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Tryptophan phosphorescence as a monitor of protein conformation in molecular films.

This report enquires on the potentiality of Trp phosphorescence for probing the conformational state of proteins deposited on solid dry films. Thin, amorphous protein films were fabricated with Apoazurin, alcohol dehydrogenase, glyceraldehyde-3-phosphate dehydrogenase and glutamate dehydrogenase the protein being incorporated into a DEAE-dextran matrix and deposited on quartz slides. The results, obtained with appositely constructed instrumentation, demonstrate that thanks to the low background radiation associated with long-lived, delayed emission phosphorescence can be readily detected down to single protein layer matrices and that both spectrum and lifetime are important indicators of the integrity of the protein globular fold. In fact, denaturation of the proteins by guanidinium hydrochloride or heat treatment points out that disruption of the native fold leads to a red shift and broadening of the spectrum with loss of vibronic structure, accompanied to considerably shorter-lived and more heterogeneous decay kinetics. It is also shown that the sensitivity of the phosphorescence lifetime towards the detection of altered, looser conformations of the polypeptide are remarkably enhanced on partial hydration of the sample.

Alcohol Dehydrogenase↗

Inert phosphorescent nanospheres as markers for optical assays.

A simple encapsulation technique is presented to produce highly phosphorescent, inert nanospheres that are suitable luminescent markers. It is based on the coprecipitation of phosphorescent ruthenium(II)-tris(polypyridyl) complexes and polyacrylonitrile (PAN) derivatives from a solution in N,N-dimethylformamide. The beads precipitate in the form of very small aggregates of spherical shape and a typical particle diameter of less than 50 nm. This process allows the encapsulation of phosphorescent and fluorescent dyes in an individual nanosphere provided that they are sufficiently lipophilic. Quenching by oxygen is negligible due to the use of PAN. The nanospheres were characterized with respect to their spectral properties (quantum yields of the luminophores, brightness, luminescence decay time), stability in aqueous buffered suspensions, and in terms of size, shape, and surface charge of the particles, as well as storage stability, quenching by oxygen, and dye leaching.

Acrylic Resins↗

Sensitive monitoring of the dynamics of a membrane-bound transport protein by tryptophan phosphorescence spectroscopy.

This paper presents a tryptophan phosphorescence spectroscopy study on the membrane-bound mannitol transporter, EII(mtl), from E. coli. The protein contains four tryptophans at positions 30, 42, 109, and 117. Phosphorescence decays in buffer at 1 degrees C revealed large variations of the triplet lifetimes of the wild-type protein and four single-tryptophan-containing mutants. They ranged from <70 microseconds for the tryptophan at position 109 to 55 ms for the residue at position 30, attesting to widely different flexibilities of the tryptophan microenvironments. The decay of all tryptophans is multiexponential, reflecting multiple stable conformations of the protein. Both mannitol binding and enzyme phosphorylation had large effects on the triplet lifetimes. Mannitol binding induces a more ordered structure near the mannitol binding site, and the decay becomes significantly more homogeneous. In contrast, enzyme phosphorylation induces a large relaxation of the protein structure at the reporter sites. The implications of these structural changes on the coupling mechanism between the transport and the phosphorylation activity of EII(mtl) are discussed. Taken as a whole, our data show that tryptophan phosphorescence spectroscopy is a very sensitive technique to explore conformational dynamics in membrane proteins.

Binding Sites↗

Protein and lipid rotational dynamics in cardiac and skeletal sarcoplasmic reticulum detected by EPR and phosphorescence anisotropy.

