Stepwise two-color laser photolysis studies of alpha-cleavage in highly excited triplet states of alpha-acyl-4-phenylphenols.

The photochemical properties of alpha-cleavage of C-O bond in highly excited triplet states (T(n) with n>2) of p-biphenyl acetate and p-biphenyl benzoate (Me-OBP and Ph-OBP) in solution were investigated in comparison with those in the lowest excited singlet and triplet states by using single laser and sequential two-color two-laser photolysis techniques. Upon 266 nm laser photolysis of Me-OBP and Ph-OBP, occurrence of C-O bond cleavage in the excited singlet state was recognized from the observation of the formation of p-phenylphenoxy radical (PPR) in the transient absorption. The quantum yields (Phi(rad)) of the PPR formation were determined to be 0.29 and 0.24 for Me-OBP and Ph-OBP, respectively. Triplet sensitization using acetone (Ac) provided efficient formation of the lowest triplet states (T(1)) of Me-OBP and Ph-OBP, and the molar absorption coefficients of the triplet-triplet absorption were determined. No photochemical reactions were found in the T(1) state. Upon 355 nm laser flash photolysis of the T(1) states of Me-OBP and Ph-OBP, formation of PPR accompanied with decomposition of the triplet state was confirmed in the transient absorption. This observation indicated that alpha-cleavage proceeds in the highly excited triplet state. The quantum yields (Phi(dec)) of the decomposition in the dissociative highly excited triplet state (T(R)) were determined to be 0.25 and 0.15 for Me-OBP and Ph-OBP, respectively. The reaction mechanism for alpha-bond cleavage in the T(R) state was discussed.     

Characterization of the transient species generated by the photoexcitation of C-phycocyanin from Spirulina platensis: a laser photolysis and pulse radiolysis study

Nanosecond laser flash photolysis and pulse radiolysis were used to generate and characterize the triplet state and cation radical of C-phycocyanin (C-PC) from Spirulina platensis. The transient absorption spectra of C-PC were measured from direct excitation and acetone sensitization in aqueous solution at room temperature by KrF (248 nm) laser flash photolysis. Laser-induced transient species have been characterized by the method of acetone sensitization and one-electron oxidation. In nitrous oxide-saturated phosphate buffer saline (pH = 7.0) of C-PC, the produced intermediates are assigned to the excited triplet state and the radical cation. Using acetone as photosensitizer, the C-PC excited triplet states produced via triplet-triplet energy transfer and the C-PC radical cation from electron transfer reaction were further confirmed. Furthermore, the corresponding kinetic parameters were determined. To our knowledge, the transient absorption spectra of C-PC have been reported for the first time.     

Primary steps of the photochemical reactions of 2-cyano-10-(3-[dimethylamino, N-oxide]-2-methylpropyl)-5-oxide-phenothiazine, the photoproduct of cyamemazine, a phototoxic neuroleptic: comparison with the sulfoxide.

The UVA-absorbing photoproduct resulting from the oxidation of the sulfur atom and of the side chain nitrogen of the phototoxic drug cyamemazine (CMZ) (2-cyano-10-(3-[dimethylamino]-2 methylpropyl)-phenothiazine) is a potent photodynamic photosensitizer. The photophysical and photochemical properties of this photoproduct (P) (2-cyano-10-(3-[dimethylamino, N-oxide]-2-methylpropyl)-5-oxide-phenothiazine)) have been investigated in neutral buffered aqueous solutions and in ethanol and compared to those of the sulfoxide (S) (2-cyano-10-(3-[dimethylamino]-2 methylpropyl)-5-oxide-phenothiazine), a CMZ oxidation product of cells. The fluorescence quantum yield (PhiF) of P is 0.25 and 0.21 in pH 7 phosphate buffer and ethanol, respectively. By contrast, S (PhiF = 0.14 in buffer) is practically unfluorescent in alcohol. In buffer, the fluorescence lifetimes of P and S are 10.5 and 11.8 ns, respectively. The transient absorbance of the first excited triplet state (3P1) with a characteristic absorption band peaking at 660 nm (epsilon = 5,300 M(-1) cm(-1)) has been observed by 355 nm laser flash spectroscopy of deaerated phosphate buffer or ethanol solutions. In buffer, the 3P1 lifetime is 0.5 micros. The energy transfer which occurs from the 3P1 to naproxen suggests that the 3P1 energy is greater than 62 kcal mol(-1). Triplet quenching by dioxygen occurs at rate 2.3 x 10(9) M(-1) s(-1). With the triplet benzophenone as actinometer, the 3P1 formation quantum yield is found to be 0. 40 in buffer. The 3P1 state is quenched by ethanol and 2-propanol with bimolecular reaction rate constants of 1.6 and 2.4 x 10(6) M(-1) s(-1), respectively. In buffer, P and S triplet states react with tryptophan, indole and cysteine at rate constants of the order of 10(9) M(-1) s(-1) for Trp and indole and 10(8) M(-1) s(-1) for Cys.     

