KINETICS OF BACTERIAL BIOLUMINESCENCE AND THE FLUORESCENT TRANSIENT

Abstract— The addition of FMNH₂ to Vibrio harveyi luciferase at 2°C in the presence of tetradecanal results in the formation of a highly fluorescent transient species with a spectral distribution indistinguishable from that of the bioluminescence. The bioluminescence reaches maximum intensity in 1.5 s and decays in a complex manner with exponential components of 10^-1s^-1, 7 × 10^-3s^-1, and 7 × 10 ⁴s^-1. The fluorescent transient rises exponentially at 7 × 10^-2s^-3 and decays at 3 × 10^-4s^-1. The slowest bioluminescence component, comprising the bulk of the bioluminescence, decays at twice the rate of the fluorescent transient under all variations of reaction conditions: concentration of reactants, temperature 2–20°C, and aldehyde chain length—decanal, dodecanal and tetradecanal. The activation energy for both the slowest bioluminescence decay and the transient fluorescence decay is 80 kJ-mol^-1. An energy transfer scheme is proposed to explain the results where two distinct chemically energized species utilize the fluorescent transient as emitter for the slower bioluminescences, and for the faster process a fluorophore present in the protein preparation. Kinetic observations suggest that typical preparations of V. harveyi luciferase comprise 15% active protein.     

CHEMICAL FILTERS FOR NARROW BAND U.V. IRRADIATION BETWEEN 235 AND 300 nm

Abstract— Six chemical filters are described. Bands of 10–20 nm half width are isolated at the following wavelengths: 235–240–252–260–277–294 nm. The filters transmit at the center of their band pass between 1.5 and 30 per cent of the incident radiation. Average photon fluence rates of 15–150 ergs mm^-2 sec^-1 (0.3 × 10^-3 to 3.5 × 10^-3μE cm^-2 sec^-1) are obtained with a 500 W high pressure mercury arc focussed on a 10 cm^-2 area. Under these conditions, the flux transmitted in the near i.r., visible and near u.v. does not exceed 1 per cent of the total flux transmitted. The flux transmitted outside a 40 nm band centered at the maximum does not exceed 1 per cent of the total transmitted flux for four of the filters, this flux goes up to 4 per cent of the total for the 294 nm filter and to 10 per cent for the 235 nm filter.     

A SINGLE PULSE PICOSECOND LASER STUDY OF EXCITON DYNAMICS IN CHLOROPLASTS

Abstract. Using single picosecond laser pulses at 610 nm, the fluorescence yield (φ) of spinach chloroplasts as a function of intensity ( I ) (10¹²-10¹⁶ photons/pulse/cm²) was studied in the range of 21–300 K. The quantum yield decreases with increasing intensity and the φ vs I curves are identical at the emission maxima of 685 and 735 nm. This result is interpreted in terms of singlet exciton-exciton annihilation on the level of the light-harvesting pigments which occurs before energy is transferred to the Photosystem I pigments which emit at 735 nm.
The yield φ is decreased by factors of 12 and 43 at 300 and 21 K, respectively. The shapes of the φ vs I curves are not well accounted for in terms of a model which is based on a Poisson distribution of photon hits in separate photosynthetic units, but can be satisfactorily described using a one-parameter fit and an exciton-exciton annihilation model. The bimolecular annihilation rate constant is found to be γ= (5–15) times 10^-9cm³s^-1 and to exhibit only a minor temperature dependence. Lower bound values of the singlet exciton diffusion coefficient (≥ 10^-3cm²s^-1), diffusion length (≥ 2 times 10^-6cm) and Förster energy transfer rates (≥ 3 ≥ 10¹⁰s^-1) are estimated from γ using the appropriate theoretical relationships.     

