DESIGN AND PERFORMANCE OF THE OKAZAKI LARGE SPECTROGRAPH FOR PHOTOBIOLOGICAL RESEARCH

A computer-operated spectrograph was recently built at Okazaki, Japan. Different specimens can be placed on a horseshoe-shaped focal curve (10 m long) covering a wavelength range of 250 to 1000 nm so they can be irradiated simultaneously. The linear dispersion is about 0.8 nm/cm. The photon fluence rate on the focal curve is 5 x 10¹⁵. photons x cm^-2 x s^-1 at 300nm and 1 x 10¹⁶ photons x cm^-2 x s^-1 at 600 and at 900 nm. The spectral half width is 5.5 nm or less on the focal curve. The stray light content is about 10^-5 of the main peak at the peak wavelength ± 100 nm. Specimens are set in microcomputer-controlled threshold boxes so that wavelengths, photon fluence rates, photon fluences and timing of irradiations are controlled automatically according to a pre-programmed schedule. An optical fiber system is also provided for remote irradiations.     

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.     

DETECTION OF THE EXCITED SINGLET STATE OF A DEPROTONATED, REDUCED FLAVIN

Abstract— The excited singlet state of a deprotonated, reduced flavin [1, 5-dihydro- N (3)-carboxymethyllumiflavin] in aqueous solution at pH 8 has been detected by laser flash photolysis. The broad absorption band maximized at ∼ 490 nm (ε= 9.9 × 10³ M ^-1 cm^-1). The lifetime of the transient was found to be 100 ± 15 ps. The lifetime was not affected by the presence of pyrimidine dimers, which would be monomerized under these conditions. A longer-lived transient, tentatively identified as the solvated electron, was also detected. The neutral reduced flavin did not give a detectable transient.     

AGREGATION DES CHLOROPHYLLES IN VITRO-II. PHOTODECOLORATION DE LA CHLOROPHYLLE a ADSORBEE SUR DES PARTICULES DE LIPOPROTEINES EXTRAITES DU LAIT

Abstract— Chlorophyll a (chl a ) adsorbed on milk proteins or lipoproteins has absorption maxima at 437 ± 1 nm and 671 ± 1 nm, whatever its concentration. A 750-nm-absorbing form appears when (chl/proteins) > 2 × 10^-2 mg chl/mg proteins, in the case of lipoproteins; or 4.5 × 10^-3 mg chl/mg proteins, in the case of proteins. In both cases, the apparent molar extinction coefficient at 671 nm is the same (3 × 10⁴ liter mole^-1 cm^-1) at the highest (chl/proteins) ratio for which no 750 nm absorbancy appears. It is shown that adsorbed chl a undergoes irreversible (in the present conditions) photo-oxidation by light in the presence of oxygen. The reaction is second order, with similar rate constants for chl a adsorbed to proteins or to lipoproteins.     

ACTINOMETRY IN MONOCHROMATIC FLASH PHOTOLYSIS: THE EXTINCTION COEFFICIENT OF TRIPLET BENZOPHENONE AND QUANTUM YIELD OF TRIPLET ZINC TETRAPHENYL PORPHYRIN

Abstract— The extinction coefficient ε_T, of triplet benzophenone in benzene has been directly determined by absolute measurements of absorbed energy and triplet absorbance, Δ D ⁰_T, under demonstrably linear conditions where incident excitation energy, E ₀, and ground state absorbance, A ₀, are both extrapolated to zero. The result, 7220 ± 320 M ^-1 cm^-1 at 530 nm, validates and slightly corrects many measurements relative to benzophenone of triplet extinction coefficients made by the energy transfer technique, and of triplet yields obtained by the comparative method.
As E ₀ and A ₀ both decrease, Δ D ⁰_T becomes proportional to their product. In this situation, the ratio R = (1/ A ₀)(dΔ D ⁰_T/d E ₀) = (ε_T - ε_G)φ_T. Measurements of R , referred to benzophenone, give (ε_T - ε_G)φ_T for any substance, without necessity for absolute energy calibration.
Both absolute and relative laser flash measurements on zinc tetraphenyl porphyrin (ε_T - ε_G at 470 nm = 7.3 × 10⁴ M ^-1 cm^-1) give φ_T= 0.83 ± 0.04.     