Triplet- vs. singlet-state imposed photochemistry. The role of substituent effects on the photo-Fries and photodissociation reaction of triphenylmethyl silanes.

The photochemistry of three structurally very similar triphenylmethylsilanes 1, 2, 3 [p-X-C(6)H(4)-CPh(2)-SiMe(3): X = PhCO, 1; H, ; Ph(OCH(2)CH(2)O)C, 3] is described by means of 248 and 308 nm nanosecond laser flash photolysis (ns-LFP), femtosecond LFP, EPR spectroscopy, emission spectroscopy (fluorescence, phosphorescence), ns-pulse radiolysis (ns-PR), photoproduct analysis studies in MeCN, and X-ray crystallographic analysis of the two key-compounds 1 and 2. The photochemical behavior of 1, 2 and 3 is discussed and compared with that of a fourth one, 4, bearing on the p-position an amino group (X = Me(2)N) and whose detailed photochemistry we reported earlier (J. Org. Chem., 2000, 65, 4274-4280). Silane 1 undergoes on irradiation with 248 and 308 nm laser light a fast photodissociation of the C-Si bond giving the p-(benzoyl)triphenylmethyl radical (1*) with a rate constant of k(diss)= 3 x 10(7) s(-1). The formation of 1* is a one-quantum process and takes place via the carbonyl triplet excited state with high quantum yield (Phi(rad)= 0.9); the intervention of the triplet state is clearly demonstrated through the phosphorescence spectrum and quenching experiments with ferrocene (k(q)= 9.3 x 10(9) M(-1) s(-1)), Et(3)N (1.1 x 10(9) M(-1) s(-1)), and styrene (3.1 x 10(9) M(-1) s(-1)) giving quenching rate constants very similar to those of benzophenone. For comparative reasons radical 1* was generated independently from p-(benzoyl)triphenylmethyl bromide via pulse radiolysis in THF and its absorption coefficient at lambda(max)= 340 nm was determined ([epsilon]= 27770 M(-1) cm(-1)). We found thus that the p-PhCO-derivative 1 behaves similar to the p-Me(2)N one (the latter giving the p-(dimethylamino)triphenylmethyl radical with Phi(rad)= 0.9), irrespective of their completely different ground state electronic properties. In contrast, compounds 2, 3 that bear only the aromatic chromophore give by laser or lamp irradiation both, (i) radical products [Ph(3)C* and p-Ph(OCH(2)CH(2)O)C-C(6)H(4)-C(*)Ph(2), respectively] after dissociation of the central C-Si bond (Phi(rad)= 0.16), and (ii) persistent photo-Fries rearrangement products (of the type of 5-methylidene-6-trimethylsilyl-1,3-cyclohexadiene) absorbing at 300-450 nm and arising from a 1,3-shift of the SiMe(3) group from the benzylic to the ortho-position of the aromatic ring (Phi approximately 0.85 for 2). Using fs-LFP on 2 we showed that the S(1) state recorded at 100 fs after the pulse decays on a time scale of 500 fs giving Ph(3)C* through C-Si bond dissociation. In a second step and within the next 10 ps trityl radicals either escape from the solvent cage (the quantum yield of Ph(3)C* formation Phi(rad)= 0.16 was measured with ns-LFP), or undergo in-cage recombination to photo-Fries products. Thus, singlet excited states (S(1)) of the aromatic organosilanes (2, 3) prefer photo-Fries rearrangement products, while triplet excited states (1, 4) favor free radicals. Both reactions proceed via a common primary photodissociation step (C-Si bond homolysis) and differentiate obviously in the multiplicity of the resulting geminate radical pairs; singlet radical pairs give preferably photo-Fries products following an in-cage recombination, while triplet radical pairs escape the solvent cage (MeCN). The results demonstrate the crucial role which is played by the chromophore which prescribes in a sense, (i) the multiplicity of the intervening excited state and consequently that of the resulting geminate radical pair, and (ii) the dominant reaction path to be followed: the benzophenone- and anilino-chromophore present in silanes 1 and 4, respectively, impose effective intersystem crossing transitions (k(isc)= 10(11) s(-1) and 6 x 10(8) s(-1), respectively) leading to triplet states and finally to free radical products, while the phenyl chromophore in 2 and 3, possessing ineffective isc (k(isc)= 6 x 10(6) s(-1)) leads to photo-Fries product formation via the energetic high lying S(1) state [approximately 443 kJ mol(-1)(106 kcal mol(-1))].     

