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At least 19 recordsLinked to original sources
PubMed1976

The study of the primary photoprocesses in photosystem I of chloroplasts. Recombination luminescence, chlorophyll triplet state and triplet-triplet annihilation.

The dependence of the delayed luminescence of Photosystem I on the state of the reaction centers has been studied. Light flash induces a charge separation in the centers: P-700-P-430 hv in equilibrium P-700+-P-430-. Dark recombination of charges is accompanied by the recombination luminescence with tau1/2 congruent to 20ms. If the centers are in the P-700-P-430- state or if P-430 is inactivated by heat, then flashing of Photosystem I generates the triplet state chlorophyll with tau1/2 congruent to 0.5 ms. The triplet state has been measured by the delayed fluorescence of chlorophyll at 20 degrees C and 77 degrees K and by the chlorophyll phosphorescence at 77 degrees K. The delayed fluorescence at 20 degrees C arises from the thermal activation of the triplet state up to the excited singlet level of chlorophyll and at 77 degrees K it is due to triplet-triplet annihilation. The quantum yield of the triplet formation, estimated by a comparison of the light saturation curves of delayed fluorescence at 20 degrees C and of P-700 photooxidation under the same experimental (optical) conditions, is approximately 0.9 of the P-700+ yield. Only one triplet of chlorophyll can be generated per P-700. Under heat inactivation of P-430 the triplet formation is not observed when P-700 is oxidized. It is assumed that the triplet-triplet annihilation at 77 degrees K is related with the strong interaction between the chlorophyll molecules in the pigment complex of Photosystem I. The possibility of a triplet participation in the primary processes of photosynthesis is discussed.

Chlorophyll↗
PubMed2005

Singlet-triplet and triplet-triplet interactions in conjugated polymer single molecules.

Single molecule fluorescence correlation spectroscopy has been used to investigate the photodynamics of isolated single multichromophoric polymer chains of the conjugated polymers MEH-PPV and F8BT on the microsecond to millisecond time scale. The experimental results (and associated kinetic modeling) demonstrate that (i) triplet exciton pairs undergo efficient triplet-triplet annihilation on the <<30 micros time scale, (ii) triplet-triplet annihilation is the dominant mechanism for triplet decay at incident excitation powers > or =50 W/cm(2), and (iii) singlet excitons are quenched by triplet excitons with an efficiency on the order of (1)/(2). The high efficiency of this latter process ensures that single molecule fluorescence spectroscopy can be effectively used to indirectly monitor triplet exciton population dynamics in conjugated polymers. Finally, correlation spectroscopy of MEH-PPV molecules in a multilayer device environment reveals that triplet excitons are efficiently quenched by hole polarons.

Journal Article↗
PubMed2003

Calculation of triplet-triplet energy transfer rates from emission and absorption spectra. The quenching of hemicarcerated triplet biacetyl by aromatic hydrocarbons.

The kinetics of triplet-triplet (T-T) energy transfer have been analysed with a view to linking theories of chemical reactions (involving the rupture and formation of bonds) with theories of processes, such as electron transfer or energy transfer, which preserve chemical bonding. As for the latter, our analysis does not support the claim that, of the two rival expressions for T-T energy transfer, both rooted in the golden rule, only one is applicable to electron transfer or T-T transfer. Though the two expressions do reflect different standpoints, the distinction is eroded by the assumption of a delta-function distribution for the vibrational spectrum. It is shown that theories of chemical reactions also furnish estimates of Franck-Condon factors; rates of chemical reactions and chemical processes are both related to the properties (strengths and lengths) of the reactive bonds, but differ in the mode of energy dissipation. The relationship between the rates of reactions and processes presents new possibilities for a unified view of chemical reactivity.

Journal Article↗
PubMed1999

Multifetal pregnancy reductions of triplets to twins: comparison with nonreduced triplets and twins.