LASER PHOTOLYSIS OF THE PURPLE MEMBRANE OF Halobacterium halobium IN THE PHOTOSTATIONARY STATE: THE PHOTOBRANCHING PROCESS FROM THE O640 INTERMEDIATE

Abstract The photobranching process from the O₆₄₀ intermediate (O) in the photocycle of bacteriorhodopsin was studied. The O form accumulated with continuous wave visible light (390–800 nm) irradiation of the acidic (pH 3.9–6.0) purple membrane of Halobacterium halobium at 22°C. The photocycle of O via an L-like (or N-like) intermediate was driven by 630 nm pulsed light. The newly found intermediate has an absorption band in the 450–560 nm region. The "green-light"-absorbing pigment, tentatively called G₅₂₀, was converted to O with a time constant of (1.2 ± 0.2) ms. No M-like species was found in the cycle. The quantum yield of the cycle was estimated to be 0.30 ± 0.15.     

QUANTUM EFFICIENCY AND PHOTOSENSITIVITY OF THE RHODOPSIN ⇌ METARHODOPSIN CONVERSION IN CRAYFISH PHOTORECEPTORS

Photosensitivity (K_λ) of a visual pigment is the product of the molecular absorption coefficient (α_λ) and the quantum efficiency for photoconversion (γ). Among the invertebrates, many visual pigments are stable not only in the rhodopsin (R) conformation but also as the photoproduct, metarhodopsin (M), We here employ a method for determining the photosensitivities of the two stable pigments of a rhodopsin-metarhodopsin pair, using kinetic analysis of fluorescence from metarhodopsin combined with measurements of spectral absorption made before and after saturation at the isosbestic wavelength of the pigment pair. A curve fitting technique, in which a theoretical function is scaled for best fit to the measured absorption spectrum of the photosteady-state mixture, yields values for the photosensitivity of rhodopsin at λ._max, the ratio of quantum efficiencies for rhodopsin—metarhodopsin interconversion, and the fractional composition of the steady-state mixture. With knowledge of the molecular extinction coefficient, the absolute values of quantum efficiency can be calculated. For crayfish ( Orconectes, Procambarus ) rhodopsin, measured in isolated rhabdoms, K_max= 1.05 x 10^-16 cm² at 535 nm with >7λR→M0.69. These values are similar to the photosensitivity and quantum efficiency of bleaching of vertebrate rhodopsins in digitonin solution (Dartnall, 1972). For the metarhodopsin, K_max= 1.02 x 10^-16 cm² at 510 nm, and λ_M-R= 0.49.     

THE CHARACTERISATION OF THE TRIPLET STATE OF CROCETIN, A WATER SOLUBLE CAROTENOID, BY NANOSECOND LASER FLASH PHOTOLYSES

Abstract— The triplet state of crocetin, which is a water soluble carotenoid, has been sensitized by psoralen. The triplet extinction coefficient, ε_T (73000 dm³ mol^-1 cm^-1 at 470 nm), the triplet-triplet spectrum and the quantum yield of triplet formation, φ_T (less than 1%) are reported in aqueous solution.
In order to calculate the extinction coefficient of crocetin it was necessary to obtain ε_T for psoralen in water (10000dm³ mol^-1 cm^-1 at 450 nm). This latter value was obtained using the complete conversion technique and is reported with the triplet-triplet spectrum.     