Singlet oxygen production by pyrano and furano 1,4-naphthoquinones in non-aqueous medium

The influence of ring size on the photobehaviour of condensed 1,4-naphthoquinone systems, such as pyrano- and furano-derivatives (1 and 2, respectively) has been investigated. The absorption spectra for both families of naphthoquinones reveal clear differences; in the case of 2 they extend to longer wavelengths. A solvatochromic red shift in polar solvents is consistent with the π,π* character of the S(0)→ S(1) electronic transition in all cases. Theoretical (B3LYP) analysis of the HOMO and LUMO Kohn-Sham molecular orbitals of the S(0) state indicates that they are π and π* in nature, consistent with the experimental observation. A systematic study on the efficiency of singlet oxygen generation by these 1,4-naphthoquinones is presented, and values larger than 0.7 were found in every case. In accordance with these results, laser flash photolysis of deoxygenated acetonitrile solutions led to the formation of detectable triplet transient species with absorptions at 390 and 450 nm (1) and at 370 nm (2), with φ(ISC) close to 1. Additionally, the calculated energies for the T(1) states relative to the S(0) states at UB3LYP/6-311++G** are ca. 47 kcal mol(-1) for 1 and 43 kcal mol(-1) for 2. A comparison of the geometrical parameters for the S(0) and T(1) states reveals a marked difference with respect to the arrangement of the exocyclic phenyl ring whilst a comparison of electronic parameters revealed the change from a quinone structure to a di-dehydroquinone diradical structure.     

Characterization of the indole triplet excited state in proteins utilizing laser flash photolysis

The triplet-triplet absorption spectrum of the sole indole side chain of human serum albumin and its decay kinetics were previously characterized, at room temperature, by using a conventional flash photolysis method [(1978) Proc. Natl. Acad. Sci. USA 75, 1172-1175]. Exploitation of this potentially useful long lived reporter group in protein studies was limited by the excessively large sample size required by that apparatus. The 265 nm laser flash instrument used in the present work avoids this problem at the price of a loss in photo-selectivity. We report that the latter concern can be mitigated. Melittin was studied first because this polypeptide contains a single aromatic residue (W-19), and because its monomeric and tetrameric forms are good models for solvent exposed and buried indole side chains of proteins. For both forms, the indole triplet and neutral radical absorption spectra could be readily time resolved and identified on the basis of shape and differential dioxygen sensitivity. The single tryptophan containing protein human serum albumin was studied next because it contains a large number of other 265 nm absorbing moieties whose transient spectra might complicate the detection of the indole triplet. These transients were shown to not interfere significantly in the wavelength region 450 nm to 600 nm, and, in contrast to the indole triplet, they were relatively dioxygen insensitive. Thus, a facile means is available by which the indole triplet of proteins may be characterized. Subsequently the question of whether this species could be detected in the presence of nuclei acid components was investigated by flashing the phage fd. The putative nucleic acid transients were shown not to interfere and the absorbance of the indole triplet was readily time resolved. The spectral assignment was persuasively confirmed by showing that the indole triplet absorption and phosphorescence emission spectra decay with the same lifetime. The present work thus provides additional evidence for the general applicability of the indole triplet excited state as a long lived intrinsic protein reporter group.     