REEVALUATION OF THE SPECTRAL AND KINETIC PROPERTIES OF HO2 AND O2- FREE RADICALS

Abstract— The spectra and molar absorbances of the HO₂ and O₂^- free radicals have been redetermined in aqueous formate solutions by pulse and stopped-flow radiolysis as well as by ⁶⁰Co gamma-ray studies. The extinction coefficients at the corresponding maxima and 23°C are ²²⁵= 1400 ± 80 M ^-1 cm^-1 and ²²⁵= 2350 ± 120 M ^-1 cm^-1 respectively. Reevaluation of earlier published rate data in terms of the new extinction coefficients yielded the following rate constants for the spontaneous decay of HO₂ and O₂^-: K _Ho2+HO2= (8.60 ± 0.62) × 10⁵ M ^-1 s^-1; K _Ho2+O2-= (1.02 ± 0.49) × 10⁸ M ^-1 s^-1; K _Ho2+O2- < 0.35 M ^-1 s^-1. For the equilibrium HO₂→ O₂^-+ H⁺ the dissociation constant is K _Ho2= (2.05 ± 0.39) × 10^-5 M or p K _HO2= 4.69 ± 0.08. G (O₂^-) has been evaluated as a function of formate concentration.     

THE FLUORESCENCE OF ADENINE. THE EFFECTS OF SOLVENT AND TEMPERATURE ON THE QUANTUM YIELD

Abstract— To investigate the mechanism of the solvent and thermal quenching of fluorescence, the absolute fluorescence quantum yield of adenine has been determined in several alcoholic glasses as a function of the concentration (10^-5-10^-4M) and temperature (77°-298°K). The yield is independent of the concentration but increases with decreasing temperature and increasing bulk cohesion and rigidity of the solvent.
The environmental effects on the yield are attributed to radiationless electronic relaxation processes caused by solute-solvent interaction. Increasing the temperature and decreasing the intra-solvent cohesion cause increases in the interaction and therefore accelerate the relaxation. The rate determining step behaves like a diffusion in the limit of low viscosity.     

MIGRATION OF EXCITATION ENERGY FROM THIONINE TO METHYLENE BLUE IN MICELLES

Abstract— The main absorption bands of thionine (Th⁺) and methylene blue (MB⁺) in aqueous solution lie at 598 nm and 664 nm, respectively. This position permits excitation energy transfer from Th⁺ to MB⁺, but not vice versa. We describe here studies of such transfer between these molecules adsorbed on micelles of sodium lauryl sulfate (SLS), imitating, at least to some extent, the state of pigments in chloroplasts.
The SLS concentration was varied from 3.0 to 11 × 10^-3 M. In the presence of dye, aggregation to micelles, each containing 70–100 detergent molecules, begins at about 3.0 × 10^-3 M SLS. Practically all dye ions are adsorbed on these micelles as soon as their formation begins.
Energy transfer from adsorbed Th⁺ ions to adsorbed MB⁺ ions can be demonstrated by observing the quenching of the fluorescence of thionine and the sensitization of that of methylene blue.
At [Th⁺] = [MB⁺] = 1 × 10^-5 M , the most efficient energy transfer (82 per cent efficiency, as derived from measurements of the quenching of Th⁺ fluorescence, or 90 per cent, as derived from sensitization of MB⁺ fluorescence) is observed at the lowest SLS-concentration (3.0 × 10^-3 M ), when the only micelles present are those formed by aggregation of dye-carrying low molecular complexes of SLS with dye cations. Each micelle carries, under these conditions, 10–14 molecules of the two dyes, and the distance between two closest dye ions is about 16 A. Transfer becomes less efficient as the SLS-concentration increases, causing pigment molecules to distribute themselves among a greater number of micelles.     

THE SPECTROSCOPY AND PHOTOCHEMISTRY OF ENAMINONITRILES INCLUDING THE SYNTHESIS AND IDENTIFICATION OF CIS-β-AMINOACRYLONITRILE

Abstract— The absorption spectral and photochemical properties of β-aminoacrylonitrile (AAN), β-aminocrotonitrile (ACN) and three other enaminonitriles have been studied. The synthesis and identification of cis -β-aminoacrylonitrile are also included. Each enaminonitrile has one intense absorption band (1–2 × 10⁴M^-1cm^-1) in the 254–273 nm region. Photoisomerization and photocyclization to imidazoles are observed. Imidazole formation is quite strongly inhibited by oxygen and the presence of oxygen can cause wavelength dependent photochemistry, other reactions and destruction of the reactant. The quantum yield of formation of imidazoles is low (<10^-4) for β-aminoacrylonitrile and β-aminocrotonitrile and photoisomerization dominates in those four cases where it can occur. Imidazole formation from a dimethylamino compound proves that the presence of H atoms on the amino group is not a prerequisite for photocyclization.     