THE PHOTOMOVEMENT OF Caenorhabditis elegans, A NEMATODE WHICH LACKS OCELLI. PROOF THAT THE RESPONSE IS TO LIGHT NOT RADIANT HEATING

Abstract— Caenorhabditis elegans adults were tested at constant temperature with 10 s periods of monochromatic light alternated with 20 s dark periods. Stimuli at effective intensities and wavelengths caused an increase in the frequency of ecclitic (phobic, avoidance) responses, which was measured as an increase in the probability of a temporary reversal in direction of movement. For monochromatic stimuli ranging from 420 to 680 nm at a constant 56 picoeinsteins s^-1 cm^-2, only those at520–600 nm elicited significant responses. At 540 nm the threshold fluence rate was approximately 30 pE s^-1 cm^-2. At saturating intensities the mean reversal probability was increased to 0.20 in 10 s from a background level of 0.12. approximately.
Because C. elegans lacks ocelli and is very sensitive to temperature, possible sources of radiant heating were considered in detail, including (a) infrared present in the stimuli, (b) absorption of light by the arena, and (c) absorption of light by a nematode pigment. All possible sources were found to cause a negligible temperature rise, on the order of or less than the natural temperature fluctuations inside the worm, 1.5 times 10^-6°C. A 2 times 10^-4°C temperature rise produced by a 1230 nm infrared stimulus had no significant effect on reversal frequency. It was concluded that the response to illumination must have been to light, and not to temperature changes.
Large, + or - 2 °C changes from the acclimation temperature caused significant increases in the background frequency of ecclitic responses (a thermoecclisis or thermoklinokinesis). However, neither the threshold nor the saturation level of light-induced responses was affected by the ± 2°C changes.     

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.     

MECHANISMS OF THE PHOTOSENSITIZED OXIDATION OF TYRAMINE

Abstract— …According to the criteria of enhancement in D₂O and inhibition by sodium azide, the oxidation of tyramine photosensitized by methylene blue is largely a singlet oxygen or Type II process. Its quantum yield approximates 0.3 in D₂O at pH 10. There is a less efficient reaction not quenched by azide, which is assigned to a dye-substrate or Type I process. It gives rise to products with distinct bands at 320 and 285nm. Products of the Type I reaction are further oxidized by singlet oxygen and thereby compete with tyramine for this reagent. Kinetic parameters were estimated by computer simulation of the dependence of quantum yield on extent of reaction. The rate constant for reaction of O₂ (¹Δ_g) with tyramine was estimated to be 2.8 × 10⁸ M ^-1 s ^-1± 20% at pH 10. The reaction was also sensitized by hypericin in what appears to be a Type II process.     

ACTION SPECTRA FOR PHOTOTROPIC BALANCE IN Phycomyces blakesleeanus: DEPENDENCE ON REFERENCE WAVELENGTH and INTENSITY RANGE

Abstract— Action spectra for phototropic balance of Phycomyces blakesleeanus sporangiophores were measured for various reference wavelengths and intensity ranges. Balance action spectra were made at fluence rates of 10^-4 W m^-2 with reference wavelengths of 450 nm, 394 nm, 507 nm, and broadband blue light. For broad-blue light and 450 nm light as references, typical flavin-like action spectra were found with a ma jor peak at 455 nm, a secondary peak at 477 nm, and a minor peak at 383 nm; these peaks are wider for broad blue than for 450 nm light. With the 394 nm reference, there is a major peak at 455 nm, a secondary peak at 477 nm and a minor peak at 394 nm. An action spectrum with 507 nm reference has a major peak at 455 nm and a minor peak at 383 nm, but no peak at 477 nm. A balance action spectrum was made with 450 nm reference light near threshold intensity (2 times 10^-8 W m^-2); there, the 386 nm peak is greatly reduced, while the 455 nm peak is enhanced. The intensity dependence of the 386 nm peak was studied in detail for reference light of 450 nm. We found that the relative quantum efficiency of the 386 nm light increases with the logarithm of the 450 nm fluence rate; in the high intensity range (0.3 W m^-2) the relative quantum efficiency of the 386 nm light is 1.3 and approaches zero at 10^-9 W m^-2. These findings indicate that P. blakesleeanus phototropism is mediated by multiple interacting pigments or by a photochromic photoreceptor.     

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.     

