Crystal perfection and triplet excitons in 1,4-dibromonaphthalene

The phosphorescent behaviour of 1,4-dibromonaphthalene single crystals at liquid-helium temperatures is strongly influenced by the crystal preparation techniques. Crystal unperfections appear to be essential for observing excitonic emission. A comparison is made between crystals grown from the melt, solution and vapour. Experiments on crystals doped with DBN-d₆ confirm the proposed model.     

Energy-band structure and charge distribution for BaC6

An ab initio self-consistent calculation has been carried out for the electronic properties of BaC₆. Energy bands and charge densities are presented for BaC₆ and compared with those of LiC₆. The results show that the band originating from Ba states has a mixture of s and d character and the d component hybridizes appreciably with the π bands of graphite. The Fermi level intersects this band as well as the graphite π bands, giving rise to a complicated Fermi surface with several types of carriers. Depending on the type of volumetric partitioning, the charge transfer from Ba to graphite layers is determined to be between 0.7 and 1.0 electron per Ba atom. The calculated results are consistent with available transport and optical measurements.     

The N4 molecule has an open-chain triplet C2h structure

The lowest-energy N₄ is computed ab initio to be the planar C_2h(³B_u) open-chain structure 13 . The open-chain N₄ singlet-state structures dissociate on geometry optimization. The tetraazatetrahedrane T_d structure 1 and the tetrazete D_2h structure 2 are minima at MP 2/6-31G *. However, both are higher in energy than 13 (24.1 and 21.2 Kcal/mol [UQCISD ) (T )(full)/6-311+G *//MP 2/6-31G * + ZPE (MP 2/6-31G )*, respectively]. The energy of 13 is 157.5 kcal/mol higher than that of two N₂(¹∑ molecules [UQCISD (T )(Full)/6-311+G *//MP 2/6-31G *] © 1993 John Wiley & Sons, Inc.     

Spatial extent of the singlet and triplet excitons in luminescent angular-shaped transition-metal diynes and polyynes comprising non-pi-conjugated group 16 main group elements

A novel approach based on conjugation interruption has been developed and is presented for a series of luminescent and thermally stable chalcogen-bridged platinum(II) polyyne polymers trans-[{-Pt(PBu3)2C[triple bond]C(C6H4)E(C6H4)C[triple bond]C-}n] (E = O, S, SO, SO2). Particular attention was focused on the photophysical properties of these Group 10 polymetallaynes and comparison was made to their binuclear model complexes trans-[Pt(Ph)(PEt3)2C[triple bond]C(C6H4)E(C6H4)C[triple bond]CPt(Ph)(PEt3)2] and their closest Group 11 gold(I) and Group 12 mercury(II) neighbours, [MC[triple bond]C(C6H4)E(C6H4)C[triple bond]CM] (M = Au(PPh3), HgMe; E = O, S, SO, SO2). The regiochemical structures of these angular-shaped molecules were studied by NMR spectroscopy and single-crystal X-ray structural analyses. Upon photoexcitation, each one has an intense purple-blue fluorescence emission near 400 nm in dilute fluid solutions at room temperature. Harvesting of the organic triplet emissions harnessed through the strong heavy-atom effects of Group 10-12 transition metals was studied in detail. These metal-containing aryleneethynylenes spaced by chalcogen units were found to have large optical gaps and high-energy triplet states. The influence of metal- and chalcogen-based conjugation interrupters on the intersystem crossing rate and on the spatial extent of the lowest singlet and triplet excitons was fully elucidated. We discuss and compare the phosphorescence spectra of these transition-metal diynes and polyynes in terms of the nature of the metal centre, conjugated chain length and Group 16 spacer unit. Our work here indicates that high-energy triplet states in these materials intrinsically give rise to very efficient phosphorescence with fast radiative decays and one could readily observe room-temperature phosphorescence for the platinum polyynes.     

Enhanced photogeneration of triplet excitons in an oligothiophene-fullerene blend.

Photoinduced and transient absorption spectroscopy is used to study triplet exciton dynamics in thin films of a new thiophene-based oligomer (DCV3T) and blends of DCV3T and fullerene C60. We find enhanced DCV3T triplet exciton generation in the blend layer, which is explained as an excitonic ping-pong effect: singlet energy transfer from DCV3T to C60, followed by immediate intersystem crossing to C60, and triplet exciton back-transfer. Estimations of the rate constants involved show that the ping-pong effect has an overall efficiency close to unity. The singlet-singlet energy transfer from DCV3T to C60 is demonstrated by efficient quenching of DCV3T luminescence in the blend, leading to sensitized emission of C60. We discuss a promising new concept of solar cells with an enlarged active-layer thickness based on potentially long-ranged triplet exciton diffusion in combination with efficient intersystem crossing.     

Interaction of triplet excitons with charge carriers in crystalline anthracene

The influence of a magnetic field on photo-enhanced hole and electron injected space charge limited currents in anthracene has shown the current enhancement is predominantly due to triplet-trapped charge carrier interactions. The observed current enhancement is too large to be produced by the production of one detrapped carrier for each annihilated triplet exciton. It is suggested that on detrapping the free carriers are in a quartet state, in which they gain energy from the applied field and then detrap further carriers themselves by scattering processes.     

