THE PRODUCTION OF SINGLET MOLECULAR OXYGEN BY ZINC(II) PHTHALOCYANINE IN ETHANOL AND IN UNILAMELLAR VESICLES. CHEMICAL QUENCHING AND PHOSPHORESCENCE STUDIES

Abstract— Zn(II)phthalocyanine (ZnPc) generates O₂(¹Δ_g) with a quantum yield of ca. 0.4 upon photocxcitation at 354 or 600 nm in ethanolic solution as determined by time-resolved phosphorescence studies at 1270 nm and photooxidation experiments using 1,3-diphenylisobenzofuran (DPBF) as substrate. The quantum yield of photooxidation slightly increases upon incorporation of ZnPc into unilamellar liposomes of dipalmitoylphosphatidylcholine. Under our irradiation conditions (600 nm, 18^°C, and short light exposure times), DPBF(5–50 μM) undergoes photooxidation by a pure Type II mechanism; the rate constant for the O₂(¹Δ_g) + DPBF reaction is (1.1 ±0.1) x 10⁹ M^-1 s^_1 in ethanol solution and determined to be about two orders of magnitude smaller when both ZnPc and DPBF are embedded into liposomes.     

BACTERIORHODOPSIN AND THE SENSORY PIGMENT OF THE PHOTOSYSTEM 565 IN HALOBACTERIUM HALOBIUM

Abstract Blocking in vivo synthesis of retinal by addition of nicotine to the culture medium leads to the loss of photobehavior in Halobacterium halobium. Addition of rrans -retinol or frans-retinol₂ (3,4-dehy-droretinol) restores the responses to light decreases in the green-yellow spectral range. Action spectra of the reconstituted retinal- and retinal₂-photosystem show maximal sensitivity at 565 and 580 nm, respectively. Addition of retinol or retinol₂ also restores the formation of bacteriorhodopsin (BR) or bacteriorhodopsin₂ (BR₂= 3,4-dehydroretinal-bacterio-opsin complex). The absorption spectra of BR and BR₂, measured in isolated membranes, as well as in living bacteria, show maxima at 568 nm (BR) and at about 600 nm (BR₂), respectively. Comparison of the action spectrum of the retinal2-containing sensory photosystem with the absorption spectrum of BR₂ suggests that a retinal pigment different from BR is responsible for the photosensory behavior to green-yellow light.     

KINETICS OF PHOTOSYNTHETIC APPARATUS ADAPTATION IN Scenedesmus obliquus TO CHANGE IN IRRADIANCE AND LIGHT QUALITY

Abstract— Cells of the unicellular green alga Scenedesmus obliquus grown under high (20 W m^-2) or low (5 W m^-2) irradiancies of white light show all characteristics of sun or shade plants, respectively. When transferred to alternate light conditions, the cells adapt within 6 h. When cells grown under high irradiance of white light are transferred to red (683 nm) or blue (424 nm) light, they show characteristics similar to cells adapted to low or high irradiancies of white light, respectively. This adaptation to different wavelengths takes about 12 h. The underlying changes in the photosynthetic apparatus are discussed.     

THE FORMATION OF TWO FORMS OF BATHORHODOPSIN AND THEIR OPTICAL PROPERTIES

Abstract— Using two kinds of rhodopsin preparations (digitonin extract and rod outer segments suspension), we measured changes in absorption spectra during the conversion of rhodopsin or isorhodopsin to a photosteady state mixture composed of rhodopsin, isorhodopsin and bathorhodopsin by irradiation with blue light (437 nm) at 77 K and during the reversion of bathorhodopsin to a mixture of rhodopsin and isorhodopsin by irradiation with red light (> 650 nm) at 77 K. The reaction kinetics could be expressed with only one exponential in the former case and with two exponentials in the latter case. These data suggest that both rhodopsin and isorhodopsin are composed of a single molecular species, while bathorhodopsin is composed of two molecular species, designated as bathorhodopsin₁ and bathorhodopsin₂. The absorption spectra of these bathorhodopsin were calculated by two different methods (kinetic method and warming-cooling method). The former was based on the kinetics of the conversion of two forms of bathorhodopsin by irradiation with the red light. The spectra obtained by this method were consistent with those obtained by the warming-cooling method. Bathorhodopsin₁ and bathorhodopsin₂ have Λ_max at 555 and 538 nm, respectively. The two forms of bathorhodopsin are interconvertible in the light, but not in the dark. Thus, we suggest that a rhodopsin molecule in the excited state relaxes to either bathorhodopsin₁ or bathorhodopsin₂ through one of the two parallel pathways.     