Singlet and triplet excited carotenoid and antenna bacteriochlorophyll of the photosynthetic purple bacterium Rhodospirillum rubrum as studied by picosecond absorbance difference spectroscopy

Picosecond absorbance difference spectra at a number of delay times after a 35 ps excitation pulse and kinetics of absorbance changes were measured in chromatophores of the photosynthetic purple bacterium Rhodospirillum rubrum after chemical oxidation of the primary electron donor P-875. Kinetics and spectra were measured of the excited singlet states of carotenoid and bacteriochlorophyll a and also of the triplet state of the carotenoid. The excited singlet state of carotenoid, produced by direct excitation at 532 nm, is characterized by a bleaching of the ground state absorption bands in the region 450–490 nm and by an absorbance increase with a maximum near 570 nm. Its lifetime was calculated to be 0.6 ± 0.1 ps in vitro and less than 1 ps in vivo. The triplet state of carotenoid in vivo is formed within 100 ps after direct carotenoid excitation via a pathway that does not involve excited states of bacteriochlorophyll. Singlet excitation of a bacteriochlorophyll a molecule causes the bleaching of its Q_x and Q_y absorption bands, and is probably associated with blue shifts of the Q_y absorption band of about six neighboring bacteriochlorophyll molecules. Upon increasing the excitation density, the average lifetime of the singlet excitations on bacteriochlorophyll decreased from about 350 ps to about 10 ps or less. The results are in quantitative agreement with the known effect of singlet-singlet annihilation upon the fluorescence yield, and furthermore show that no bacteriochlorophyll or carotenoid triplet formation is associated with this annihilation.     

Excited-state properties of Escherichia coli DNA photolyase in the picosecond to millisecond time scale

Escherichia coli DNA photolyase contains a stable flavin radical that is readily photoreduced in the presence of added electron donors. Picosecond, nanosecond, and conventional flash photolysis technique have been employed to investigate the events leading to photoreduction from 40 ps to tens of milliseconds following flash excitation. Direct light absorption by the flavin radical produces the first excited doublet state which undergoes rapid (within 100 ps) intersystem crossing to yield the lowest excited quartet (n pi*) state. In contrast, light absorption by the folate chromophore produces a new intermediate state via interaction of the folate excited singlet state with the ground-state flavin radical, leading to an enhanced yield of the excited radical doublet state and hence quartet state. Subsequent reaction of the excited quartet state involves hydrogen atom abstraction from a tryptophan residue. Secondary electron transfer from added electron donors occurs to the oxidized tryptophan radical with rate constants ranging from 10(4) (dithiothreitol) to 4 x 10(6) M-1 s-1 (n-propyl gallate). The low value of the latter rate compared to reduction of the tryptophan radical in lysozyme suggests that the reactive tryptophan is highly buried in photolyase. A redox potential diagram has been constructed for the ground and excited states involved. It is concluded that the one-electron reduction potential of the excited quartet state of the flavin radical must be at least 1.23 V more positive than the ground state, in agreement with the value of delta E greater than 1.77 V calculated from spectroscopic data.     

Excited carbonyl formation in the combination and disproportionation of free radicals

The pyrolyisis of di-tert-butyl peroxyoxalate in the presence of para-substituted benzaldehydes produces almost quantitatively the corresponding p,p′-disubstituted benzils. The formation of these products is accompanied by chemiluminescence arising from excited triplets. From the quantum yield of excited triplet generation and the rate constants for the triplet photocleavage it is possible to obtain the change in Gibbs free energy associated with triplet formation. The values obtained are ?5.6, ?5.7 and ?8.1 kcal/mol for benzil, p,p′-dimethylbenzil and p,p′-dimethoxybenzil, respectively. The pyrolysis of di-tert-butyl peroxyoxalate in the presence of isopropanol or benzoin leads to the formation of acetone and benzil. These products are generated in disproportionation processes involving the α-hydroxy radical produced by hydrogen abstraction. The luminescence observed in these reactions constitutes the first experimental indication of excited species generation in the disproportionation of uncorrelated free radicals.     

Quantum yield and rate of formation of the carotenoid triplet state in photosynthetic structures

The formation of the triplet state of carotenoids (detected by an absorption peak at 515 nm) and the photo-oxidation of the primary donor of Photosystem II, P-680 (detected by an absorption increase at 820 nm) have been measured by flash absorption spectroscopy in chloroplasts in which the oxygen evolution was inhibited by treatment with Tris. The amount of each transient form has been followed versus excitation flash intensity (at 590 or 694 nm). At low excitation energy the quantum yield of triplet formation (with the Photosystem II reaction center in the state Q⁻) is about 30% that of P-680 photo-oxidation. The yield of carotenoid triplet formation is higher in the state Q⁻ than in the state Q, in nearly the same proportion as chlorophyll a fluorescence. It is concluded that, for excited chlorophyll a, the relative rates of intersystem crossing to the triplet state and of fluorescence emission are the same in vivo as in organic solvent. At high flash intensity the signal of P-680⁺ completely saturates, whereas that of carotenoid triplet continues to increase.