AN ULTRASENSITIVE BIOASSAY FOR THE DETECTION OF FUROCOUMARINS AND OTHER PHOTOSENSITIZING MOLECULES

Abstract— A photobiological assay based upon inhibition of growth in the DNA repair-deficient bacterium E. coli B _s-1, is described for the analysis of a number of photosensitizing agents. The lower limits of detection were as follows: psoralen 5 × 10^-11g; 5-methoxypsoralen 1 × 10^-9 g; 8-methoxypsoralen 1 × 10^-9 g; 4,5',8-trimethylpsoralen 1 × 10-¹¹ g; angelicin 5 × 10^-9 g; 5,7-di-methoxycoumarin 1 × 10^-7 g; isoimperatorin 5 × 10^-9 g; dictamnine 1 × 10^-8 g; oxypeucedanin 5 × 10^-7 g; 5-nitroxanthotoxin 5 × 10^-7 g; and α-terthienyl 1 × 10^-6 g. All active compounds with the exception of α-terthienyl were more easily detected by several orders of magnitude by E. coli B _s-1 than with the normal wild type E. coli. 5—Geranoxypsoralen and isopimpinellin were not active. The application of this technique, after TLC, to the analysis of complex mixtures from lemon oil, oil of bergamot, Heracleum lanatum, Angelica dawsonii , and celery and parsnip is illustrated. The bioassay described is more rapid and sensitive than previously published methods, permits replica plates to be made, and allows tentative identification of the photosensitized molecular target.     

CHEMILUMINESCENCE IN THE PROCESS OF OXIDATIVE RING-OPENING OF PURPUROGALLINQUINONES

Abstract— The oxidation of purpurogalline (PPG) by alkaline solution of H₂O₂ pH 9–11 at 298°K is accompanied by chemiluminescence (CL) in the spectral range 400–600 nm with the maximum at 500 nm and quantum yield about 10^-6. The optimal concentrations of reactants with respect to maximal intensity are: 2 × 10^-4 M PPG, 10^-2 M NaOH, 1 M H₂O₂. Activation energy calculated from the maximum intensity of CL is 8.1×0.4 kcal/mole. Light emission occurs only when OH-groups of the phenolic ring of PPG undergo oxidation and the blue anion of o -PPG-quinone is formed. The rate that determines step in the reaction associated with luminescence is the nucleophilic attack of OOH^- ion on the blue anion of o -PPG-quinone. In this exergonic step (-ΔH = 63 to 230kcal/mole) the o - and/or p -quinone ring is opened and carbonyl derivatives of α-tropolone are produced. They display fluorescence in the region 400–600 nm. The fluorescence spectrum of the reaction mixture after oxidation of PPG is very close to that of CL. It is likely that carbonyl derivatives of α-tropolone are emitters of CL.     

THE INFLUENCE OF MOLECULAR CONFORMATION ON THE STABILITY OF ULTRAVIOLET STABILIZERS TOWARD DIRECT AND DYE-SENSITIZED PHOTOIRRADIATION: THE CASE OF 2-(2'-HYDROXY-5'-METHYPHENYL)BENZOTRIAZOLE (TIN P)

Abstract— The mechanism for photodegradation of the ultraviolet photostabilizer 2-(2'-hydroxy-5'-methylphenyl)benzotriazole (TIN P) upon direct and dye-sensitized (singlet molecular oxygen [O₂(1Δ_g)]-mediated) irradiation was studied. From the experimental TIN P photodegradation rate data, and low temperature (77 K) fluorescence and phosphorescence quantum yields, one can conclude that the photodegradative process involves phosphorescent states of TIN P. The open conformer of TIN P quenches O₂(¹Δ_g) by physical scavenging with a rate constant (k_q) in dimethylsulfoxide of 2.8 times 10⁶ M ^-1 s^-1. The intramolecular hydrogen-bonded conformer does not appreciably interact with O₂(¹Δ_g). In the presence of a relatively high concentration of OH- (either 5 times 10^-2 M KOH in ethanol or water at pH 13), the ionic form of TIN P (with an ionized phenol group) physically and chemically quenches O₂(¹Δ_g). The reaction rate constant ( k _r) is 1 times 10 ⁸ M ^-1 s^-1, and the ratio k _q/ k _r is approximately three in alkaline aqueous media.     