FLUENCE-RATE DEPENDENCE OF MONOPHOTONIC REACTIONS OF NUCLEIC ACIDS IN VITRO AND IN VIVO

The Bunsen-Roscoe law, also known as the reciprocity law ( E = f(F) with F = I t ) has only limited validity for monophotonic reactions of nucleic acids. Especially at low fluence rates, the extent of in vitro and in vivo photoreactions of nucleic acids in the far-UV and near-UV range is a function of the fluence and of the fluence rate ( E = f (F;I)). In vitro experiments with poly(dA)poly(dT) clearly show that the far-UV (254 nm) response, indicated by the changes of the ellipticity at 315 nm, does not obey the Bunsen-Roscoe law at low fluence rates in the range between 1 W m^-2 and 20 W m^-2. In vivo experiments with Escherichia coli revealed very similar anomalies. Studying the growth delay after irradiation with far-UV light at 280 nm or near-UV light at 334 nm, we have confirmed the lack of reciprocity in both spectral ranges. The failure of the Bunsen-Roscoe law for the 280 nm and 334 nm UV irradiation effect at low fluence rates was in the range O < I < 40 W m^-2. In both cases reciprocity occurred at higher fluence rates (40 < I < 100 W m^-2).     

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.     

CHEMILUMINESCENCE AND THE FORMATION OF SINGLET OXYGEN IN THE OXIDATION OF CERTAIN POLYPHENOLS AND QUINONES

Abstract— The possibility of ¹O₂ (¹Δ_g) participation in the oxidation of polyphenols and quinones has been investigated in two systems: (1) the system involving autooxidation leading to oxidative polymerization and destruction, and (2) the modified Trautz-Schorigin reaction, i.e. oxidation of polyphenols and HCHO with H₂O₂ in concentrated alkaline solutions. The red band with maximum at 635 nm observed in chemiluminescence of pyrocatechol, adrenaline, pyrogallol, gallic acid, adrenochrome and p -benzoquinone corresponds to the transition 2O₂(¹Δ_g) → 2O₂(³Σ^-_g). Emission bands in the range 475–540 nm arise from the superposition of the 2O₂(¹Δ_g) → 2O₂(³Σ^-_g) transition and radiative deactivation of excited oxidation products. In system (2) chemiluminescence has a broad band from 580 nm beyond 800 nm and much higher intensity than in system (1). Formaldehyde was found to enhance light emission in system (1) by a factor of about 30. The influence of solvents, including D₂O in which ¹O₂ has varying lifetimes, on kinetics of chemiluminescence as well as quenching effect of β-carotene, hydroquinone, cysteine, bilirubin and biliverdin strongly support the involvement of ¹O₂ in the chemiluminescence of both systems.     

THE ROLE OF 4-THIOURIDINE IN LETHAL EFFECTS AND IN DNA BACKBONE BREAKAGE CAUSED BY 334 nm ULTRAVIOLET LIGHT IN Escherichia coli

Strains of Escherichia coli that lack 4-thiouridine (⁴Srd) are killed by monochromatic 334 nm UV light (UV) less efficiently than their wild-type parents, which contain ⁴Srd. Oxygen enhancement ratios (OER) at 10% survival are 3.3 for a strain that possesses ⁴Srd, and 2.6 for one that lacks ⁴Srd. Single-strand breaks in DNA caused by 334 nm UV accumulate more than twice as fast in the wild-type strains than in the strains lacking ⁴Srd. The results suggest that ⁴Srd is an important chromophore in some near-UV lethal effects. The results also suggest that the excitation energy from 334 nm UV light may be passed from RNA to DNA, resulting in single-strand breaks.     

PHOTOBLEACHING OF A CYANINE DYE IN SOLUTION AND IN MEMBRANES

Abstract— N,N'-bis(2-ethyl-1,3-dioxolane)-kryptocyanine (EDKC), a lipophilic dye with a delocalized positive charge, photosensitizes cells to visible irradiation. In phosphate-buffered saline (PBS), EDKC absorbs maximally at 700 nm (ε= 1.2 × 10⁵ M⁻¹ cm⁻¹) and in methanol, the absorption maximum is at 706 nm (ε= 2.3 × 10⁵ M⁻¹ cm⁻¹). EDKC partitions from PBS into small unilamellar liposomes prepared from saturated phospholipids and into membranes prepared from red blood cells (RBC) and binds to human serum albumin (HSA). The EDKC fluorescence maximum red shifts from 713 nm in PBS to 720–725 nm in liposomes and RBC membranes and the fluorescence intensity is enhanced by factors of 14–35 compared to PBS (φ= 0.0046). EDKC is thermally unstable in PBS (T_1/2= 2 h at 1.3 × 10⁻⁵ M EDKC), but stable in methanol. In liposomes and RBC membranes, EDKC is 10 times more stable than in PBS, indicating that it is only partially exposed to the aqueous phase. Quenching of EDKC fluorescence in liposomes and RBC membranes by trinitrobenzene sulfonate also indicates that EDKC is not buried within the membranes. Photodecomposition of EDKC was oxygen-dependent and occurred with a low quantum yield (6.4 × 10⁻⁴ in PBS). Singlet oxygen was not detected upon irradiation of EDKC in membranes or with HSA since the self-sensitized oxidation of EDKC occurred at the same rate in D₂O as in H₂O and was not quenched by sodium azide or histidine.     