ULTRAVIOLET RESONANCE RAMAN STUDY ON PURPLE AND BLUE MEMBRANES OF Halobacterium halobium

Abstract— Two hundred and forty and 213 nm excited resonance Raman spectra of purple membrane (PM) and blue membrane (BM) of Halobacterium halobiurn were studied. Generally intense Trp scattering and a strong relative intensity of the W3 band at 1553 cm^-1 in the 240 nm spectrum of PM indicate red-shifted B_b absorptions of some Trp sidechains. A high intensity ratio of Trp doublet at 1360 and 1340 cm^-1 suggests interactions with highly hydrophobic Trp environments. These Trp are not strongly H-bonded and their N₁ sites are located in positions easily reached by solvent water molecules. Tyrosines are also in very hydrophobic environments and H-bonded. The mainchain consists of normal and distorted α-helices whose amide NH are hardly deuterated in D₂O suspension, and some NH exchangeable irregular segments on the membrane surface. Upon acidification, the ratio of Trp doublet with 240 nm excitation decreases concomitant with increase in retinal absorbance at 600 nm, and the W3 relative intensity and overall Trp scattering also decrease. These observations strongly indicate that the counterpart of Trp interactions in PM is the retinal and that the interactions partly diminish upon acidification. The Tyr environment also changes with the color. Although the 240 nm amide I intensity is greater in acid BM than in PM, the change is not related to the color change because the amide I intensity of deionized BM is practically the same as that of PM. The amide I intensity increase in acid BM is ascribable to a structural change of the surface peptides due to acid induced aggregation.     

REGENERATION OF BLUE AND PURPLE MEMBRANES FROM DEIONIZED BLEACHED MEMBRANES OF Halobacterium halobium

Abstract— Bleached purple membrane normally binds Ca²⁺ and Mg²⁺, which can be removed by the divalent cation chelator ethylenediaminetetraacetic acid (EDTA). Regeneration of pigments from EDTA-treated bleached membrane (apomembrane) and retinal leads to the formation of blue membrane at pH 4.8, and purple membrane at neutral pH. The pigments take much longer to regenerate than with un-deionized apoprotein. Adding back cations to the deionized apomembrane only partially speeds up the regeneration process. Like native purple membrane, the regenerated purple membrane also undergoes a photocycle and shows a light-induced proton release and uptake, although with much slower kinetics than the native species. Thus, cations control the kinetics of pigment regeneration, and also some aspects of the pigment's conformation which controls the photocycle kinetics. The removal and replacement of the cations is not completely reversible, suggesting the cations are not merely bound in the double layer.     

THE PHOTOCHEMICAL INTERACTION BETWEEN THE TRIPLET STATE OF 8-METHOXYPSORALEN AND THE MELANIN PRECURSORL–3, 4 DIHYDROXYPHENYLALANINE

Abstract— The photochemical interaction between 8-methoxypsoralen (8-MOP) and the melanin precursorL–3,4-dihydroxyphenylalanine(dopaH₂) has been studied using laser flash photolysis. Triplet excited 8-MOP was thus found to abstract electrons from dopaH₂ ( k ∼ 2 × 10⁹ dm³ mol^-1 s^-1) to form semireduced 8-MOP and semioxidised dopaH₂.The technique of pulse radiolysis was used to establish separately the spectra of (a) the semi-reduced form of 8-MOP at pH 6.5 and (b) the semioxidised forms of dopaH₂ at pH 6.5, 5.8, 4.6 and 3.3. The corresponding λ_max and extinction coefficients found were: for 8-MOP at pH 6.5, λ_max= 350 nm (= 9050 dm³ mol^-1 cm^-1); for dopa at pH 6.5, λ_max= 305 nm (ε= 12000 dm³ mol^-1 cm^-1) and for dopaH at pH 3.3, λ= 305 nm (ε= 5900 dm³ mol^-1 cm^-1).     