We have used time-resolved phosphorescence anisotropy and electron paramagnetic resonance (EPR) spectroscopy to detect the rotational dynamics of the Ca-ATPase and its associated lipids in dog cardiac sarcoplasmic reticulum (DCSR), in comparison with rabbit skeletal SR (RSSR), in order to obtain insight into the physical bases for different activities and regulation in the two systems. Protein rotational motions were studied with time-resolved phosphorescence anisotropy (TPA) of erythrosin isothiocyanate (ERITC) and saturation-transfer EPR (ST-EPR) of a maleimide spin-label (MSL). Both labels were attached selectively and rigidly to the Ca-ATPase. Lipid rotational motions were studied with conventional EPR of stearic acid spin-labels. As in previous studies on RSSR, the phosphorescence anisotropy decays of both preparations at 4 degrees C were multiexponential, due to the presence of different oligomeric species. The rotational correlation times for the different rotating species were similar for the two preparations, but the total decay amplitude was substantially less for cardiac SR, indicating that more of the Ca-ATPase molecules are in large aggregates in DCSR. ST-EPR spectra confirmed that the Ca-ATPase is less rotationally mobile in DCSR than in RSSR. Lipid probe mobility and fatty acid composition were very similar in the two preparations, indicating that the large differences observed in protein mobility are not due to differences in lipid fluidity. We conclude that the higher restriction in protein mobility observed by both ST-EPR and TPA is due to more extensive protein-protein interactions in DCSR than in RSSR.

Animals↗

Penetration of analogues of H2O and CO2 in proteins studied by room temperature phosphorescence of tryptophan.

The influence of the protein matrix on the reactivity of external molecules with a species buried within the protein interior is considered in two general ways: (1) there may be structural fluctuations that allow for the diffusive penetration of the small molecules and/or (2) the external molecule may react over a distance. As a means to study the protein matrix, a reactive species within the protein can be formed by exciting tryptophan to the triplet state, and then the reaction of the triplet-state molecule with an external molecule can be monitored by a decrease in phosphorescence. In this work, the quenching ability (i.e., reactivity) was examined for H2S, CS2, and NO2- acting on tryptophan phosphorescence in parvalbumin, azurin, horse liver alcohol dehydrogenase, and alkaline phosphatase. A comparison of charged versus uncharged quenchers (H2S vs SH- and CS2 vs NO2-) reveals that the uncharged molecules are much more effective than charged species in quenching the phosphorescence of fully buried tryptophan, whereas the quenching for exposed tryptophan is relatively independent of the charge of the quencher. This is consistent with the view that uncharged triatomic molecules can penetrate the protein matrix to some extent. The energies of activation of the quenching reaction are low for the charged quenchers and higher for the uncharged CS2. A model is presented in which the quenchability of a buried tryptophan is inversely related to the distance from the surface when diffusion through the protein is the rate-limiting step.(ABSTRACT TRUNCATED AT 250 WORDS)

Carbon Dioxide↗

Quenching of tryptophan phosphorescence in Escherichia coli alkaline phosphatase by long-range transfer mechanisms to external agents in the rapid-diffusion limit.

Quenching of the room-temperature phosphorescence of Escherichia coli alkaline phosphatase by several freely diffusing molecules was studied, each of whose absorption spectrum overlaps the long-lived emission of this protein and which therefore can quench the excited triplet state by diffusion-enhanced Förster energy transfer. The presence of additional nonresonance transfer mechanisms was also detected, from a lack of linear dependence of quenching rate on spectral overlap. The quenching agents used were the dye molecules methyl red, methyl orange, and 2-[(4-hydroxyphenyl)azo]benzoic acid, as well as the embedded heme groups of myoglobin, metmyoglobin, and the reduced and oxidized forms of cytochrome c. Quenching was found to be greatly diminished upon reduction of each acceptor, indicating that electron transfer occurs efficiently from the excited tryptophan to the oxidized form of the acceptors. The elimination of this electron transfer in the reduced form affords the opportunity to separately measure the Förster transfer rates for the heme proteins. When the transfer rate constant thus measured for myoglobin is applied to a model where both donor and acceptor proteins are taken to be spherical with both tryptophan and the heme group placed off center (a model whose quenching rate equation is newly presented here), the depth of the phosphorescent tryptophan beneath the surface of alkaline phosphatase is found to be 16 A. This value is close to the depth of tryptophan 109 (which is known to be the phosphorescent residue in alkaline phosphatase), showing that with properly chosen probes this technique is indeed valuable for distance determinations in protein structure studies.(ABSTRACT TRUNCATED AT 250 WORDS)

Alkaline Phosphatase↗

Quenching of room temperature protein phosphorescence by added small molecules.

