THE DOSE RESPONSE CURVE IN PHYTOCHROME-MEDIATED ANTHOCYANIN SYNTHESIS IN THE MUSTARD SEEDLING

Abstract —The dose response curve for light (phytochrome)-induced anthocyanin synthesis was determined in the mustard seedling. The curve gives the amount of anthocyanin (A) synthesized within 24 h as a function of the amount of P_fr* produced by a brief light pulse. The [P_fr] response curve is composed of two linear parts with very different slopes ( a _1,2) connected by a relatively narrow transient range (curved segment). The [P_fr] response curve extrapolates precisely through zero [P_fr]. The reciprocity law is valid over the whole range investigated (up to 320 s of irradiation). It is concluded that the initial (or primary) reaction of P_fr (P_fr+ X → P_frX) does not involve any significant cooperativity in the case of phytochrome-mediated anthocyanin synthesis. It is speculated that the linear parts of the [P_fr] response curve truly reflect the mode of phytochrome action ( A = a _1,2 [P_fr]; X does not come into play since it is not rate limiting) whereas the curved segment represents a transition of the reaction matrix of P_fr. The large difference between a₁ and a₂ seems to indicate that the physiological effectiveness of a given amount of P_fr (or P_frX) is determined by [P_fr] through a P_fr-induced change in the reaction matrix.     

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 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.     

INTERACTIONS AMONG PHOTOSYNTHETIC ANTENNA EXCITED STATES

Abstract. The data of Kung and DeVault (1978) showing high-order fluorescence from chromatophores of photosynthetic bacteria are analyzed in relation to other data on first-order fluorescence of photosynthetic systems, particularly that of Monger and Parson (1977). The wavelengths of emission observed (down to 445 nm) require energy equivalent to two lowest singlet-excited states. The dependence on excitation intensity is best explained by any of the following third-order processes: (a) 3 S ₁→3 S ₀; (b) 2 S ₁+ T , → 2 S ₀+ T ₁; (c) S ₁+ 2 T ₁→ 3 S ₀. However, (c) is ruled out because it predicts heavy T ₁-destruction which is not observed. Contribution from the second order process: 2 S ₁→ S ₀ is probable, but even the data of Monger and Parson show that it is insufficient by itself. Two-photon absorption: S ₀+ hv ₁→ S ₁; S ₁+ hv ₁→ S _n; S _n S ₀+ hv ₂ could also account for the high-order fluorescence and its dependence on excitation intensity. [ S ₀, S ₁ S _n are ground, first excited and a higher excited singlet states, respectively, of antenna bacteriochlorophyll, T _t is the lowest triplet state, c/v , is the exciting wavelength (694 or 868 nm) and c/v ₂ the wavelength of the high-order fluorescence (445, 535. or 600 nm), where c = velocity of light.] Maximum values are estimated for some of the rate constants.     

CONCENTRATION-DEPENDENT LIFETIMES OF Cu(NN)+2 SYSTEMS: EXCIPLEX QUENCHING FROM THE ION PAIR STATE

Abstract— The concentration dependence of the lifetimes of the charge transfer excited states of Cu(dmp)⁺₂ and Cu(dpp) ⁺₂ has been investigated in CH₂C1₂ solution at 20^°C. (dmp denotes 2,9-dimethyf-1,10-phenanthroline, and dpp denotes 2,9-diphenyl-l,10-phenanthroline.) In dilute solution (< 30 μM) the lifetime of Cu(dmp)⁺₂, is 95 ± 5 ns, independent of the anion. At higher concentrations the lifetime decreases, in most cases, to a limiting value that depends upon the counterion. The measured limiting lifetimes range from 38 ± 3 ns for CIO^-₄ to 78 ± 5 ns for PF^-₆. The anion-induced quenching is attributed to exciplex quenching which is mediated by an ion pair which exists in the ground state. The results imply that the quenching ability of the anions follows the order BPh-₄ < PF -₆, < BF-₄ < CIO -₄ < NO-₃ which is consistent with previous estimates of donor strength. The lifetime of Cu(dpp)⁺₂ is also concentration dependent, but the effect is much smaller because the phenyl substituents impede attack by the anion.     