ON THE PRIMARY PHOTOPROCESS OF 124-kdalton PHYTOCHROME

The photoreaction between P_τ and the first detectable intermediate, lumi-R, of 124-kdalton oat phytochrome has been investigated at low temperatures. The temperature dependence of the quantum yields of the photoreactions, P_τ to lumi-R and lumi-R to P_τ, has been determined. From measurements over a temperature range from 119 to 155 K, an activation barrier of 3.6 ± 0.5 kJ mol ₁ is found for the photoreaction of P_τ with 661-nm actinic light. A higher value (5.7 ± 0.7 kJ mol ^-1) is found for the photoreaction of lumi-R to P^τ. with 698-nm actinic light. Increased quantum yields are found in deuterated buffer solutions at low temperatures. The activation energies for deuterated phytochrome (3.2 ± 0.7 kJ mol^–1 for P_τ with 661-nm irradiation and 6.2 ± 1.2 kJ mol^-1 for lumi-R at 698-nm irradiation) are identical within the limits of error with those of protonated phytochrome. The lack of a deuterium effect for the activation energies favors the Z,E-isomerization rather than proton transfer or tautomerization for the chromophore photochemistry during P_τ⇄lumi-R conversion.     

STUDIES ON THE INTERRELATIONSHIP AMONG THE INTENSITY OF A RAMAN MARKER BAND OF CAROTENOIDS, POLYENE CHAIN STRUCTURE, AND EFFICIENCY OF THE ENERGY TRANSFER FROM CAROTENOIDS TO BACTERIOCHLOROPHYLL IN PHOTOSYNTHETIC BACTERIA

Abstract Resonance Raman spectroscopy was used to study the polyene-chain structure of carotenoids in light-harvesting pigment-protein complexes from purple photosynthetic bacteria. When major carotenoids of Rhodobacter sphaeroides were incorporated into the light-harvesting complexes of Chromatium vinosum , they showed a relatively intense Raman band at 965 cm^-1 arising from the CH out-of-plane wagging modes of the polyene chain. This result was almost the same as that for the intrinsic carotenoids in Chromatium vinosum , but completely different from that for the intrinsic carotenoids in Rhodobacter sphaeroides . On the other hand, the intrinsic carotenoids of Chromatium vinosum lost the intensity of the 965 cm^-1 Raman band upon protein denaturation. These results support the view that the intensity of the 965 cm^-1 Raman band reflects distortion of the polyene chain, independent of its chemical structure. The polyene-chain distortion is affected by the apoprotein to which carotenoids are bound. The distortion of the polyene chain is correlated with a decrease in the efficiency of the energy transfer from carotenoids to bacteriochlorophyll.     

INVOLVEMENT OF SINGLET OXYGEN IN THE PHOTOTOXICITY MECHANISM FOR A METABOLITE OF PIROXICAM

It has been previously shown that a metabolite of piroxicam but not piroxicam itself causes phototoxicity to cells in vitro after exposure to UVA (320–400 nm) radiation. The phototoxicity mechanism for this metabolite, 2-methyl-4-oxo-2H-l,2-benzothiazine-l,l-dioxide (Compound I), was investigated. In vitro phototoxicity to human mononuclear cells was assayed using 0.5 m M Compound I and UVA radiation. The UVA fluence required for phototoxicity of Compound I was lower by a factor of 2-3 in D₂O buffer compared to H₂O buffer. Superoxide dismutase and mannitol, which remove O₂^- and OH", respectively, do not decrease the phototoxicity. The photodecomposition of Compound I was inhibited by sodium azide, enhanced by human serum albumin and unaffected by mannitol. Stable photoproducts of Compound I were not toxic to the cells. The quantum yield of singlet oxygen based on its emission at 1270 nm was 0.19 and 0.35 for Compound I and s2 ± 10^-3 and 10^-2 for piroxicam in D₂O and C₆H₆, respectively. While the extremely low quantum yield for singlet oxygen from piroxicam appears to account for its lack of phototoxicity, the phototoxicity mechanism for its metabolite, Compound I, most likely does involve singlet oxygen.     

LASER FLASH PHOTOLYSIS STUDIES OF DNA-COMPLEXED ETHIDIUM BROMIDE

Abstract— Laser flash photolysis studies of DNA-complexed ethidium bromide were undertaken. We have observed a singlet-singlet (S₁-S_n) absorption process for DNA-complexed ethidium bromide. The observed lowest singlet excited state lifetime was 21 ± 2 ns. The molar difference extinction coefficient was measured to be 2.4 ± 0.4 × 10³M^-1 cm^-1 at 370 nm. The assignment of this transition was confirmed by time resolved fluorescence measurements.