OBJECTIVE: Multifetal pregnancy reduction has been shown to improve survival rates in high-order multifetal pregnancies (>/=4). There is, however, some controversy as to whether multifetal pregnancy reduction improves pregnancy outcomes of triplets reduced to twins. The purpose of this study was to evaluate this issue by comparing outcomes of triplet gestations undergoing reduction to twins with outcomes of nonreduced twin gestations and expectantly managed triplet gestations. STUDY DESIGN: The study included 143 triplet pregnancies that underwent reduction to twins over a 10-year period at a single center. These were compared with 12 nonreduced triplet pregnancies from the Wayne State University Perinatal Database and with 2 groups of twin pregnancies: 605 from the Wayne State University Perinatal Database and 207 from the Quest Diagnostics Database. RESULTS: The miscarriage rate for expectantly managed triplets was 25%, compared with 6.2% for triplets reduced to twins. This rate was similar to the rates for both groups of nonreduced twins: 5.8% (Quest) and 6.3% (Wayne State University). Severe prematurity occurred in 25% of nonreduced triplets compared with 4. 9% of twins after reduction. This rate was also similar to that of nonreduced twins: 7.7% (Quest) and 8.4% (Wayne State University). The mean gestational age at delivery for expectantly managed triplets (32.9 +/- 4.7 weeks) was significantly shorter than for triplets reduced to twins (35.6 +/- 3.1 weeks). By comparison, nonreduced twins had a mean gestational age at delivery of 35.8 +/- 3.9 weeks for Quest and 34.4 +/- 3.6 weeks for Wayne State University. Mean birth weights were significantly lower in expectantly managed triplets as compared with triplets undergoing reduction to twins (1636 +/- 645 g vs 2381 +/- 602 g, respectively). Nonreduced twins had a mean birth weight of 2254 +/- 653 g for Quest and 2123 +/- 634 g for Wayne State University. Pregnancy loss rates, mean length of gestation, and mean birth weight did not vary significantly between triplets who underwent reduction to twins and nonreduced twins. CONCLUSIONS: Reduction of triplets to twins significantly reduces the risk for prematurity and low birth weight and may also be associated with a reduction in overall pregnancy loss. This suggests that multifetal pregnancy reduction of triplets to twins is a medically justifiable procedure not only from an actuarial viewpoint but also from the ethical perspective of supporting patients' autonomy and respect for patients' individual circumstances.

Abortion, Spontaneous↗
PubMed1995

[Antenatal complications in triplet pregnancies and birth weights of triplets compared with those of twins].

A mailed questionnaire survey was conducted on 96 mothers of triplets to study antenatal complications in triplet pregnancies and birth weights of triplets, and compared to 122 controls recruited from mothers of twins. The following results were obtained. 1) Antenatal complications occurred in approximately 80% of both triplet and twin pregnancies. In the triplet pregnancies the incidence of toxemia of pregnancy and anemia was 25.0% and 47.9%, respectively. There was no significant difference in the incidence of antenatal complications, toxemia of pregnancy and anemia between triplet and twin pregnancies. On the other hand, the incidence of preterm labor and threatened miscarriage was higher in triplets (70.8% and 34.4% respectively) than in twin pregnancies (45.9% and 12.3% respectively). 2) The mean birth weight was 1831.7 g for each individual triplet and 5495.0 g for each triplet set. In triplets, 94.7% were low in birth weight (< 2500 g). 3) The antenatal complications of preterm labor and threatened miscarriage in triplet pregnancies have increased since 1990 in Japan. The frequency of toxemia of pregnancy and anemia did not particularly change significantly during the surveyed years. However, mean birth weight for each individual triplet showed a tendency to decrease from year to year (1978-1989, 1934.5 g; 1990-1991, 1900.3 g; 1992-1993, 1741.1 g).

Adult↗
PubMed2005

Time-dependent density-functional theory calculations of triplet-triplet absorption.

We present density-functional theory calculations of triplet-triplet absorption by three different approaches based on time-dependent density-functional theory (DFT): unrestricted DFT linear response, open-shell restricted DFT linear response applied to the triplet state, and quadratic response with triplet excitations applied to the ground state. Comparison is also made with corresponding results obtained by Hartree-Fock and multiconfiguration self-consistent-field response theory. Two main conclusions concerning triplet-triplet transitions are drawn in this study: First, the very good agreement between unrestricted and restricted DFT results indicates that spin contamination of the triplet state is not a serious problem when computing triplet-triplet spectra of common organic molecules. Second, DFT response calculations of triplet-triplet transitions can be affected by triplet instability problems, especially for the combination of DFT quadratic response with functionals containing fractional exact Hartree-Fock exchange.