ELECTRON TRANSFER FROM CHLOROPHYLL a TO QUINONE IN MONO- AND MULTILAYER ARRAYS

Abstract— Mono- and multilayers of chlorophyll a (Chl a )– lecithin have been prepared on quartz slides, by means of the Blodgett-Langmuir technique, for fluorescence studies. Self-quenching of the Chl a fluorescence has been observed in Chl a -lecithin single layer excited with a laser light at 632.8 nm. The fluorescence yield is reduced by 50% at a concentration of 7 ± 10¹² Chl a molecules cm⁻². Chl a fluorescence quenching, by adding N,N -distearoyl-1,4-diaminoanthraquinone (SAQ), has been studied. in a single layer, in pure Chl a and also at various dilutions of Chl a in lecithin. The results are explained in terms of a dynamic quenching rather than in terms of a permanent complex formation, at the ground state, between Chl a and SAQ. The fluorescence quenching has been interpreted as the result of an electron transfer from excited Chl a to SAQ, and rate constants of 8.3 ± 10⁻⁵ cm² molecule⁻¹ S⁻¹ and 2.4 ± 10⁻⁴ cm² molecule⁻¹ s⁻¹ have been found for pure diluted Chl a , respectively. Ten per cent of the diluted Chl a fluorescence always remains unquenchable and independent of the quinone concentration. In multilayers, where SAQ and Chl a are in different layers, there is no fluorescence quenching for pure or diluted Chl a even when the chromophores are in two adjacent layers. This happens only if SAQ is not able to diffuse from one layer to another. A minimum value of 22.4 nm has been found for the singlet exciton diffusion length in pure Chl a multilayers.     

PROFLAVINE MEDIATED PHOTOINACTIVATION OFBACTERIOPHAGE φX174 AND ITS ISOLATED DNA: EFFECTS OF AGENTS MODIFYING VARIOUS PHOTOCHEMICAL PATHWAYS

Abstract. Thiols and disulfides protect both φX174 phage and its isolated DNA from the lethal action of proflavine plus light. The protective ability of these compounds appears to be attributed to the -SH or the -S-S- group and the property to interact with the proflavine-phage DNA complex. The phage inactivation efficiency per proflavine bound to DNA is reduced by 50 to 30% upon addition of cysteine or cystamine. Substances that affect the lifetime of singlet oxygen modify the rate of phage photoinactivation in the presence of proflavine; the inactivation rate is decreased by N^-₃ and increased by D₂O. Irradiation under N₂ atmosphere markedly decreases the phage photosensitization by proflavine. Irradiation with monochromatic light of 440 nm is less efficient than irradiation with light of 440 nm plus 360 nm, and the difference is more pronounced in N₂ than in air. These results are discussed in relation to various possible photochemical pathways.     

PHOTOVOLTATC EFFICIENCIES OF MICROCRYSTALLINE AND ANHYDROUS CHLOROPHYLL a

Abstract— A thin layer of chlorophyll a (around 2000 Å). a p -type organic semiconductor. was sandwiched between two different metals. aluminum and silver. We used the photovoltaic effect in order to study the efficiency of light conversion by the crystalline and anhydrous forms of Chl a . When the photovoltaic cell is illuminated through the semi-transparent aluminum electrode. an action spectrum similar to the visible absorption spectrum of Chl a is obtained. The anhydrous form. always shows a maximum, in the red, at 672 nm and the crystalline one at 746 nm to 738 nm depending on the amount of water vapor present in the measuring area. The light conversion efficiency has been measured at the maximum absorption in the red for both forms of Chl a . For the anhydrous form, we found values as high as 0.036%, which is very significant even compared to 0.21%, the highest value found for the crystalline form. In both cases. the incident light power was approximately 10 μW on the cell. The light conversion efficiency of both forms of Chl a cells was found to depend on a combine effect of the nature of the gas (O₁. N₂. air. Ar. N₂O. SF ₆ , H₂) and the amount of water vapor present in the measuring area. The best conversion efficiency was obtained with O ₂ , or air saturated with water. This combined effect was very large for the crystalline form whereas the anhydrous form was only slightly affected.     