FAR-RED INDUCED, LONG-LIVED AFTERGLOW FROM PHOTOSYNTHETIC CELLS. SIZE OF AFTERGLOW UNIT AND PATHS OF ENERGY ACCUMULATION AND DISSIPATION

Abstract— –Small amounts of N -methyl phenazonium methosulphate (PMS) added to a suspension of Chlorella pyrenoidosa accelerate the emission of the long-lived far-red induced afterglow without greatly changing the amount of light emitted. The effect is noticeable in dilute suspensions at a PMS concentration of 10^-9 M. The concept of afterglow unit is introduced and defined as that part of the sample in which the rate of energy reemission can be controlled by a single molecule of PMS. The number of chlorophyll molecules per afterglow unit is about 10⁵. It is possible that the afterglow unit is identical to the thylakoid.
The rate constant for the final first order decay phase of afterglow at room temperature is about 0.7 min^-1 without PMS and about 3 times larger for a unit with one PMS molecule.
Diuron (DCMU) lowers the rate of afterglow decay. Desaspidin on the other hand decreases the amount of light emitted without affecting the decay rate. Carbonylcyanide- m -chlorophenyl hydrazone (CCCP) decreases the afterglow over the whole time-range and increases the decay rate. A kinetic model is developed to account for the results.     

AN EPR STUDY OF THE SPECIES PRODUCED DURING THE UV PHOTOLYSIS OF HETEROCYCLIC COMPOUNDS IN METHYLTETRAHYDROFURAN AT 77 K

Abstract —The ultraviolet irradiation (290 nm ≤Λ≤ 390 nm) of indole, purine, indazole, acridine and quinoline in 2-methyltetrahydrofuran glass at 77 K produces trapped radicals. Two electron-paramagnetic-resonance (EPR) signals are found at 77 K during illumination, one at high magnetic field (3–25 times 10^-1 T) assigned to the matrix radical and the other at low field (1.3 times 10^-1 to 1–5 times 10^-1 T) attributed to the lowest triplet state of the heterocyclic molecule. Quantum yields for triplet production at 77 K are 0–34 for indole, 0.51 for purine, 0.55 for indazole, 0.15 for acridine, and 0.94 for quinoline. The rate of formation of matrix radicals varies as the n _R^th power of the incident light intensity, I ₀^nR, where 1.6 ≤ n _R=≤ 2. Solvent radical yields, which depend on the light intensity, have been determined. Under the experimental conditions, no signals attributable to trapped electrons or cations have been observed. The dependence of the reciprocal value of the rise lifetime of the low field EPR signal as a function of the intensity of exposure is in accordance with a biphotonic mechanism.     

METHYL VIOLOGEN AGGREGATION

Abstract— Methyl viologen (paraquat, l,l'-dimethyl-4, 4'-bipyridinium dichloride) has been observed to start forming aggregates in methanol at 2.5 times 10^-3 M, and in aqueous solutions at about 10^-2 M depending on other experimental parameters. The number of molecules per aggregate is 2–3 for concentrations < 0.1 M.     

PHOTOINACTIVATION OF CATALASES FROM MAMMAL LIVER, PLANT LEAVES AND BACTERIA. COMPARISON OF INACTIVATION CROSS SECTIONS AND QUANTUM YIELDS AT 406 nm

Abstract— Photoinactivation in vitro at pH 7.0 of catalases from different sources (bovine liver, spinach leaves, and Micrococcus lysodeikticus) was studied. The wavelength of the inactivating light was close to the Soret peak of catalase. No great difference in light sensitivity between soluble catalases were found; the inactivation cross sections found ranged from 3.8.10^-4 to 5.0. 10^-4Ų/molecule. The inactivation quantum yield is 2.2. 10^-5 for bovine liver catalase and 3.110^-5 for Micrococcus catalase. The quantum yield for soluble spinach catalase is of a similar order of magnitude. There are some indications of a greater resistance to photodestruction of the spinach leaf catalase activity associated with small particles.     

