefunctions are expanded into linear combinations of Slater determinants representing configurations built from closed-shell SCF orbitals. This allows a more detailed comparison of the different methods of calculation.

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Zusammenfassung Berechnungen nach der beschränkten SCF Methode für offene Schalen werden an Triplettzuständen von -Elektronensystemen und Dublettzuständen einiger ihrer Ionen ausgeführt. Die Resultate werden mit denjenigen verglichen, welche die beschränkte Konfigurationswechselwirkung und der Satz von Koopmans liefern. Die SCF Wellenfunktionen für offene Schalen werden, für gewisse Beispiele, in Linearkombinationen von Slater-Determinanten entwickelt, welche aus SCF Orbitalen für geschlossene Schalen aufgebaut sind und verschiedene Konfigurationen darstellen. Dies erlaubt einen eingehenderen Vergleich der verschiedenen Berechnungsmethoden.

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Résumé Des calculs selon la méthode SCF avec restriction pour les couches ouvertes sont effectués sur les états triplets de systèmes d'électrons et sur les états doublets de certains de leurs ions. Les résultats sont comparés à ceux obtenus par la méthode d'interáction de configurations limitée et par l'emploi du théorème de Koopmans. Pour certains exemples les fonctions SCF à couches ouvertes sont développées en combinaison linéaire de déterminants de Slater représentant des configurations bâties à partir d'orbitales S.C.F. de couches fermées. Cela permet une comparaison plus détaillée des différentes méthodes de calcul.

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Presented in parts at the Theoretical Chemistry Symposium in Vienna, March 1967.     

Theoretical study of low-lying triplet states of aniline

Multireference complete active space self-consistent-field CASSCF(10,12)/ANO and second-order perturbation theory MS-CASPT2 calculations were performed to determine the vertical low-lying singlet and triplet states of aniline. The sequence of the seven lower lying triplet states is T1(1(3)A'), T2(1(3)A' '), T3(2(3)A'), T4(3(3)A'), T5(2(3)A' '), T6(4(3)A'), and T7(3(3)A' '). The 3(3)A', 4(3)A', and 3(3)A' ' states are assigned as 3s, 3py, and 3pz Rydberg states, respectively, while other states correspond to pi <-- pi excitations. Both the T1 and T2 states are found to be below at the lowest-lying singlet S1 (1(1)A' ') state. Geometry, vibrational modes, and electron distribution of the lowest lying T1 state were determined using UB3LYP calculations. The vertical and adiabatic singlet-triplet energy gaps DeltaE(S0-T1) amount to 3.7 and 3.5 +/- 0.2 eV, respectively. In clear contrast with the S0 state, the triplet aniline is no longer aromatic, and its protonation occurs preferentially at the ring meta-carbon site, with a proton affinity PA = 243 +/- 3 kcal/mol.     

Lowest excited triplet states of hypericin and isohypericin

The fluorescence and phosphorescence of hypericin and isohypericin were studied in an ethanol matrix at 1.2 K. The prompt fluorescence spectra are mirror images of the absorption around the 0-0 transition, as expected. The 0-0 vibronic lines of the phosphorescence are found at 13190 and 13622 cm⁻¹, and the phosphorescence decay times are 2.79 and 6.6 ms at 1.2 K for hypericin and isohypericin respectively. The fluorescence excitation spectrum of isohypericin reveals a small trace of a different pigment, possibly a tautomeric form of isohypericin. The decay of the phosphorescence of isohypericin is biexponential. The slow component is attributed to an unknown contaminant with a high quantum yield of phosphorescence.     

Low-lying singlet and triplet electronic states of RhB

The low-lying XSigma+, a3Delta, A1Delta, b3Sigma+, B1Pi, c3Pi, C1Phi, D1Sigma+, E1Pi, d3Phi, and e3Pi electronic states of RhB have been investigated at the ab initio level, using the multistate multiconfigurational second-order perturbation (MS-CASPT2) theory, with extended atomic basis sets and inclusion of scalar relativistic effects. Among the eleven electronic states included in this work, only three (the X1Sigma+, D1Sigma+, and E1Pi states) have been investigated experimentally. Potential energy curves, spectroscopic constants, dipole moments, binding energies, and chemical bonding aspects are presented for all electronic states.     

Ro-vibrational states of triplet H2D+

We present rotational term values for J < or = 3 of the vibrational states with up to twofold excitation of H2D+ in the lowest electronic triplet state (a3sigma(u)+). The calculations were performed using the method of hyperspherical harmonics and our recent accurate double many-body expansion potential energy surface.     

Monomer and excimer triplet states in glassy phenanthrene

Phosphorescence spectra recorded with vapor-deposited glassy phenanthrene layers reveal the existence of several inhomogeneously broadened monomeric triplet traps of structural origin and two excimeric triplet traps. Temperature-dependent studies yield estimates for both the triplet excimer binding energies and the parameters governing triplet trapping kinetics.     

Models for intramolecular triplet exciton migration applied to vinyl aromatic polymers

Models for intramolecular triplet exciton migration have been developed for vinyl aromatic polymers. A one-dimensional model which allows only neighbor-to-neighbor migrations yields frequencies which are several orders of magnitude smaller than those predicted either by exchange or dipole-dipole mechanisms. An intramolecular model permitting three translational degrees of freedom predicts triplet exciton hop frequencies on the order of 10⁴ s⁻ in reasonable agreement with either exchange or dipole-dipole mechanisms.     

Efficient triplet pair separation from intramolecular singlet fission in dibenzopentalene derivatives

In intramolecular SF(iSF), the strong coupling nature and confinement of diffusional separation of ~1(TT) limits the extraction and harnessing of triplet energy. In order to investigate the possible ~1(TT) separation and the role of molecular parameters on it, a series of iSF-capable dibenzopentalene derivatives(DBPs) have been synthesized and their photoinduced dynamics are monitored. iSF takes place in DBPs, accompanied by consecutive ~1(TT) separation in polycrystalline film with almost ~100% yield. It is suggested the strong intermolecular coupling provided by the closely packing configuration in the film facilitates the disentanglement of correlated ~1(TT). Highly efficient triplet pair separation to yield free triplets makes one step forward for utilizing triplet energy from iSF materials for further optoelectronic applications.