The rate of triplet-triplet energy transfer from chlorophyll a to carotenoids has been derived from the rise time of the absorption change at 515 nm, in chloroplasts and in several light-harvesting pigment-protein complexes. In all cases the rate is very high, around 8 · 10⁷ s⁻¹ at 294 K. It is about 2–3 times slower at 5 K. The transitory formation of chlorophyll triplet has been verified in two pigment-protein complexes, at 5 K.     

Preparation and photophysical properties of precursors of inorganic macromolecules. Mono and binuclear complexes of Ru(II) and terpyridine derivatized with thiophene and 4-(5-bromothiophene) groups

The preparation and characterization of mono and binuclear complexes of Ru(II) with a newly synthesized derivate of the terpyridine ligand, 4^′-(5-bromothiophene)-2,2^′,6^′,2″-terpyridine, are communicated. In the binuclear complex, 2,5-bis(2,2^′,6^′,2″-terpyridine-4^′yl)thiophene was used as a bridge between two Ru(II) centers. The new compounds were characterized by H NMR, UV-Vis and IR spectroscopies. Bands at ∼500 nm for the Ru(II) to terpyridine charge transfer transition and absorption bands at λ<400 nm assigned to intraligand transitions, π^*←π, centered in the tpy moiety were observed in the UV-Vis spectra of the complexes. Irradiation of the complexes in CH₃CN at 337 or 500 nm induced luminescence with maxima at ∼670 nm and lifetimes τ?10² ns. Time-resolved absorption spectroscopy revealed the formation of long-lived species during the decay of the metal to ligand charge transfer excited states. The intermediates were tentatively assigned as unstable products of ligand-substitution or orthometalation excited state reactions.     

Further evidence for dissipative energy migration via triplet states in photosynthesis. The protective mechanism of carotenoids in Rhodopseudomonas spheroides chromatophores.

The protection action of carotenoids against irreversible photodestruction was discovered in photosynthetic bacteria by Stanieda and coworkers. In green plant material it was found by Wolff and Witt (1969) Z. Naturforsch, 24b, 1031-1037 and (1972) Proc. 2nd. Int. Congr. Photosynthesis Res. Stresa (Forti, G., Avron, M. and Melandri, A., eds.), Vol. 2, pp. 931-936, Dr. W. Junk, N. V. Publ. The Hague) that the formation of special carotenoid triplet states (via very rapid energy transfer from excited chlorophylls) and their fast radiationless decay in tau1/2 approximately 3 microns is at least one mechanism for the protective action of carotenoids to irreversible photooxidation of the chlorophylls. Hence, it is anticipated that the same mechanism might be realized also in bacteria. The present study gives evidence for such a "triplet valve" to be established also in bacteria. This conclusion was derived from the following observations: 1. The light-induced difference spectrum shows a bleaching of a carotenoid at three characteristic wavelength between 400 and 500 nm. A positive peak around 533 nm indicates the formation of a carotenoid triplet state. 2. The absorption changes can be induced by red light which excites only bacteriochlorophyll. This indicates an energy transfer from bacteriochlorophyll to carotenoids. 3. The light-induced carotenoid triplets decay radiationless in 3 microns in air-saturated aqueous suspensions of the chromatophores. 4. The carotenoid triplet formation occurs only at actinic flash intensities where the photosynthesis becomes saturated. 5. Addition of dithionite, which blocks photosynthesis, markedly increases the extent of carotenoid triplet formation. The different types of exciton migration within the photosynthetic unit are discussed, especially the routes leading to the dissipation of excess excitation energy.     