PICOSECOND LASER SPECTROSCOPY AND OPTICALLY DETECTED MAGNETIC RESONANCE ON A MODEL PHOTOSYNTHETIC SYSTEM

Fluorescence-detected magnetic resonance of triplets in zero magnetic field (FDMR), fluorescence fading (FF) due to triplet-formation, both at 4.2 K, and prompt fluorescence decay kinetics (FDK) at room temperature have been measured for free pheophorbide- a (f-Pheo) and bound (b-Pheo) to a synthetic polypeptide (L-L ys -L-A la -L-A la )_n, dissolved in dimethylformamide (DMF). Fluorescence decay kinetics measurements of f-Pheo in DMF yielded 1-5 ns lifetimes, for b-Pheo in DMF a ~ 50 ps decay-component was found emitting at 730–750 nm. Zero-field splitting parameters |D| and |E| of the lowest triplet state T₁ were determined from FDMR spectra as (337 and 24) 10^-4 cm^-1 for f-Pheo and (359 and 25) 10^-4 cm^-1 for b-Pheo, both in DMF. Decay rate constants of the three spin levels of T¹ of b-Pheo ( K _x= 1200 50 s^-1, k _y= 440 25 s^-1, k _z= 80 5 s^-1) and relative steady-state populations (N_x= 28 2%, N_y= 47 2%, N_z= 26 2%) determined from FF curves predict a fluorescence decrease at the D–E and D + E FDMR transitions, whereas experimentally a fluorescence increase is observed. The FDMR sign-inversion results from singlet-singlet energy transfer from b-Pheo monomers to their aggregates, followed by fast intersystem crossing to T₁. These results indicate that aggregates are formed by two or more b-Pheo molecules at different positions on the folded polypeptide chain. This situation resembles that in chlorophyll-proteins, containing low-lying traps, resulting from interaction of chromophores with other chromophores and with the protein environment.     

THE NATURAL PHOSPHORESCENCE LIFETIME OF BIACETYL AND BENZIL IN FLUID SOLUTION

Abstract— The quantum yields of phosphorescence and fluorescence and the phosphorescence lifetime have been determined for biacetyl in benzene, p-xylene, n-heptane, and water, and for benzil in n-heptane at 22C. The following values for the fluorescence quantum yield and natural phosphorescence lifetime were obtained: For biacetyl in benzene, 2.7 times 10^-3 and 7.8 msec, in p-xylene, 2.5 times 10^-3 and 10.8 msec, in n-heptane, 2.9 times 10^-3 and 10.8 msec, in water, 1.1 times 10^-3 and 10.0 msec, and for benzil in n-heptane, 1.1 times 10^-3 and 10.4 msec.     

THE AQUEOUS PHOTOLYSIS OF ETHYLENE GLYCOL ADSORBED ON GOETHITE

Abstract— Suspensions of goethite (α-FeOOH) were photolyzed in aerated ethylene glycol-water solutions at pH 6.5, with ultraviolet light in the wavelength range300–400 nm. Under these conditions, formaldehyde and glycolaldehyde were detected as photoproducts. Quantum yields of formaldehyde production ranged from 1.9 7times; 10^-5 to 2.9 × 10^-4 over the ethylene glycol concentration range of 0.002-2.0 mol/ℓ, and gave evidence that the reaction occurred at the goethite surface. Quantum yields of glycolaldehyde were 20% less than those of formaldehyde, and displayed a concentration-dependent relationship with ethylene glycol similar to that of formaldehyde. Immediately after photolysis, Fe²⁺ was measured to be 4.6 × 10^-7 mol/ℓ in an aerated suspension containing 1.3 mol/ℓ ethylene glycol, and 8.5 × 10^-6 mol/ℓ in the corresponding deoxygenated suspension. Glycolaldehyde was not generated in the deoxygenated suspensions. These results are consistent with a mechanism involving the transfer of an electron from an adsorbed ethylene glycol molecule to an excited state of Fe³⁺ (Iron[III]) in the goethite lattice, to produce Fe²⁺ and an organic cation. In a series of reactions involving O₂, FeOOH, and Fe²⁺, the organic cation decomposes to form formaldehyde and the intermediate radicals "OH and" CH₂OH. OH reacts further with ethylene glycol in the presence of O₂ to yield glycolaldehyde. Aqueous photolysis of ethylene glycol sorbed onto goethite is typical of reactions that can occur in the aquatic environment.     