PHOTOMORPHOGENESIS IN Penicillium isariaeforme: EXOGENOUS CALCIUM SUBSTITUTES FOR LIGHT

Abstract— Penicillium isariaeforme is a photomorphogenic fungus which produces upright bundles of conidia-bearing mycelia (called coremia) when grown on a defined medium in visible (450–500 nm) light. We found that exogenous Ca²⁺ ions could substitute for light. In the dark 1–2 m M Ca²⁺ triggered coremia formation. Dark induction of coremia was specific for Ca²⁺ in that it could not be duplicated by 50 m M Ba²⁺, Fe²⁺, Mg²⁺, Mn²⁺, Sr²⁺, or Zn²⁺. Additionally, light-induced coremia formation was inhibited by both KI (2.5 m M ) and phenylacetic acid (0.25 m M ).     

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.     

CHEMILUMINESCENCE IN THE PEROXIDATION OF TANNIC ACID

Abstract— Peroxidation of tannins with alkaline H₂O₂ is accompanied by weak chemiluminescence in the spectral region 480–800 nm. o-Di and tri-hydroxy groups of polyphenols undergo oxidation by a free-radical mechanism and a green intermediate anion-radical with absorption Δ_max= 600 nm is formed. The radical mechanism is supported by the low activation energy 14–20 kJ/mol and the quenching effect of radical scavengers. The reaction of the green intermediate with peroxy anions is the chemiluminescence rate limiting step. In the presence of a-hydroxy-methylperoxide formed from H₂O₂ and formaldehyde, the alkaline peroxidation of tannins is accompanied by strong red luminescence (420–800 nm). The base catalyzed decomposition of peroxides gives only a weak red emission (460–800 nm). Light intensity is enhanced in D₂O by a factor 6.5. Quenchers of O₂(¹Δ_g) and 1,3-di-phenylisobenzofurane diminish light intensity in non-aqueous solutions. The data suggest ¹O₂ participation in the observed chemiluminescence. Thermo-chemical calculations give —ΔH values from 250–1000 kJ/mol for one elementary reaction step which limits the mechanism of chemi-enereization. Chemiexcitation of tannins is relevant to biochemical mechanisms of aerobic degradation of aromatic compounds, energy utilization as well as to defense and resistance processes in plants.     

LUMINESCENCE AND PHOTOCHEMISTRY OF 4-THIOURIDINE IN AQUEOUS SOLUTION

Abstract— In bidistilled water, 4-thiouridine (4TU) exhibits a weak unusual luminescence, the quantum yield of which is 3 × 10^-4 at 25°C. The excitation spectrum corresponds well to the 4TU absorption spectrum. The emission lies at longer wavelengths (Λ_max 550 nm) than the 4TU phosphorescence observed at 77 K (Λ_max, 470–480 nm). From the emission signal obtained after an excitation flash of 3 ns half-width, an "apparent" rate constant for the radiative deactivation process, shorter than 5 × 10⁶ s, can be inferred. The 300 K emission is efficiently quenched by halides and by oxygen: quenching involves a long-lived intermediate (⋍ 200 ns).
Clearly the emissive state X is populated through the S₀-S₁ electronic transition π→π* of 4TU. The nature of X cannot be unambiguously determined: it cannot be an excimer but can be either the 4TU triplet state or another chemical state distinct from the 4TU excited singlet or triplet states.
An interesting finding is that the 300 K emission and the ability of 4TU to photoreact are related: they are quenched with the same efficiency by halide anions. This indicates that quenching occurs at the same long-lived intermediate species , which is either a precursor of the emitter or the emitter itself.     