Journal Article↗
PubMed2006

Base triplet nonisomorphism strongly influences DNA triplex conformation: effect of nonisomorphic G* GC and A* AT triplets and bending of DNA triplexes.

Structural understanding of DNA triplexes is grossly inadequate despite their efficacy as therapeutic agents. Lack of structural similarity (isomorphism) of base triplets that figure in different DNA triplexes brings in an added complexity. Recently, we have shown that the residual twist (Deltat degrees ) and the radial difference (Deltar A) adequately define base triplet nonisomorphism in structural terms and allow assessment of their role in conferring stability as well as sequence-dependent structural variations in DNA triplexes. To further corroborate these, molecular dynamics (MD) simulations are carried out on DNA triplexes comprising nonisomorphic G* GC and A* AT base triplets under different sequential contexts. Base triplet nonisomorphism between G* GC and A* AT triplets is dominated by Deltat degrees (9.8 degrees ), in view of small Deltar (0.2 A), and is in contrast to G* GC and T* AT triplets where both Deltat degrees (10.6 degrees ) and Deltar (1.1A) are prominent. Results show that Deltat degrees alone enforces mechanistic influence on the triplex-forming purine strand so as to favor a zigzag conformation with alternating conformational features that include high (40 degrees ) and low (20 degrees ) helical twists, and high anti(G) and anti(A) glycosyl conformation. Higher thermal stability of this triplex compared to that formed with G* GC and T* AT triplets can be traced to enhanced base-stacking and counterion interactions. Surprisingly, it is found for the first time that the presence of a nonisomorphic G* GC or A* AT base triplet interrupting an otherwise mini A* AT or G* GC isomorphic triplex can induce a bend/curvature in a DNA triplex. These observations should prove useful in the design of triplex-forming oligonucleotides and in the understanding the binding affinities of this triplex with proteins.

Adenine↗
PubMed2005

A new algorithm for predicting triplet-triplet energy-transfer activated complex coordinate in terms of accurate potential-energy surfaces.

The new algorithm presented here allows, for the first time, the determination of the optimal geometrical distortions that an acceptor molecule in the triplet-triplet energy-transfer process undergoes, as well as the dependence of the activation energy of the process on the triplet energy difference of donor and acceptor molecules. This algorithm makes use of the complete potential-energy surfaces (singlet and triplet states), and contrasts with the first-order approximation already published [L. M. Frutos, O. Castano, J. L. Andres, M. Merchan, and A. U. Acuna, J. Chem. Phys. 120, 1208 (2004)] in which an expansion of the potential-energy surfaces was used. This algorithm is gradient based and finds the best trajectory for the acceptor molecule, starting from S(0) ground-state equilibrium geometry, to achieve the maximum variation of the singlet-triplet energy gap with the minimum energy of activation on S(0). Therefore, the algorithm allows the determination of a "reaction path" for the triplet-triplet energy-transfer processes. Also, the algorithm could also serve eventually to find minimum-energy crossing (singlet-triplet) points on the potential-energy surface, which can play an important role in the intersystem crossing process for the acceptor molecules to recover their initial capacity as acceptors. Also addressed is the misleading use of minimum-energy paths in T(1) to describe the energy-transfer process by comparing these results with those obtained using the new algorithm. The implementation of the algorithm is illustrated with different potential-energy surface models and it is discussed in the frame of nonvertical behavior.

Journal Article↗
PubMed2002

Conformational energetics of stable and metastable states formed by DNA triplet repeat oligonucleotides: implications for triplet expansion diseases.