PHOTOCHEMICAL INTERACTIONS BETWEEN NITROXIDE FREE RADICALS AND PHENOTHIAZINES IN SOLUTION

Abstract— Ultraviolet irradiation of photosensitive molecules like phenothiazine derivatives leads to the formation of short lived free radicals which are able to reduce stable nitroxide free radicals generally used as spin labels. The measurement of the electron spin resonance signal decay of nitroxides offers a tool for studying the photochemical reaction of phenothiazine derivatives in solution at room temperature, in a 10^-5 to 10^-2 M concentration range. Analysis of the reaction mechanism shows that the paramagnetic nitroxide is an efficient quencher of the phenothiazine triplet state; this reaction was used to demonstrate the influence of the solvent, quenching by oxygen and the role of the chemical structure of six phenothiazine derivatives on their photoreactivity in solution.     

ACID DEPENDENT FLUORESCENCE QUANTUM YIELD AND TETRAMETHYL- 1,2-DIOXETANE CHEMI-ENERGIZED FLUORESCENCE OF ERGOSTATETRAENONE*

Abstract. –In acidified acetonitrile, ergostatetraenone (E) efficiently quenches the tetramethyl-1,2-dioxetane (TMD) chemiluminescence at 410 nm, with the appearance of a new chemiluminescence at ca. 530 nm due to ergostatetraenone fluorescence. Control experiments exclude energization by triplet acetone and the trivial process (emission and reabsorption), establishing singlet-singlet energy transfer between excited singlet acetone (A) and ground state ergostatetraenone as major pathway. From the kinetics the rate constant for singlet-singlet energy transfer ( K ^ss_A,1,) was estimated to be ca. 10^{1 2}S^-1. The chemiluminescence yield (φ^CL) for the TMD/ergostatetraenone system was determined to be ca. 12 × 10^-8. The fluorescence efficiency of ergostatetraenone (φ) in acidified acetonitrile is a function of acid concentration, ranging between 0.06-0.82. The efficiency of singlet acetone production (α) was found to be 500-fold lower than in neutral medium due to a competing acid-catalysed, dark decomposition of TMD. A 60-fold light enhancement has been established for this binary chemiluminescent system.     

ENERGY CONVERSION IN THE DECAY OF TRIPLET LUMIFLAVIN IN THE PRESENCE OF FERRI- AND FERROCYANIDE

Abstract— Flash photolysis at 450 nm has been used to study the quenching of the excited triplet state of lumiflavin and the transient species formed in subsequent reactions in deaerated phosphate buffer (pH 6.9).
The effect of the presence of ferricyanide on the life time of triplet lumiflavin has been studied. The results suggest an energy transfer reaction without concurrent electron transfer reactions. The rate constant for the process was 2.8 times 10⁹ M ^-1 s^-1. The analogous reaction with ferrocyanide could not be observed because of the efficient electron transfer reaction (δG = -20.6 kcal mol^-1) leading to the formation of the semireduced lumiflavin and ferricyanide. The rate constant for this reaction was 3.3 times 10⁹ M ^-1 s^-1. The semireduced lumiflavin radical was found to disappear in a second order reaction with a rate constant of 1.7 times 10⁹ M ^-1 s^-1. It was found to react with ferricyanide with a rate constant of 0.7 times 10⁹ M ^-1 s^-1.
A model for the various photochemical and photophysical processes involved in the decay and quenching of the lumiflavin triplet state is suggested and discussed.