A number of molecular agents that can efficiently quench the room temperature phosphorescence of tryptophan were identified, and their ability to quench the phosphorescence lifetime of tryptophan in nine proteins was examined. For all quenchers, the quenching efficiency generally follows the same sequence, namely, N-acetyltryptophanamide (NATA) greater than parvalbumin approximately lactoglobulin approximately ribonuclease T1 greater than liver alcohol dehydrogenase greater than aldolase greater than Pronase approximately edestin greater than azurin greater than alkaline phosphatase. Quenching rate constants for O2 and CO are relatively insensitive to protein differences, while H2S and CS2 are somewhat more sensitive. These small molecule agents appear to act by penetrating into the proteins. However, penetration to truly buried tryptophans is less favorable than previously suggested; in five proteins studied, quenching efficiency by O2 is 20-1000 times lower than for NATA, and up to 10(5) lower for H2S and CS2. Larger and more polar quenchers--including organic thiols, conjugated ketones and amides, and anionic species--were also studied. The efficiency of these quenchers does not correlate with quencher size or polarity, the quenching reaction has low energy of activation, and quenching rates are insensitive to solvent viscosity. These results indicate that the larger quenchers do not approach the buried tryptophans by penetrating into the proteins, even on the long phosphorescence time scale, and are also inconsistent with a mechanism in which quencher encounter with the tryptophan occurs in free solution, as in a protein-opening reaction. The results obtained suggest that the quenching process involves a long-range radiationless transfer.(ABSTRACT TRUNCATED AT 250 WORDS)

Luminescent Measurements↗

Ionic strength dependent conformational changes of transfer ribonucleic acid studied by circular polarization of phosphorescence.

The circularly polarized phosphorescence emitted by the 4-thiouridine base was measured for bulk Escherichia coli tRNA, E. coli tRNA1Val, E. coli tRNAfMet, and E. coli tRNAPhe as a function of ionic strength in the presence of 1 mM Mg2+. The emission anisotropy factor, gem, was found to be dependent on the degree of local stacking in the vicinity of the chromophore. For bulk tRNA and tRNAfMet a marked similarity was observed between the behavior of gem and the translational diffusion coefficient D020,w [Pots, R. O., Wang, C. C., Fritzinger, D. C., Ford, N. C. & Fournier, M. J. (1979) in Cold Spring Harbor Monograph Series (Schimmel, P. R; Söll, D., & Abelson, J. N., Eds.) Part A, p 207, Cold Spring Harbor Laboratory, Cold Spring Harbor, NY]. This was interpreted to mean that a relationship exists between the local stacking around the 4-thiouridine chromophore and the overall general similarity of behavior was observed, each species of tRNA examined exhibited a distinctive dependence of conformation on salt concentration. tRNAPhe was found to be a particular exception in the low-salt region (less than 50 mM). The value of the phosphorescence anisotropy factor was found to be remarkably larger (about 50-fold). Thus minor conformational changes in the tRNA molecule are more readily detected by circular polarization of phosphorescence than by circular dichroism

Escherichia coli↗

Characterization of the tryptophan residues of Escherechia coli alkaline phosphatase by phosphorescence and optically detected magnetic resonance spectroscopy.