Analysis of substances issuing from Zajdela ascitic hepatoma cells after exposure to UV radiation of different wave-lengths. I. Relationship to dose]

The release of substances from the Zaidela ascitic hepatoma cells after irradiation with physiological doses of short-wave (254 nm) and long-wave (300-380 nm) UV light (far and near UV light) has been studied spectrophotometrically. Within the range of 200-520 nm, the absorption spectra of releasing substances show maxima at 215 and 260 nm and are identical to spectra of non-irradiated cells. The amount of substances increases with dose making up, at the maximal alteration, 180-220%, of the amount releasing from non-irradiated cells. Irradiation with far UV light exceeds by one order that with near UV light. The effect of minimum doses is opposite to the action of high doses: the release of substances from irradiated cells is much less.     

豆壳过氧化物酶的电子吸收光谱性质

应用电子吸收光谱技术研究了豆壳过氧化物酶 ( EC1 .1 1 .1 .7)的不同氧化态电子吸收光谱 ,并与其它来源的过氧化物酶作了比较研究 .天然态酶的特征吸收峰位为 40 4 nm的 Soret带 ,638nm的α带和 50 8nm的β带 ,与过氧化氢反应可生成三类复合物 .复合物 ( Com )在 40 8、580、61 8和 655nm处出现特征吸收 ;复合物 ( Com )在 41 9、52 9和 556nm处显示特征吸收 ;复合物 ( Com )则于 41 8、543和 578nm处显示特征吸收 .天然态酶经连二亚硫酸钠还原则出现 435和 558nm的特征峰 ,与氰化钾作用在 42 2和 544nm处显示特征吸收 .氰化钾对该酶的抑制为竞争性抑制 ,其 Ki 值为 2 .4μmol/L.     

Optically detected magnetic resonance of the phosphorescent bases of Escherichia coli valine-specific transfer ribonucleic acid

Phosphorescence spectroscopy and optical detection of triplet state magnetic resonance (ODMR) spectroscopy have been used to characterize bases that contribute to the phosphorescence emission of Escherichia coli valine-specific transfer ribonucleic acid. When it is excited with 335-nm light, a short-lived phosphorescence with an origin near 435 nm is observed and is assigned to 4-thiouridine (s4U) at position 8 of the tRNA sequence. With excitation at 290-300 nm, a structured, long-lived phosphorescence is observed with an origin near 380 nm, in addition to the s4U phosphorescence. Comparison was made of the phosphorescence and ODMR spectra between Mg2+-containing and Mg2+-free tRNA samples. The s4U phosphorescence of the Mg2+-containing sample is more structured, and the peak is blue shifted relative to the Mg2+-free sample. Both samples give a single low-frequency (ca. 2.9 GHz) ODMR signal, but the high-frequency signal region (ca. 19-20 GHz) is structured. The Mg2+-containing sample has a partially resolved group of lines centered at 19.3 GHz, whereas the Mg2+-free sample has two broad bands centered at 19.2 and 20.0 gHz. The differences are attributed to effects of Mg2+ on the tRNA conformation. The ODMR signals observed by monitoring the long-lived phosphorescence are assigned to a pyrimidine nucleoside, possibly 5-(carboxy-methoxy)uridine in the anticodon.     

Reduced formation of bipyrimidine photoproducts in DNA UV irradiated at high intensity

DNA was irradiated using an excimer laser (248 nm) at low intensity (3.15 x 10(7) watts/m2) or high intensity (1.25 x 10(11) watts/m2). Fluences up to 30 kJ/m2 were delivered at either intensity. Following irradiation, DNA damage products were measured, yielding the following findings: 1) the rate of formation of thymine-thymine and thymine-cytosine cyclobutane dimers and the bipyrimidine photoadduct 6-4'-[pyrimidine-2'-one]thymine were reduced at high intensity by about 2-fold and 2) extensive release of free thymine and thymine decomposition fragments occurred at high intensity, but not at low intensity. The effects of high intensity UV are due to promotion of low-lying excited state(s) by absorption of a second photon, producing higher excited state(s) with consequent ionization and base loss. Possible excited state intermediates in this process are the lowest triplet state of DNA bases and prolonged singlet states associated with excimer formation. The depletion of these excited states via promotion may be the cause of the diminished yield of bimolecular pyrimidine photoproducts, suggesting that these photoproducts are formed at low UV intensity in part from long-lived excited states. Long-lived excited states present at conventional UV intensities may contribute to formation of some photoproducts that occur rarely, but are of potential biologic importance, such as dimers between nonadjacent pyrimidines on the same strand and interstrand dimers forming DNA cross-links.     