Hole-induced quenching of triplet and singlet excitons in conjugated polymers

Quantitative information on the mechanisms and rates of hole (radical cation)-induced quenching of triplet and singlet excitons in the conjugated polymer poly[2-methoxy-5-(2'-ethylhexyloxy)-p-phenylene vinylene] has been acquired by a new technique, fluorescence-voltage time-resolved single molecule spectroscopy (FV-TR-SMS). FV-TR-SMS measures the fluorescence intensity of a single conjugated polymer molecule that is embedded in a capacitor-like device while simultaneously modulating the bias on the device and the irradiation intensity. The results demonstrate that triplet excitons are efficiently quenched by holes in conjugated polymers for hole densities >10(16) charges/cm(3), while singlet excitons are quenched with a much lower efficiency. Detailed kinetic analysis shows that the greater efficiency for quenching of triplets by holes (compared to that for singlets) is due to a >10(6) times longer exciton lifetime for triplets. In fact, the results suggest that while singlet quenching is less efficient due to a much shorter singlet lifetime, the rate constant for the quenching of singlets by holes actually exceeds that for triplets by several orders of magnitude.     

Spin—lattice relaxation of linear triplet excitons in 1,4 dibromonaphthalene

We report measurements on spin—lattice relaxation (SLR) of linear triplet excitons in 1,4 dibromonaphthalene (1,4 DBN) single crystals at liquid helium temperatures and at room temperature. SLR was found to be temperature dependent but isotropic with respect to the external magnetic field.     

Temperature dependence of ESR lineshapes of triplet excitons in molecular pairs

The ESR lineshape of triplet excitons moving between two differently oriented molecules of a pair is calculated. Our model hamiltonian contains the electronic interaction matrix element for the coherent exciton transport, the Zeeman energy of the triplet spin in an external magnetic field, the fine structure of the differently oriented molecules, the phonons in the crystal which are described as a heat bath, and the microscopic interaction between excitons and phonons. For the naphthalene pair the lineshapes are discussed with respect to the temperature and a parameter characterizing the strength of the interaction between excitons and photons.     

Delayed-fluorescence ODMR and EPR studies of triplet excitons in charge-transfer molecular crystals

Triplet excitons in electron donor—acceptor charge-transfer (CT) molecular crystals are generated through the intersystem crossing process by excitation in the CT visible band and give rise to delayed fluorescence. Delayed-fluorescence optically detected magnetic resonance (DF ODMR) in magnetic field is analyzed in terms of microwave-induced transitions between energy levels of either the isolated triplet excitons or the annihilating triplet exciton pair. The spin polarization of the triplet excitons plays an important role in the described phenomena. A comparison between DF ODMR and EPR spectra of the anthracene—tetracyanobenzene and biphenyl—tetracyanobenzene systems is presented. In the former case the microwave transitions occurring between free exciton sublevels are predominantly responsible of the DF ODMR signal, whereas the transitions between energy levels of the exciton pair are the most important for biphenyl—TCNB.     

Spin-lattice relaxation of linear triplet excitons in tetrachlorobenzene at high magnetic fields

Spin-lattice relaxation of linear triplet excitons in 1,2,4,5-tetrachlorobenzene has been studied by an optical method at high magnetic fields B and at low crystal temperature. We find the interesting result that the field dependence of the relaxation rate constants for the direct processes cannot be described by a simple B³ law. The experimental relaxation rate for the Δm = 2 transition increases as B², and for the Δm = 1 transition as B^2,6.     

The source of excess linewidth in EPR of triplet excitons in molecular crystals

It is shown that the EPR linewidth spectrum of triplet excitons in molecular crystals can be severely distorted by weak orientational disorder. The demonstration employs a one-parameter correction procedure based on the assumption that the angular dependence of excess width is directly proportional to the angular gradient of the resonant field. Application to the discrepant data of Haarer and Wolf brings them into agreement with theory and with more recent experiments. A phenomenological model of the disorder is used to interpret the distortion parameter. These results suggest the potential value of exciton EPR as a probe of structural imperfections in molecular crystals.     

Mutual annihilation of triplet excitons in a nearly one-dimensional system: 1,4-dibromonaphthalene

The analysis of the variation with incident flux of the time dependence of the delayed fluorescence in conjunction with the determination of the absolute ground state-first excited triplet absorption coefficients at room temperature, yields the value of γ_tot = (5.5 ± 2.0) × 10^?12 cm³ s^?1, for the total triplet-triplet annihilation rate constant in 1,4-dibromonaphthalene crystals. The one-dimensional mutual annihilation rate constant for the triplet exciton motion restricted to linear chains along the crystal c axis is γ¹_tot = (1.0 ± 0.4) × 10³ cm s^?1. The results are discussed in terms of recent theories of mutual annihilation of triplets in one-dimensional systems.     