The phosphorescence and zero field optically detected magnetic resonance (ODMR) of the tryptophan (Trp) residues of alkaline phosphatase from Escherechia coli are examined. Each Trp is resolved optically and identified with the aid of the W220Y mutant and the terbium complex of the apoenzyme. Trp(109), known from earlier work to be the source of room-temperature phosphorescence (RTP), emits a highly resolved low-temperature phosphorescence (LTP) spectrum and has the narrowest ODMR bands observed thus far from any protein site, revealing a uniquely homogeneous local environment. The decay kinetics of Trp(109) at 1.2 K reveals that the major triplet population (70%) undergoes inefficient crystallike spin-lattice relaxation by direct interaction with lattice phonons, the remainder being relaxed efficiently by local disorder modes. The latter population is smaller than is typical for protein sites, suggesting an unusual degree of local rigidity and order consistent with the long-lived RTP. Trp(220) emits a broader LTP spectrum originating to the blue of Trp(109). It has typically broad ODMR bands consistent with local heterogeneity. The LTP of Trp(268) has an ill-defined origin blue shifted relative to Trp(220) and ODMR frequencies consistent with a greater degree of solvent exposure. Trp(268) has noticeable dispersion of its decay kinetics, consistent with quenching at the triplet level by a nearby disulfide residue.

Alkaline Phosphatase↗

Phosphorescence and optically detected magnetic resonance of 4',6-diamidino-2-phenylindole (DAPI) and its complexes with [d(CGACGTCG)]2 and [d(GGCCAATTGG)]2.

Phosphorescence and optical detection of magnetic resonance (ODMR) is used to study the excited triplet state of 4',6-diamidino-2-phenyl indole (DAPI) and its complexes with the oligonucleotides [d(CGACGTCG)](2) and [d(GGCCAATTGG)](2), where binding occurs by intercalation between GC base pairs and by minor groove insertion, respectively. Weaker binding of DAPI to phosphate is also detected, and the triplet state of this complex is characterized. Intercalation with [d(CGACGTCG)](2) produces a phosphorescence redshift, while groove binding with [d(GGCCAATTGG)](2) leads to a blueshift. Both binding modes give rise to a small decrease in the zero-field splitting (zfs) of the DAPI triplet state. The largest redshift and zfs decrease are found for the phosphate complex. The phosphorescence lifetimes are shorter by an order of magnitude than that of indole or tryptophan as expected for the lower triplet state energy, E(00), of DAPI. The lifetimes agree well with a correlation with E(00) introduced by Siebrand [Siebrand, W. (1966) J. Chem. Phys. 44, 4055-4057] except for the [d(GGCCAATTGG)](2) minor groove complex with a lifetime that is about 20% too long. The longer lifetime is attributed to distortion of the amidino groups in this complex, resulting in less efficient intersystem crossing.

Deoxyribonucleotides↗

Tryptophan phosphorescence study of enzyme flexibility and unfolding in laboratory-evolved thermostable esterases.

Directed evolution of p-nitrobenzyl esterase (pNB E) has yielded eight generations of increasingly thermostable variants. The most stable esterase, 8G8, has 13 amino acid substitutions, a melting temperature 17 degrees C higher than the wild-type enzyme, and increased hydrolytic activity toward p-nitrophenyl acetate (pNPA), the substrate used for evolution, at all temperatures. Room-temperature activities of the evolved thermostable variants range from 3.5 times greater to 4.0 times less than wild type. The relationships between enzyme stability, catalytic activity, and flexibility for the esterases were investigated using tryptophan phosphorescence. We observed no correlation between catalytic activity and enzyme flexibility in the vicinity of the tryptophan (Trp) residues. Increases in stability, however, are often accompanied by decreases in flexibility, as measured by Trp phosphorescence. Phosphorescence data also suggest that the N- and C-terminal regions of pNB E unfold independently. The N-terminal region appears more thermolabile, yet most of the thermostabilizing mutations are located in the C-terminal region. Mutational studies show that the effects of the N-terminal mutations depend on one or more mutations in the C-terminal region. Thus, the pNB E mutants are stabilized by long-range, cooperative interactions between distant parts of the enzyme.

Directed Molecular Evolution↗

Room temperature phosphorescence from ruthenium(II) complexes bearing conjugated pyrenylethynylene subunits.