HO2 ELIMINATION FROM α-HYDROXYALKYLPEROXYL RADICALS IN AQUEOUS SOLUTION

Abstract— In aqueous solutions α-hydroxyalkylperoxyl radicals undergo a spontaneous and a base catalysed HO₂ elimination. From kinetic deuterium isotope effects, temperature dependence, and the influence of solvent polarity it was concluded that the spontaneous reaction occurs via an HO₂ elimination followed by the dissociation of the latter into H⁺ and O₂^-. The rate constant of the spontaneous HO₂ elimination increases with increasing methyl substitution in α-position ( k (CH₂(OH)O₂) < 10s^-1 k (CH₃CH(OH)O₂) = 52s^-1 k ((CH₃)₂C(OH)O₂) = 665 s^-1). The OH^- catalysed reaction is somewhat below diffusion controlled. The mixture of peroxyl radicals derived from polyhydric alcohols eliminate HO₂ at two different rates. Possible reasons for this behaviour are discussed. The mixture of the six peroxyl radicals derived from d -glucose are observed to eliminate HO₂ with at least three different rates. The fastest rate is attributed to the HO₂ elimination from the peroxyl radical at C-l ( k > 7000s^-1). Because of the HO₂ eliminations the peroxyl radicals derived from d -glucose do not undergo a chain reaction in contrast to peroxyl radicals not containing an α-OH group. In competition with the first order elimination reactions the α-hydroxylalkylperoxyl radicals undergo a bimolecular decay. These reactions are briefly discussed.     

MECHANISMS OF PHOTOELIMINATION REACTIONS OF ALKYL BENZOHYDROXAMATES

Abstract— Photolysis at 254 nm of alkyl benzohydroxamates [C, H, CONHOR: R = CH₃ H₂CH₃ CH(CH₃)₂, CH₂C₆H₅ CH(CH₃)C₂H₅ CH(CH₃)- n -C₆H₁₃] in acetonitrile or hydrocarbon solvents gives benzamide. These reactions can be sensitized by benzophenone (at ca. 350 nm) and are quenched by cis-piperylene. Racemization occurred when 2-octyl (+)-benzohydroxamate was irradiated in cyclohexane. These results are consistent with a mechanism involving a triplet biradical. Photolysis of phenyl benzohydroxamate [C₆H₅CONHOC₆H₅] and benzyl N -methylbenzohydroxamate [C₆H₅CON-(CH₃)OCH₂Q₆H₅] cannot be quenched with ris-piperylene and appear to be singlet reactions.     

MECHANISM OF THE PHOTOCHEMICAL REACTION OF DIPHENYLAMINES WITH CARBON TETRACHLORIDE

Abstract. The quantum yields of HCI (φ_HC1) formation have been measured for the photolysis of N -methyldiphenylamine (MeDPA), triphenylamine (TPA) and diphenylamine (DPA) in the presence of CCl₄ in polar solvents. The quantum yields of N-methylcarbazole formation (φ_mφca) have also been determined for the system MeDPA-CCl₄. With increasing CCl₄ concentration, φ_HCl increases as φ_MeCA decreases, and φ_HCl reaches maximum values 2.7 at 1 M CCl₄. Using laser photolysis, transient spectra have been recorded for MeDPA in the absence and presence of CCl₄ in polar and non-polar solvents, and for TPA. Transient absorption due to the triplet states and photocyclization products (without CCU), exciplexes, the (C₆H₅)₂ NCHi radical, the MeDPA⁺ cation radical, the (TPA⁺., CCl₄) ion pair, and the TPA⁺ cation radical have been identified. The mechanistic implications of these results are discussed.     

A LASER FLASH PHOTOLYSIS STUDY OF PYRENE-1-ALDEHYDE. INTERSYSTEM CROSSING EFFICIENCY, PHOTOREACTIVITY AND TRIPLET STATE PROPERTIES IN VARIOUS SOLVENTS

Abstract— Triplet-and singlet-related photoprocesses of pyrene-1-aldehyde (PA) in various solvents have been investigated in detail using 337.1 and 355 nm laser flash photolysis in conjunction with time-correlated determination of fluorescence lifetimes (τ_F) and steady-state photochemical and absorption-emission spectral measurements. In benzene, the lowest triplet of PA (43 < E_T < 46 kcal/mol) has a lifetime of about 50 µs (τ_T) and displays the absorption maximum at 443 nm with a maximum extinction coefficient (ε_max) of 21000 M ^-1cm^-1; the corresponding ketyl radical has a sharp absorption maximum at 428 nm (ε_max≥ 25000 M ^-1cm^-1). The quantum yields (φ_T) of lowest triplet occupation are high in nonprotic solvents (0.6–0.8), decrease in protic solvents (alcohols) as the polarity of the latter is increased, and maintain a complementary relationship with the quantum yields (φ_F) of fluorescence. Quantum yields (φ_PC) of loss of PA due to photoreactions in some solvents have also been determined under conditions of steady irradiation at 366 nm; φ_PC is in the range 0.1–0.2 in electron-rich olefinic solvents such as cyclohexene and tetramethylethylene. These results concerning τ_F, τ_T, φ_F. φ_T and φ_PC as well as the effects of 1,2,4-trimethoxybenzene and 2,5-dimethyl-2,4-hexadiene as quenchers for fluorescence, triplet yield, and photochemistry are discussed in the light of possible state orders for PA in polar and nonpolar environments.     