High-order fluorescence and exciton interaction in photosynthetic bacteria

We have observed fluorescence at visible wavelengths from chromatophores of photosynthetic bacteria excited with infrared radiation which we attribute to bacteriochlorophyll of the antenna system. The fluorescence is prompt (no delay greater than 5 ns). Its spectrum shows peaks at 445, 530 (broad) and 600 nm when excited with either 694 or 868 nm. Quantum yield is of the order of 10^?9. The dependence on intensity indicates generation by mainly third-order processes which could involve triplet states in combination with excited singlets. Second-order single-singlet fusion could also contribute. The high-order fluorescence can also be explained as arising from absorption of a second photon by singlet excited states.     

Syntheses of imido-substituted glycosans and their photocyclisation towards highly functionalised heterotricycles.

Reaction of O-protected amino-1,6-anhydro-beta-D-hexopyranoses with succinic or glutaric anhydride and subsequent intramolecular acylation afforded the succinimido- and glutarimido-substituted glycosans. Irradiation with UV light of 254 nm wavelength led to gamma-hydrogen abstraction at the pyranose ring by the excited carbonyl function. The stereoselective recombination of the resulting 1,4-diradicals gave annelated azetidinols, which fragmented by a retrotransannular ring opening reaction to give the glycosan-annelated azepanedione and azocanedione systems, respectively.     

The final stages of folding of the membrane protein bacteriorhodopsin occur by kinetically indistinguishable parallel folding paths that are mediated by pH

The folding of the transmembrane protein bacteriorhodopsin that occurs during the binding of its retinal cofactor is investigated in a membrane-like environment. Changes in the retinal absorption band reveal two transient retinal-protein intermediate states, with apparent absorption maxima at 380 nm and 440 nm, respectively. Studies on a bacteriorhodopsin mutant of Lys216, which cannot bind retinal covalently, add to evidence that retinal is non-covalently bound in these intermediate states. The two retinal-protein intermediates are genuine intermediate states that form in parallel, each with an observed rate constant of 1.1 s-1. Meanwhile no formation of the folded state is detected. Folded bacteriorhodopsin, with all trans retinal covalently bound, forms from both retinal-bound intermediates with the same apparent rate constant of 0.0070 s-1 that is independent of retinal concentration. Retinal isomerisation then occurs with a rate constant of 0.00033 s-1 to give bacteriorhodopsin containing all trans and 13 cis-retinal. These results provide experimental evidence for multiple folding routes for a membrane protein that are pH dependent, with pH conditions determining the apparent folding route. These observed parallel folding paths are kinetically indistinguishable, which contrasts with most other observations of parallel folding pathways where only pathways with different kinetics have been reported. Furthermore, together with previous work, this study shows that bacteriorhodopsin has to populate at least two folding intermediates, during folding in the mixed lipid micelles investigated here, before the final fold is attained.     

Quenching of chlorophyll triplet states by carotenoids in reconstituted Lhca4 subunit of peripheral light-harvesting complex of photosystem I

In this study, triplet quenching, the major photoprotection mechanism in antenna proteins, has been studied in the light-harvesting complex of photosystem I (LHC-I). The ability of carotenoids bound to LHC-I subunit Lhca4, which is characterized by the presence of the red-most absorption components at wavelength >700 nm, to protect the system through quenching of the chlorophyll triplet states, has been probed, by analyzing the induction of carotenoid triplet formation. We have investigated this process at low temperature, when the funneling of the excitation toward the low-lying excited states of the Chls is stronger, by means of optically detected magnetic resonance (ODMR), which is well-suited for investigation of triplet states in photosynthetic systems. The high selectivity and sensitivity of the technique has made it possible to point out the presence of specific interactions between carotenoids forming the triplet states and specific chlorophylls characterized by red-shifted absorption, by detection of the microwave-induced Triplet minus Singlet (T-S) spectra. The effect of the red forms on the efficiency of triplet quenching was specifically probed by using the Asn47His mutant, in which the red forms have been selectively abolished (Morosinotto, T., Breton, J., Bassi, R., and Croce, R. (2003) J. Biol. Chem. 278, 49223-49229). Lack of the red forms yields into a reduced efficiency of the triplet quenching in LHC-I thus suggesting that the "red Chls" play a role in enhancing triplet quenching in LHC-I and, possibly, in the whole photosystem I.