We have embedded the hexameric triplet repeats (CAG)(6) and (CTG)(6) between two (GC)(3) domains to produce two 30-mer hairpins with the sequences d[(GC)(3)(CAG)(6)(GC)(3)] and d[(GC)(3)(CTG)(6)(GC)(3)]. This construct reduces the conformational space available to these repetitive DNA sequences. We find that the (CAG)(6) and (CTG)(6) repeats form stable, ordered, single-stranded structures. These structures are stabilized at 62 degrees C by an average enthalpy per base of 1.38 kcal.mol(-1) for the CAG triplet and 2.87 kcal.mol(-1) for the CTG triplet, while being entropically destabilized by 3.50 cal.K(-1).mol(-1) for the CAG triplet and 7.6 cal.K(-1).mol(-1) for the CTG triplet. Remarkably, these values correspond, respectively, to 1/3 (for CAG) and 2/3 (for CTG) of the enthalpy and entropy per base values associated with Watson-Crick base pairs. We show that the presence of the loop structure kinetically inhibits duplex formation from the two complementary 30-mer hairpins, even though the duplex is the thermodynamically more stable state. Duplex formation, however, does occur at elevated temperatures. We propose that this thermally induced formation of a more stable duplex results from thermal disruption of the single-stranded order, thereby allowing the complementary domains to associate (perhaps via "kissing hairpins"). Our melting profiles show that, once duplex formation has occurred, the hairpin intermediate state cannot be reformed, consistent with our interpretation of kinetically trapped hairpin structures. The duplex formed by the two complementary oligonucleotides does not have any unusual optical or thermodynamic properties. By contrast, the very stable structures formed by the individual single-stranded triplet repeat sequences are thermally and thermodynamically unusual. We discuss this stable, triplet repeat, single-stranded structure and its interconversion with duplex in terms of triplet expansion diseases.

Base Sequence↗
PubMed1998

Photophysics of the cationic 5,10,15,20-tetrakis (4-N-methylpyridyl) porphyrin bound to DNA, [poly (dA-dT)]2 and [poly (dG-dC)]2: interaction with molecular oxygen studied by porphyrin triplet-triplet absorption and singlet oxygen luminescence.

Interaction between molecular oxygen and the cationic free-base 5,10,15,20-tetrakis (4-N-methylpyridyl) porphyrin (H2TMpyP4+) complexed with [poly (dA-dT)]2, [poly (dG-dC)]2 and calf thymus DNA, has been monitored in air-saturated heavy water solutions through porphyrin triplet-triplet absorption and singlet oxygen luminescence. Three different rate constants of porphyrin triplet state quenching have been found which correspond to different accessibilities of molecular oxygen to porphyrins embedded in the duplexes. The longest triplet state lifetime (30 microseconds), found for porphyrin bound to [poly (dG-dC)]2, corresponds to molecules well protected from oxygen. This supports the hypothesis of an intercalative binding mode of the porphyrin between GC base-pairs ('type A' sites). The fraction fT delta of the porphyrin triplet states quenched by molecular oxygen with singlet oxygen generation, is unity. In [poly (dA-dT)]2-porphyrin complexes, two sites ('type B' and 'C' sites of interaction) are involved, yielding very different triplet state lifetimes (5.5 microseconds and 20.5 microseconds) and efficiencies of singlet oxygen generation (fT delta = 0.50 and 0.82). The fT delta decreases can likely be explained in terms of competition between energy and electron transfer from the porphyrin excited triplet state to molecular oxygen. All three types (A, B and C) of interaction sites can be expected in porphyrin-DNA complexes.

Absorption↗
PubMed2004

Triplet-sensitized photolysis of the photoisomer of a 2,11-diaza[3,3](9,10)anthracenoparacyclophane: an adiabatic cycloreversion and a [2pia + 2pia + 2sigmas] rearrangement in a triplet state of the biplanophane system.