We describe the synthesis, electrochemistry, and photophysical properties of several Ru(II) complexes bearing different numbers of pyrenylethynylene substituents in either the 5- or 5,5'-positions of 2,2'-bipyridine, along with the appropriate Ru(II) model complexes bearing either bromo- or ethynyltoluene functionalities. In addition, we prepared and studied the photophysical behavior of the diimine ligands 5-pyrenylethynylene-2,2'-bipyridine and 5,5'-dipyrenylethynylene-2,2'-bipyridine. Static and dynamic absorption and luminescence measurements reveal the nature of the lowest excited states in each molecule. All model Ru(II) complexes are photoluminescent at room temperature and exhibit excited-state behavior consistent with metal-to-ligand charge transfer (MLCT) characteristics. In the three Ru(II) molecules bearing multiple pyrenylethynylene substituents, there is clear evidence that the lowest excited state is triplet intraligand (3IL)-based, yielding long-lived room temperature phosphorescence in the red and near IR. This phosphorescence emanates from either 5-pyrenylethynylene-2,2'-bipyridine or 5,5'-dipyrenylethynylene-2,2'-bipyridine, depending upon the composition of the coordination compound. In the former case, the excited-state absorption difference spectra that were measured for the free ligand are easily superimposed with those obtained for the metal complexes coordinated to either one or two of these species. The latter instance is slightly complicated since coordination of the 5,5'-ligand to the Ru(II) center planarizes the diimine structure, leading to an extended conjugation on the long axis with a concomitant red shift of the singlet pi-pi absorption transitions and the observed room temperature phosphorescence. As a result, transient absorption measurements obtained using free 5,5'-dipyrenylethynylene-2,2'-bipyridine show a marked blue shift relative to its Ru(II) complex, and this extended pi-conjugation effect was confirmed by coordinating this ligand to Zn(II) at room temperature. In essence, all three pyrenylethynylene-containing Ru(II) complexes are unique in this genre of chromophores since the lowest excited state is 3IL-based at room temperature and at 77 K, and there is no compelling evidence of interacting or equilibrated excited states.

Journal Article↗

Theoretical studies of phosphorescence spectra of tris(2,2'-bipyridine) transition metal compounds.

Phosphorescence spectra of tris(2,2'-bipyridine) metal compounds, [M(bpy)3]n+, where M = Zn(II), Ru(II), Os(II), Rh(III), and Ir(III), were calculated using a harmonic oscillator approximation of adiabatic potential surfaces obtained by density functional theory (DFT). Using the Huang-Rhys (S) factors calculated by theoretical Franck-Condon analysis of T1 and S0 geometries, we successfully reproduced the emission spectra observed under various conditions by nonempirical calculations. The simulations of well-structured spectra of the Zn(II), Rh(III), and Ir(III) compounds confirmed that the emission originated from localized ligand-centered excited states with considerably distorted geometries of C2 symmetry. The spectrum simulation revealed that the phosphorescence state of [Ru(bpy)3]2+ was localized 3MLCT both in a solution and a glass matrix. Furthermore, a highly resolved phosphorescence spectrum observed for [Ru(bpy)3]2+ doped in a [Zn(bpy)3](ClO4)2 crystal was reproduced well using the geometry of the localized 3MLCT by assuming mode-specific broadening of low-frequency intramolecular vibrational modes. The deuterium effects of the electronic origins of the doped crystal observed by Riesen et al. were in excellent agreement with those predicted for the localized 3MLCT. However, the calculated satellite structures of the localized 3MLCT involving bpy-h8 in [Ru(bpy-h8)(3-x)(bpy-d8)x]2+ (x = 1,2) exhibited only the bpy-h8 vibrational modes, inconsistent with the simultaneous appearance of both bpy-h8 and bpy-h8 modes in the observed spectra. A simulation on the basis of the geometry of the delocalized 3MLCT was in reasonable agreement with an unresolved spectrum observed for a neat crystal of [Ru(bpy)3](PF6)2, which is inconsistent with the assignments of localized 3MLCT on the basis of the electronic origins. The inconsistency of the assignment on the basis of the adiabatic model is discussed in terms of vibronic coupling between the localized 3MLCT states. The 3MLCT state in [Os(bpy)3]2+ seems to vary with the environment: a fully localized 3MLCT in a solution, partially localized in a glass matrix, and delocalized in PF6 salts.