QUANTIFICATION OF THE SOLVENT EFFECTS ON THE TRIPLET QUANTUM YIELD OF PSORALEN BY THE "LINEAR SOLVATION ENERGY RELATIONSHIP"

Triplet formation quantum yields (Φ_τ) of psoralen in a set of 17 pure solvents ranging from n -hexane to water and in dioxane: water mixtures were obtained by nanosecond laser flash photolysis. The triplet yield increases with solvent polarity. The extremum values are 0.009 and 0.545 in n -hexane and water, respectively. Good correlations of the experimental Φ_τ values with empirical "polarity" scales (Dimroth/Reichardt's E_T [30], Kamlet/Taft's solva-tochromic parameters β, and α, and Swains acity/basity A_S/B_S) were obtained: Ln(φ_T^-1 - 1) = 8.86 - 0.143E_T(30) Ln(φ_T^-1 - 1) = 4.40 - 2.34_τ - 1.70α Ln(φ_T^-1 - 1) = 4.65 - 3.72A_s - 1.12B_s The results are discussed in terms of the sensitivity of psoralen triplet quantum yield to solvent polarity and hydrogen-bonding abilities.     

INACTIVATION OF Trypanosoma cruzi TRYPOMASTIGOTE FORMS IN BLOOD COMPONENTS BY PHOTODYNAMIC TREATMENT WITH PHTHALOCYANINES

Abstract— -Three phthalocyanine dyes HOSiPcOSi(CH₃)₂(CH₂)₃N(CH₃)₂ (Pc 4), HOSiPc-OSi(CH₃)₂(CH₂)₃N+(CH₃)3I- (Pc 5) and aluminum tetrasulfophthalocyanine hydroxide (AlOHPcS₄) were evaluated for their ability to inactivate the trypomastigote form of Trypanosoma cruzi in fresh frozen plasma (FFP) and red blood cell concentrates (RBCC). The compound Pc 4 was found to be highly effective in killing T. cruzi, Pc 5 less effective and AlOHPcS₄ ineffective. With FFP as the medium, a complete loss of parasite infectivity in vitro (≥5 log₁₀) was found to occur with 2 μ M Pc 4 after irradiation with red light (>600 nm) at a fiuence of 7.5 J/cm², while with RBCC as the medium, a complete loss was found to occur at a fiuence of 15 J/cm². Even without illumination, Pc 4 at 2 μ M also killed about 3.7-4.1 log₁₀ of T. cruzi in FFP during 30 min. Observed differences in T. cruzi killing by the various phthalocyanines may relate to differences in binding; Pc 4 binds to the parasites about twice as much as Pc 5. Ultrastructural analysis of treated parasites suggests that mitochondria are a primary target of this photodynamic treatment. The data indicate that Pc 4 combined with exposure to red light could be used to eliminate bloodborne T. cruzi parasites from blood components intended for transfusion. The inactivation of T. cruzi by Pc 4 in the dark suggests a possible therapeutic application.     

A Water-Soluble Luminescence Oxygen Sensor

We developed a water-soluble luminescent probe for dissolved oxygen. This probe is based on (Ru[dpp(SO₃Na)₂]₃) Cl₂, which is a sulfonated analogue of the well-known oxygen probe (Ru[dpp]₃)Cl₂. The compound dpp is 4,7-diphenyl-1,10-phenanthroline and dpp(SO₃Na)₂ is a disulfonated derivative of the same ligand. In aqueous solution in the absence of oxygen (Ru[dpp(SO₃Na)₂]₃)Cl₂ displays a lifetime of 3.7 μs that decreases to 930 ns on equilibrium with air and 227 ns on equilibrium with 100% oxygen. The Stern–Vohner quenching constant is 11330 M⁻¹. This high oxygen-quenching constant means that the photoluminescence of Ru(dpp[SO₃Na]₂)₃Cl₂ is 10% quenched at an oxygen concentration of 8.8 x 10⁻⁶ M , or equilibration with 5.4 torr of oxygen. The oxygen probe dissolved in water displays minimal interactions with lipid vesicles composed of dipalmityl-L-α-phosphatidyl glycerol but does appear to interact with human serum albumin. The absorption maximum near 480 nm, long lifetime and large Stokes'shift allow this probe to be used with simple instrumentation based on a light-emitting diode light source, allowing low-cost oxygen sensing in aqueous solutions. To the best of our knowledge this is the first practical water-soluble oxygen sensor.     