The triplet-sensitized photoreactions of the title biplanophane system 6, the photoisomer of a 2,11-diaza[3,3](9,10)anthracenoparacyclophane derivative 5, were investigated by stationary and laser-flash photolyses using xanthone (XT) and benzophenone (BP) as triplet sensitizers. When photoisomer 6 underwent XT-sensitized irradiation, a triplet cyclophane 5 and a novel polycyclic product 7 were obtained via an adiabatic cycloreversion and a formal [2pia + 2pia + 2sigmas] rearrangement, respectively. The maximum quantum yield for the formation of cyclophane 5 (0.69) and the upper-limit efficiency for the formation of polycycle 7 (0.31) were determined by laser photolysis techniques. For BP-sensitized photolysis of photoisomer 6, oxetane 8, in addition to triplet cyclophane 5 and polycycle 7, was formed by a Paterno-Buchi reaction. The quenching rate constant (k(q)) of triplet BP by photoisomer 6 (3.4 x 10(8) dm(3) mol(-)(1) s(-)(1)) was found to be 1 order of magnitude smaller than that for XT (5.0 x 10(9) dm(3) mol(-)(1) s(-)(1)). On the basis of the relationship between k(q) and the triplet donor-acceptor energy gap, the triplet energy level of photoisomer 6 was estimated to be approximately 71 kcal mol(-)(1). The photochemical and the photophysical processes involved in the sensitized photolyses are summarized in an energetic reaction diagram and discussed in detail.

Journal Article↗
PubMed2005

Photochemical reactions of triplet p-phenylbenzyl derivatives studied by using laser flash triplet-sensitization techniques.

Photochemical properties in the triplet states of p-phenylbenzyl derivatives (PBX; X = H, Cl, Br, OH or SH) were investigated by using laser photolysis techniques of triplet-acetone sensitization. Beta-bond dissociation of triplet phenylbenzyl mercaptan (X = SH) was shown for the first time while formation of triplet states were seen for phenyl toluene and phenylbenzyl alcohol by triplet energy transfer. Beta-bond cleavage was absent for halide compounds (X = Cl and Br) upon sensitization because of the short triplet lifetimes due to a heavy atom effect. The reactivity for beta-bond cleavage was interpreted in terms of difference in the bond enthalpy, D(C-X), relative to the triplet energies.

Journal Article↗
PubMed2003

p-Benzyne derivatives that have exceptionally small singlet-triplet gaps and even a triplet ground state.

In an effort to find a p-benzyne (1,4-didehydrobenzene) derivative with a triplet ground state, we have investigated tetrasubstitution by -F, -NH(2), -CH(3), and -NO(2) groups. These were predicted to reduce the singlet-triplet gap, but none led to a triplet ground state because of unexpected destabilization of one of the radical orbitals. This effect is likely the result of rehybridization of the substituted C atom, which has been observed for substituted benzene and perturbs the side sigma and sigma* orbital energies of the phenyl ring. The role of substituent rotation on the energy difference between the two nominally singly occupied orbitals (S and A) was then investigated. The energy of the A radical orbital was found to be much more sensitive to perturbations within the sigma C[bond]C framework than the S MO. Consequently, we believe that rehybridization of the ring carbons destabilizes the A radical orbital and can lead to large singlet-triplet splittings. To test this hypothesis, calculations on a p-benzyne with 2,6 substitution by oxygen were performed. Interestingly, a triplet ground state was predicted. Yet, examination of the geometry and wave function showed that 2,6-quinone p-benzyne is a very twisted molecule with a C3-C4-C5 allene linkage and a C1 triplet carbene center.

Journal Article↗
PubMed2006

Direct observation of the intramolecular triplet-triplet energy transfer in poly(aryl ether) dendrimers.

A series of benzophenone (BP) and naphthalene (NA) labeled poly(aryl ether) dendrimers (BP-Gn-NA), generations 1-4, were synthesized, and their photophysical properties were examined. Flash photolysis demonstrates that the triplet energy in BP-Gn-NA can be transferred from the peripheral BP chromophores to the core NA group with the efficiencies of ca. 0.97, 0.96, 0.88, and 0.54 and with the rate constants of 1.4x10(8), 1.2x10(8), 9.5x10(7), and 1.3x10(7) s-1 at room temperature for generations 1-4, respectively. The transient absorption spectra of BP-Gn-NA show clearly the formation of the triplet NA absorption along with the decay of the triplet BP one with an isosbestic point at 475 nm, which gives direct evidence of the triplet energy transfer from the periphery BP chromphores to the core NA group. The phosphorescence of the NA group attached to the focal point was observed when the periphery BP chromophores were selectively irradiated in BP-G1-NA at 77 K. The triplet energy transfer occurs at 77 K with the efficiencies of 1.0, 0.16, 0.17, and 0.21 for generations 1-4, respectively. The intramolecular triplet energy transfer is proposed to proceed mainly via a through space mechanism.