Journal Article↗

The triplet-state lifetime of indole in aqueous and viscous environments: significance to the interpretation of room temperature phosphorescence in proteins.

The interpretation of room temperature phosphorescence studies of proteins requires an understanding of the mechanisms governing the tryptophan triplet-state lifetimes of residues fully exposed to solvent and those deeply buried in the hydrophobic core of proteins. Since solvents exposed tryptophans are expected to behave similarly to indole free in solution, it is important to have an accurate measure of the triplet state lifetime of indole in aqueous solution. Using photon counting techniques and low optical fluence (J/cm(2)), we observed the triplet-state lifetime of aqueous, deoxygenated indole and several indole derivatives to be approximately 40 micros, closely matching the previous reports by Bent and Hayon based on flash photolysis (12 micros; Bent, D. V.; Hayon, E. J. Am. Chem. Soc. 1975, 97, 2612-2619) but much shorter than the 1.2 ms lifetime observed more recently (Strambini, G. B.; Gonnelli, M. J. Am. Chem. Soc. 1995, 117, 7646-7651). However, we have now been able to reproduce the long lifetime reported by the latter workers for aqueous indole solutions and show that it likely arises from geminate recombination of the indole radical cation and solvated electron, a conclusion based on studies of the indole radical cation in water (Bent and Hayon, 1975). The evidence for this comes from a fast rise in the phosphorescence emission and measurements of a corresponding enhanced quantum yield in unbuffered solutions. This species can be readily quenched, and the corresponding fast rise disappears, leaving a monoexponential 40 micros decay, which we argue is the true indole triplet lifetime. The work is put in the context of room temperature phosphorescence studies of proteins.

Indoles↗

Sonochemical production of fluorescent and phosphorescent latex particles.

A novel method for producing nanosized polymer latex particles doped with fluorescent and phosphorescent solutes is described. Methyl methacrylate monomer (10 wt %) containing either pyrene, 4-dicyanomethylene-2-methyl-6-(p-dimethylaminostyryl)-4H-pyran (DMDP), or 1-bromonaphthalene was ultrasonically dispersed in water and simultaneously polymerized to produce approximately 60 nm diameter latex particles. A fluorescence spectroscopic examination of the latex dispersion containing either pyrene or DMDP showed that the solutes were not covalently bound to the polymer and that they were embedded in a highly viscous environment possessing a low polarity (dielectric constant on the order of 2). The fluorescence lifetime of the pyrene in the core of the poly(MMA) latex was found to be 520 ns, irrespective of the oxygen concentration in the dispersion. Room-temperature phosphorescence was observed from 1-bromonaphthalene, with a lifetime of 2.0 ms in an argon atmosphere. In the presence of air, phosphorescence was still observable although with a partially reduced emission intensity.

Journal Article↗

Phosphorescence quenching by conjugated polymers.

Energy transfer between phosphors and conjugated polymers was investigated using a fluorene trimer (F3) as a model conjugated material. The phosphors studied were bis-cyclometalated iridium complexes (FP, PPY, BT, PQ, and BTP), with triplet energies of 2.6, 2.4, 2.2, 2.1, and 2.0 eV, respectively (based on phosphorescence spectra). Stern-Volmer analysis of luminescent quenching shows that energy transfer from either FP or PPY to F3 is an exothermic process with Stern-Volmer quenching constants (kqSV) of near 109 M-1 s-1 while energy transfer from BT, PQ, and BTP is endothermic (kqSV = 107-106 M-1 s-1). On the the basis of above results, the triplet energy of F3 is estimated to be less than 2.3 eV (530 nm). This study suggests that conjugated polymers, which typically have lower T1 energies than F3, should also quench phosphorescent emission in thin films and organic light-emitting diodes (OLEDs) incorporating these and related phosphorescent dopants.

Journal Article↗

Homoleptic cyclometalated iridium complexes with highly efficient red phosphorescence and application to organic light-emitting diode.