A MORE EXACT THEORETICAL INTERPRETATION OF RECENT EXPERIMENTAL DATA OBTAINED USING THE SEPARATED SENSITIZER AND SUBSTRATE METHOD TO INVESTIGATE O2(lδg) INTERACTIONS. POSSIBLE IMPORTANCE OF O2(1σg+)

Abstract— Recent experimental data obtained using the separated sensitizer and substrate method to investigate the interaction of O₂(¹δ_g) with various substances has been re-interpreted by means of a more complete theory. Comparison of experimental and recalculated values of the dependence of relative reaction rates on the sensitizer-substrate separation indicate general accord for experiments in which singlet oxygen acceptors in aqueous solution were used. The presumption is therefore that singlet molecular oxygen O₂(¹δ_g) is indeed the active oxidizing agent and that the theory presented and experiment are entirely in agreement.
For experiments in which bacterial targets were used a very distinct disagreement between theory and experiment is evident, the conclusion being that the kill rate does not depend linearly on the O₂(¹δ_g) concentration in the immediate proximity of the bacteria. However, the data is consistent with a quadratic dependence on the ¹δ_g concentration. A possible conclusion therefore is that the cytotoxic species is actually O₂(¹σ⁺_g), formed by an energy pooling reaction involving two O₂(¹δ_g) molecules.     

EFFECT OF AGGREGATION ON THE HEMATOPORPHYRIN-SENSITIZED PRODUCTION OF SINGLET MOLECULAR OXYGEN

Abstract— The hematoporphyrin-sensitized production of singlet molecular oxygen, O₂(¹Δ_g), has been investigated in methanol and in aqueous solution. The quantum yield for formation of O₂(¹Δ_g) (Φ_Δ) has been measured by both steady-state (oxygen consumption) and time-resolved (near-infrared luminescence) methods. In methanol, both techniques indicate that Φ_Δ= 0.76 and the value remains independent of sensitizer concentration over a wide range. This finding is consistent with the dye persisting in a monomelic form in methanol solution. In contrast, Φ_Δ decreases markedly with increasing sensitizer concentration in water due to dimerization of the dye. Analysis of the steady-state data indicates Φ_Δ values of 0.74 and 0.12, respectively, for monomer and dimer. It is further shown that the efficiency whereby quenching of the triplet state by O₂ results in generation of O₂(¹Δ_g) is substantially lower for the dimer than for the corresponding monomer. Because monomer and dimer possess quite different absorption spectral profiles, the efficacy for photodynamic action with hematoporphyrin exhibits a pronounced wavelength dependence.     

PHOTOLESIONS IN DNA UPON 193 nm EXCITATION

Aqueous solutions of plasmid (pBR322 and pTZ18R) and calf thymus DNA were excited by 20 ns laser pulses at 193 nm. The quantum yields of single- and double-strand break formation, interstrand cross-links, locally denatured sites, (6–4)photoproducts and biological inactivation (Φ_ssb, Φ_dsb, Φ_icl, Φ_ids, Φ_6–4 and Φ_ina, respectively) were measured. The quantum yields are virtually independent of intensity, demonstrating a one-quantum process. The obtained values in aerated neutral solution in the absence of additives are Φ_ssb= 1.5 × 10^--³, Φ_dsb, = 0.06 × 10^--³ (dose: 10–200 J m^-2), Φ_icl=Φ_Ids= 0.1 × 10³ and Φ_6–4= 0.5 × 10^--³ Both Φ_ssb and Φ_dsb decrease strongly with increasing concentrations of TE buffer (0.01–10 m M ). Biological inactivation of the pTZ18R plasmid was determined from the transformation efficiency of Escherichia coli bacteria strains AB1157, AB1886 uvr and A82480 uvr rec; the Φ_ina values are 1.4 × 10³, 2.1 × 10³ and 3 × 10^--³, respectively. The monoexponential survival curves in all cases show that a single damage site leads to inactivation (one single hit). The biological consequences of different photoproducts are discussed.     