Journal Article↗
PubMed2004

Forward (singlet-singlet) and backward (triplet-triplet) energy transfer in a dendrimer with peripheral naphthalene units and a benzophenone core.

The photochemical and photophysical behaviour of two dendrimers consisting of a benzophenone core and branches that contain four (4) and eight (5) naphthalene units at the periphery has been investigated in CH(2)Cl(2) solution (298 K) and in CH(2)Cl(2)/CHCl(3) 1:1 v/v rigid matrix (77 K). For comparison purposes, the photophysical properties of dimethoxybenzophenone (1), 2-methylnaphthalene (2) and of a dendron containing four naphthalene units (3) have also been studied. In both dendrimers 4 and 5, excitation of the peripheral naphthalene units is followed by fast (1.1 x 10(9) s(-1) at 298 K, > 2.5 x 10(9) s(-1) at 77 K for 5; 2.9 x 10(8) s(-1) at 298 K, 7 x 10(5) s(-1) at 77 K for 5) singlet-singlet energy transfer to the benzophenone core. On a longer time scale (>1 x 10(6) s(-1) at 298 K, >6 x 10(3) s(-1) at 77 K for 4; 3.1 x 10(7) s(-1) at 298 K, ca. 3 x 10(2) s(-1) at 77 K for 5) a back energy transfer process takes place from the triplet state of the benzophenone core to the triplet state of the peripheral naphthalene units. Selective excitation of the benzophenone unit is followed by intersystem crossing and triplet-triplet energy transfer to the peripheral naphthalene units. In hydrogen donating solvents, the benzophenone core is protected from degradation by the presence of the naphthalene units. In solutions containing Tb(CF(3)SO(3))(3), sensitization of the green Tb(3+) luminescence is observed on excitation of both the peripheral naphthalene units and the benzophenone core of 5. Upon excitation of the naphthalene absorption band (266 nm) with a laser source, intradendrimer triplet-triplet annihilation of naphthalene excited states leads to delayed naphthalene fluorescence (lambda(max)= 335 nm), that can also be obtained upon excitation at 355 nm (benzophenone absorption band). The results obtained show that preorganization of photoactive units in a dendritic structure can be exploited for a variety of useful functions, including photosensitized emission, protection from undesired photoreactions, and energy up-conversion.

Journal Article↗
PubMed2002

Thermodynamic contributions for the incorporation of GTA triplets within canonical TAT/TAT and C+GC/C+GC base-triplet stacks of DNA triplexes.

Nucleic acid triple helices may be used in the control of gene expression. One limitation of using triplex-forming oligonucleotides as therapeutic agents is that their target sequences are limited to homopurine tracts. To increase the repertoire of sequences that can be targeted, it has been postulated that a guanine can target a thymidine forming a stable GTA mismatch triplet. In this work, we have used a combination of optical and calorimetric techniques to determine thermodynamic unfolding profiles of two triplexes containing a single GTA triplet, d(A(3)TA(3)C(5)T(3)AT(3)C(5)T(3)GT(3)) (ATA) and d(AGTGAC(5)TCACTC(5)TCGCT) (GTG), and their control triplexes, d(A(7)C(5)T(7)C(5)T(7)) (TAT7) and d(AGAGAC(5)TCTCTC(5)TCTCT) (AG5T). In general, the presence of a GTA mismatch in DNA triplexes is destabilizing; however, this destabilization is greater when placed in a C(+)GC/C(+)GC base-triplet stack than between a TAT/TAT stack. These destabilizations are accompanied by a reduced unfolding enthalpy of approximately 10 kcal/mol, suggesting a decrease in the base stacking contributions surrounding the mismatch. Relative to their corresponding control triplexes, the folding of ATA is accompanied by a lower counterion uptake and a similar proton uptake, while GTG folding is accompanied by an increase in the counterion and proton uptakes. These effects are consistent with the observed decrease in stacking interactions. The overall results indicate that the main difficulty of targeting pyrimidine interruptions is that the decrease in stacking contributions, due to the incorporation of a GTA mismatch, affects the stability of the neighboring base triplets. This suggests that nucleotide analogues that increase the strength of these base-triplet stacks will result in a more effective targeting of pyrimidine interruptions.