Phosphorescence studies of a series of facial homoleptic cyclometalated iridium(III) complexes have been carried out. The complexes studied have the general structure Ir(III)(C-N)(3), where (C-N) is a monoanionic cyclometalating ligand: 2-(5-methylthiophen-2-yl)pyridinato, 2-(thiophen-2-yl)-5-trifluoromethylpyridinato, 2,5-di(thiophen-2-yl)pyridinato, 2,5-di(5-methylthiophen-2-yl)pyridinato, 2-(benzo[b]thiophen-2-yl)pyridinato, 2-(9,9-dimethyl-9H-fluoren-2-yl)pyridinato, 1-phenylisoquinolinato, 1-(thiophen-2-yl)isoquinolinato, or 1-(9,9-dimethyl-9H-fluoren-2-yl)isoquinolinato. Luminescence properties of all the complexes at 298 K in toluene are as follows: quantum yields of phosphorescence Phi(p) = 0.08-0.29, emission peaks lambda(max) = 558-652 nm, and emission lifetimes tau = 0.74-4.7 micros. Bathochromic shifts of the Ir(thpy)(3) family [the complexes with 2-(thiophen-2-yl)pyridine derivatives] are observed by introducing appropriate substituents, e.g., methyl, trifluoromethyl, or thiophen-2-yl. However, Phi(p) of the red emissive complexes (lambda(max) > 600 nm) becomes small, caused by a significant decrease of the radiative rate constant, k(r). In contrast, the complexes with the 1-arylisoquinoline ligands are found to have marked red shifts of lambda(max) and very high Phi(p) (0.19-0.26). These complexes are found to possess dominantly (3)MLCT (metal-to-ligand charge transfer) excited states and have k(r) values approximately 1 order of magnitude larger than those of the Ir(thpy)(3) family. An organic light-emitting diode (OLED) device that uses Ir(1-phenylisoquinolinato)(3) as a phosphorescent dopant produces very high efficiency (external quantum efficiency eta(ex) = 10.3% and power efficiency 8.0 lm/W at 100 cd/m(2)) and pure-red emission with 1931 CIE (Commission Internationale de L'Eclairage) chromaticity coordinates (x = 0.68, y = 0.32).

Journal Article↗

Polymorphic forms of a gold(I) arylacetylide complex with contrasting phosphorescent characteristics.

The spectroscopic properties and crystal structures of the gold(I) arylacetylide complexes [(R(3)P)Au(Ctbd1;CAr)] (R = Cy, Ar = 4-nitrophenyl, 1; 4-trifluoromethylphenyl, 2; pentafluorophenyl, 3; R = Ph, Ar = 4-nitrophenyl, 4) have been examined. The dipole-allowed and -forbidden transitions of 1 (4 in parentheses) at lambda(max) 340 (336) and ca. 485 (470) nm in CH(2)Cl(2) solution at 298 K are assigned to the singlet and triplet intraligand charge transfer (ILCT) transitions of the 4-nitrophenylacetylide moiety, whereas 2 (3 in parentheses) shows localized singlet and triplet acetylenic pipi transitions at lambda(max) 287 (276) and 426 nm, respectively. Two polymorphs of 1 with contrasting phosphorescent characteristics have been identified. At 298 K, the emissive form of 1, as well as 2-4, are highly phosphorescent with peak maximum at 504, 425, 521, and 495 nm, respectively; the other polymorph of 1 is nonemissive at 298 K but emission is detected at 77 K with peak maximum at 486 nm. Crystallographic studies reveal that the major differences between the emissive and nonemissive forms of 1 are the orientations of the molecular dipoles and the dihedral angles between neighboring 4-nitrophenyl moieties. Crystal 2 is isostructural to the nonemissive form of 1, but does not display polymorphism. The molecular planes of two neighboring lumophores are coplanar in the emissive form of 1, parallel in 4, and nearly perpendicular (78.6 degrees ) to each other in the nonemissive form of 1. Both the nature of the excited state and the dihedral angle between adjacent [Au(Ctbd1;CAr)] moieties determine the phosphorescent properties of these molecular crystals.

Journal Article↗