TIME RESOLUTION OF A BACK PHOTOREACTION IN BACTERIORHODOPSIN

Abstract— The back photoreaction from the M(412nm) intermediate in the photocycle of light-adapted bacteriorhodopsin, BR_LA(570 nm), is studied using pulsed laser excitation. The decay of a primarily produced species, M_P, regenerates BR_LA(570nm) in a process characterized by a half life of 200 ns at 25°C. The absorption maximum of M_P is blue shifted (Λ_max≃ 395 nm) relative to that of M(412nm). The primary photochemical step, M(412nm) → M_P, is attributed to a conformational change in the polyene residue. The energy and entropy of activation of the subsequent M_P→ BR_LA (570 nm) relaxation are reported and discussed.     

RELATIONSHIP BETWEEN PHYTOCHROME PHOTOCONVERSION and RESPONSE

Abstract— The action of phytochrome on appearance of NADH-dependent glutamate synthase (NADH-GOGAT) and ferredoxin-dependent glutamate synthase (Fd-GOGAT) was studied in the cotyledons of the mustard ( Sinapis alba L.) seedling. It was found that the [P_fr]-response curves are composed of two branches with two very different slopes (a₁ a₂). This explains the biphasic fiuence response curves reported previously. While a, is the same with both enzymes, a, is much higher in NADH-GOGAT than in Fd-GOGAT. However, the transition from the high (a₁) to the low (a₁) slope occurs at the same P_fr/P_tot ratio irrespective of the steepness of a₁ While the appearance of NADH-GOGAT is very sensitive to small amounts of P_rr (high a₁), the response is not sensitive to the "High Irradiance Reaction" (HIR) of phytochrome. On the other hand, appearance of Fd-GOGAT (relatively low a₁) exhibits the usual HIR. It is concluded that the presently available models of phytochrome action, including the dimeric model, are not adequate to account for the actual data. At present it appears that a multiplicity of primary actions of phytochrome exist, and that it is the availability of the primary reactant (X, _1,2,3) which determines transduction or non-transduction of the phytochrome signal.     

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.     

THE REACTION OF METHYLENE WITH HYDROGEN

Abstract— An investigation has been made of the reaction between methylene, formed by the photolysis of ketene, and hydrogen. Ethane, ethylene and methane are the major hydrocarbon products, and it has been shown that the formation of these products may be adequately described by the sequence of processes
CH₂CO + hv → CH₂+ CO (1)
CH₂+ H₂→ CH₃+H (2)
2CH₃→ C₂H₆ (3)
CH₃+ H₂+ CH₄+ H (4)
CH₂+ CH₂CO → C₂H₄+ CO (7)
In particular, the relative rates of ethane and methane formation are consistent with the known rate constants for reactions (3) and (4), and it is not therefore necessary to postulate the participation of an 'insertion' process
CH₂+ H₂→ CH₄ (6) to account for the formation of methane.
Decrease of the energy possessed by the methylene, either by increase of the wavelength of ketene photolysis, or by increase of gas pressure, is shown to result in an increase in the reactivity of the methylene towards ketene relative to its reactivity towards hydrogen (i.e. the ratio k₂/k₂ increases).     

MECHANISM OF PHOTOSENSITIZATION BY PHEOPHORBIDE a STUDIED BY PHOTOHEMOLYSIS OF ERYTHROCYTES AND ELECTRON spIN RESONANCE SPECTROSCOPY

Abstract Phcophorbide a (PPa), a causal substance of food intoxication, when excited by exposure to light wavelengths of over 600 nm, caused the photohemolysis of goat erythrocytes in proportion to the incubation time of the cells. The addition of N-₃, an effective scavenger of ¹O₂, to the medium markedly inhibited the hemolysis of erythrocytes in a concentration-dependent manner, whereas the addition of superoxide dismutase (SOD) and catalase, inhibitors of O^-₂ and H₂O₂ generation, respectively, to the medium had little effect on it.
Methods for converting ¹O₂ to a nitroxide radical by 2,2,6,6-tetramethyl-4-piperidone (TMPD) and for trapping O^-₂ and OH by 5,5-dimethyl-l-pyrroline-A'-oxide (DMPO) were employed to observe directly these activated oxygens by electron spin resonance (ESR). The methods provided evidence that only ¹O₂, was produced by PPa, which was excited by light wavelengths of over 600 nm. Both the addition of N₃ to the solution and the removal of oxygen from the solution inhibited the generation of ¹O₂.
These results led us to conclude that ¹O₂ was mainly responsible for the hemolysis of erythrocytes by photoexcited PPa.