Adenosine↗
PubMed2006

Triplet-state conformational changes in 15-cis-spheroidene bound to the reaction center from Rhodobacter sphaeroides 2.4.1 as revealed by time-resolved EPR spectroscopy: strengthened hypothetical mechanism of triplet-energy dissipation.

Time-resolved EPR spectra of 15-cis-spheroidene bound to the reaction center from Rhodobacter sphaeroides 2.4.1 were recorded at low temperatures. (1) A three-component analysis of the spectral-data matrices by singular-value decomposition followed by global fitting identified the transformation of the triplet carotenoid, (3)Car(I) --> (3)Car(II); during this process, the leak of the triplet population was suggested. A four-component analysis suggested the presence of a representative intermediate, (3)Car(R), that forms a leak channel of the triplet population. (2) A theoretical calculation of the zero-field splitting parameters, |D| and |E|, by the use of a polyene model, showed that the transformation, (3)Car(I) --> (3)Car(R) --> (3)Car(II), accompanies the conformational changes of (0 degrees , 0 degrees , 0 degrees ) --> (+20 degrees , -20 degrees , +20 degrees ) --> (+45 degrees , -40 degrees , +40 degrees ) around the central cis C15=C15', trans C13=C14, and trans C11=C12 bonds, respectively. (3) The initial, rapid decrease followed by the inversion of spin polarization along the z axis of (3)Car was observed, which was correlated with a change in the spin angular momentum. (4) In reference to the binding pocket of the Car, determined by X-ray crystallography, the conformational changes were ascribed to the intrinsic isomerization property of 15-cis (3)Car as well as the Car-peptide intermolecular interaction; a detailed picture was proposed. All of the above results support the mechanism of triplet-energy dissipation proposed previously: the rotational motions around the central double bonds cause a change in the orbital angular momentum and, through the spin-orbit coupling, a change in the spin angular momentum, which enhances the T(1) --> S(0) intersystem crossing dissipating the triplet energy.

Carotenoids↗
PubMed2005

Triplet acetylenes as synthetic equivalents of 1,2-bicarbenes: phantom n,pi state controls reactivity in triplet photocycloaddition.

Diaryl acetylenes, in which one of the aryl groups is either a pyridine or a pyrazine, undergo efficient triplet state photocycloaddition to 1,4-cyclohexadiene with formation of 1,5-diaryl substituted tetracyclo[3.3.0.0(2,8).0(4,6)]octanes (homoquadricyclanes). In the case of pyrazinyl acetylenes, the primary homoquadricyclane products undergo a secondary photochemical rearangement leading to diaryl substituted tricyclo[3.2.1.0(4,6)]oct-2-enes. Mechanistic and photophysical studies suggest that photocycloaddition proceeds through an electrophilic triplet excited state whereas the subsequent rearrangement to the tricyclooctenes proceeds through a singlet excited state. Chemical and quantum yields for the cycloaddition, in general, correlate with the electron acceptor character of aryl substituents but are attenuated by photophysical factors, such as the competition between the conversion of acetylene singlet excited state into the reactive triplet excited states (intersystem crossing: ISC) and/or to the radical-anion (photoelectron transfer from the diene to the excited acetylene: PET). Dramatically enhanced ISC between pi-pi S(1) state and "phantom" n,pi triplet excited state is likely to be important in directing reactivity to the triplet pathway. The role of PET can be minimized by the judicious choice of reaction conditions (solvent, concentration, etc.). From a practical perspective, such reactions are interesting because "capping" of the triple bond with the polycyclic framework orients the terminal aryl (4-pyridyl, 4-tetrafluoropyridyl, phenyl, etc.) groups in an almost perfect 60 degrees angle and renders such molecules promising supramolecular building blocks, especially in the design of metal coordination polymers.

Journal Article↗