COMPARATIVE ANALYSES OF ACTION SPECTRA OF GLYCOLATE EXCRETION ("PHOTORESPIRATION") AND PHOTOSYNTHESIS IN THE BLUE-GREEN ALGA AN ACYSTIS NIDULANS

Abstract. The action spectra were determined by measuring photosynthetic H¹⁴CO^-₃-fixation and ¹⁴C-glycolate excretion to the medium during 15 min exposure to light at 15 different wavelengths in the visible region using interference filters and a 2500 W high pressure Xe lamp at a constant photon flux of about 1.51 × 10¹⁹ quanta m^-2.s^-1 at all wavelengths.
When plotted on relative scales the action spectrum of glycolate excretion lies below that of photosynthesis at all wavelengths shorter than 517 nm. As glycolate excretion had an exponential relationship to photosynthetic rates, different methods were used to analyze for a specific blue light effect which demonstrated that the relative amount of glycolate excretion was depressed by blue light compared with that by green and red. The greatest difference was observed around 460–480 nm. However, on statistical grounds it is not permitted to draw a difference spectrum which might indicate the absorption characteristics of pigment(s) involved.
A hypothesis is discussed assuming that some glycolate is consumed in an oxidation process for supply of electrons to Photosystem I when Photosystem II is poorly excited in the blue region of the spectrum, which was the case for Anacystis used in the present investigation.     

EFFECT OF INTENSITY AND WAVELENGTH OF FLUORESCENT LIGHT ON CHROMOSOME DAMAGE IN CULTURED MOUSE CELLS

Abstract—A single 3- to 20-hr exposure of line NCTC 9266 mouse cells to cool-white fluorescent light (4.6 W/m²) produces chromatid breaks and exchanges. The effective wavelength is in the visible range and coincides with the mercury emission peak at 405 nm. Increasing light intensity from 4.6 W to 15.3 W/m² for 20 h causes a concomitant increase both in production of chromosome damage and formation of hydrogen peroxide (H₂O₂) in the serum-free medium. Cells washed free of medium and illuminated in saline for 3 h show chromosome damage to the same extent as cells illuminated in culture medium. Addition of catalase during the exposure period of 3 h eliminates the light-induced damage. We conclude that the light-induced chromatid breaks and exchanges result from H₂O₂ production within the cell and that exogenous catalase can enter the cell and prevent the damage.     

AN EXPERIMENTAL STUDY OF THE CHANGES IN PIGMENTATION IN HUMAN SKIN IN VIVO WITH VISIBLE AND NEAR INFRARED LIGHT

Abstract— The skin of the lower inner arm of volunteers was irradiated, with a 390–1700 nm light source, through a fiber optic bundle for times of up to 1.2 × 10⁴ s and with powers of up to 0.35 W/cm². Simultaneously with the irradiation, spectra (390–720 nm) of the remitted intensity were measured, while a 5.0 cm in diameter area of the skin around the fiber bundle was maintained at constant temperature, within 0.2°C. The generation of a photoproduct was observed and measured as changes in the remitted intensity within 600 s (10 min) of the start of irradiation.
The photoproduct formed was characterized by a weak absorption in the blue part of the spectrum (400–450 nm), leading to a bluish appearance in the irradiated area only. The color change appears as a two step process. It starts with a "soluble" photoproduct, which disappears, within 24 h after irradiation, and an "insoluble" photoproduct which appears with irradiation greater than 3 ×10³ s (50 min). No spectral differences were detected between the two photoproducts. The "insoluble" photoproduct persists for periods of up to 8 weeks. The color change in the skin is immediate and there is no erythema associated with this color change.     

THE EFFECT OF IRRADIANCE ON VIRUS STERILIZATION AND PHOTODYNAMIC DAMAGE IN RED BLOOD CELLS SENSITIZED BY PHTHALOCYANINES

Abstract— Phthalocyanines are being studied as photosensitizers for virus sterilization of red blood cells (RBC). During optimization of the reaction conditions, we observed a marked effect of the irradiance on production of RBC damage. Using a broad-band light source (600–700 nm) between 5 and 80 mW/ cm², there was an inverse relationship between irradiance and rate of photohemolysis. This effect was observed with aluminum sulfonated phthalocyanine (AlPcS_n) and cationic silicon (HOSiPc-OSi[CH₃]₂ [CH₂]₃N⁺[CH₃]₃I^- phthalocyanine (Pc5) photosensitizers. The same effect occurred when the reduction of RBC negative surface charges was used as an endpoint. Under the same treatment conditions, vesicular stomatitis virus inactivation rate was unaffected by changes in the irradiance. Reduction in oxygen availability for the photochemical reaction at high irradiance could explain the effect. However, theoretical estimates suggest that oxygen depletion is minimal under our conditions. In addition, because the rate of photohemolysis at 80 mW/cm² was not increased when irradiations were carried out under an oxygen atmosphere this seems unlikely. Likewise, formation of singlet oxygen dimoles at high irradiances does not appear to be involved because the effect was unchanged when light exposure was in D₂O. While there is no ready explanation for this irradiance effect, it could be used to increase the safety margin of RBC virucidal treatment by employing exposure at high irradiance, thus minimizing the damage to RBC.