EPR study of spin polarization of charge transfer triplet excitons in anthracene-tetracyanobenzene single crystals

The population rates of the sublevels of triplet excitons in anthracene-1,2,45-tetracyanobenzene are determined from the angular dependence of the polarization of EPR spectra. Their values are closely related to those of the acceptot molecular Anomalous tnintensities of the polarized lines are attributed to a cross-relaxation process involving a triplet trap.     

The dynamic properties of triplet excitons in p-dichlorobenzene. A study by electron-spin-echo spectroscopy

The time evolution of the X-trap population in p-dichlorobenzene, following flash excitation into the exciton (T₀ ← S₀) 0-0 absorption, is explained by the combined effect of spin-lattice relaxation in, and trapping of, the exciton. The fast SLR is understood as arising from a fast inter-stack hopping.     

Delayed fluorescence in a pyrene-doped naphthalene crystal: homofusion and heterofusion of triplet excitons

Prompt and delayed emissions from a naphthalene crystal doped with pyrene have been investigated in the temperature range 77–300 K. It is shown that delayed fluorescence (DF) in this crystal originates from heterofusion and homofusion of two different types of trap triplets at low temperature (T< 130 K) and from homofusion of pyrene triplets at high temperature (T >200 K). Pyrene concentration effects on DF suggest that free triplet excitons are trapped more efficiently at monomeric pyrene sites than at nascent excimeric pyrene sites.     

Productive harvesting of triplet excitons in anthracene-based emitters toward high-performance deep-blue nondoped organic light-emitting diodes

Developing efficient deep-blue non-doped organic light-emitting diodes (OLEDs) is of great significance in practical applications. Here, two highly efficient asymmetric anthracene-based fluorescent emitters, 1-phenyl-2-(4-(10-(4-(2-phenyl-1H-phenanthro[9,10-d]imidazole-1-yl)phenyl)anthracen-9-yl)phenyl)-1H-phenanthro [9,10-d]imidazole (PPI-An-NPPI) and 1-phenyl-2-(4-(10-(4-(2,4,5-triphenyl-1H-imidazole-1-yl)phenyl) anthracen-9-yl)phenyl)-1H-phenanthro[9,10-d]imidazole (PPI-An-NPIM), have been designed and synthesized by introducing large steric hindrance imidazole moieties to regulate molecular excited states and photophysical properties. Experimental data show that they have high photoluminescence efficiencies, good thermal stabilities, and suitable energy levels for carrier injection. Theoretical calculations present that their high-lying excited states exhibit dominant locally excited-state characteristics with enhancing oscillator strength compared with anthracene core. The calculated transition dipole moments data show that two molecules are preferentially oriented along the horizontal direction. In addition, some hot exciton mechanism-like channels are also observed and confirmed, which are beneficial for the productive triplet-singlet exciton conversion. The non-doped OLED using PPI-An-NPPI as the emitting layer achieves a maximum external quantum efficiency (EQE_max) of 7.75% and Commission Internationale de L’Eclairage (CIE) coordinates of (0.15, 0.11), whereas PPI-An-NPIM gives a better color purity of CIE (0.14, 10) with an EQE_max of 7.48%. Moreover, all devices exhibit an insignificant efficiency roll-off at high luminescence and still yield an EQE of 7.61% and 7.14% at 1,000 cd/m². This work provides an interesting insight into developing efficient deep-blue fluorescent emitters for high-performance non-doped OLEDs.     

Benzyltripropylammonium bromide: a structure in polar space group P42bc

Crystals of the title compound, C₁₆H₂₈N⁺·Br⁻, were grown from solution in a mixture of acetone and propan‐2‐ol by slow evaporation. The structure was solved in the polar space group P4₂bc with five moieties in the asymmetric unit, namely two benzyl­tri­propyl­ammonium cations in general positions, and two Br⁻ anions in special Wyckoff positions (4a2.. and 4b2..) and one in a general position. The structure consists of two kinds of molecular columns parallel to c , built of cations connected through C—H⋯π hydrogen bonds and stabilized by weak C—H⋯Br interactions.     

Generation and decay dynamics of triplet excitons in Alq3 thin films under high-density excitation conditions

We studied the generation and decay dynamics of triplet excitons in tris-(8-hydroxyquinoline) aluminum (Alq3) thin films by using transient absorption spectroscopy. Absorption spectra of both singlet and triplet excitons in the film were identified by comparison with transient absorption spectra of the ligand molecule (8-hydroxyquinoline) itself and the excited triplet state in solution previously reported. By measuring the excitation light intensity dependence of the absorption, we found that exciton annihilation dominated under high-density excitation conditions. Annihilation rate constants were estimated to be gammaSS = (6 +/- 3) x 10(-11) cm3 s(-1) for single excitons and gammaTT = (4 +/- 2) x 10(-13) cm3 s(-1) for triplet excitons. From detailed analysis of the light intensity dependence of the quantum yield of triplet excitons under high-density conditions, triplet excitons were mainly generated through fission from highly excited singlet states populated by singlet-singlet exciton annihilation. We estimated that 30% of the highly excited states underwent fission.