FLUORESCENCE OF 5-METHYLCYTOSINE

Abstract— 5-Methylcytosine and 5-methyldeoxycytidylic acid are fluorescent in aqueous solution at room temperature and neutral pH. 5-Methylcytosine, 10^-3M, pH 8.5, 25°C, has a quantum yield of 5 ×10^-4, 5-Methyldeoxycitydylic acid, 10^-4M, pH 7.5, 20°C, has a quantum yield of 8 × 10^-4. Emission maxima are 2.91 and 2.80μ^-1. At pH 14, the quantum yield of 5-methylcytosine is 1.6 × 10^-2; the emission maximum is 2.82μ^-1. At pH I, the quantum yield of both compounds is less than or equal to 10^-4. Both compounds were chromatographically homogeneous, had absorption spectra which agreed with published data, and excitation spectra which agreed closely with absorption spectra.     

Depopulation of Highly Excited Singlet States of DNA Model Compounds: Quantum Yields of 193 and 245 nm Photoproducts of Pyrimidine Monomers and Dinucleoside Monophosphates

Abstract— Formation of uracil and orotic acid photodimers, uridine and 5'-UMP photohydrates, TpT photodimers and (6-4)photoproducts, dCpT photohydrates and (6-4)photo-products and UpU, CpC and CpU photohydrates were studied in neutral deoxygenated aqueous solution at room temperature upon irradiation at either 193 or 254 nm. The photoproducts were identified and quantified and the contribution from photoionization to substrate decomposition, using λ_irr= 193 nm, was separated. The ratio of the quantum yields of respective stable products,η=φ¹⁹³/φ²⁵⁴ is indicative of the yield of internal conversion from the second to the first excited singlet state, S₂→ S₁. For the observed photodimers η decreases from 0.94 for uracil to 0.7 for TpT and further to 0.55 for orotic acid. For the (6-4)photoproducts of TpT and dCpT T| = 0.5-0.8 and for the photohydrates in the cases of UpU, CpC, CpU and dCpT TJ ranges from 0.55 to 1.     

SOLVENT EFFECTS ON THE TAUTOMERIZATION OF 5'-DEOXYPYRIDOXAL. A PHOTOPHYSICAL STUDY

Abstract— Absorption and fluorescence spectra of 5'-deoxypyridoxal (DPL) in various pure solvents and mixtures were recorded both at room temperature and over the range10–65°C. The areas under the absorption bands were analyzed to obtain the mole fraction (f_N, f_z) of two tautomers (the zwitterionic, Z, and neutral, N, forms) in the ground state. The following spectral parameters were determined from the fluorescence spectra: Stokes shift (Δ v ), fluorescence quantum yield of the neutral form (Q_N), fluorescence ratio of the neutral to the zwitterionic form (ø_N/ø_Z) and the rate constant of tautomerization ( k ₁) from Z to N in the excited state. Some of these parameters (f_N, Δ v , Q_N, k ₁) were found to depend on the proton donor character of the solvent, whereas others (ø_N/ø_Z) depended on its dipole moment. Thus, the absorption and fluorescence spectra of DPL allow one to obtain information on the polarity and the concentration of –OH groups on its environment.     

Potassium Iodide as a Chemical Actinometer for 254 nm Radiation: Use of lodate as an Electron Scavenger

Abstract— A solution of 0.6 M iodide and 0.1 M iodate in 0.01 M borate buffer (pH 9.25) can be used as a chemical actinometer to measure the incident fluence from a low-pressure mercury lamp that puts out more than 85% of its energy at 254 nm. The actinometric solution is optically opaque to light below 290 nm and is optically transparent to wavelengths greater than 330 nm. Hence, the solution absorbs all of the germicidal wavelengths but little if any of the ambient light normally present in the laboratory. Iodate acts as an electron scavenger and prevents the back reaction of the free electron with the iodine atom following UV excitation of KI. Irradiation results in the linear formation of triiodide, which is quantitated by measuring its absorbance at 352 nm. The quantum yield for this system is approximately 0.75 0.03 at 20.7A_oC or approximately three times greater than that obtained previously using nitrous oxide as an electron scavenger. A model is proposed to account for this difference. A precise expression to account for the concentration and temperature dependence of the quantum yield is given by pH = 0.75(1 + 0.23[C - 0.577])(1 + 0.02[T - 20.7]) where C is the concentration of iodide and T is the temperature. The concentration of iodide can be obtained from the absorbance at 300 nm prior to irradiation using 1.061 MJ cm⁻¹ as the molar extinction coefficient. This actinometric system meets the quality criteria established by the International Union of Pure and Applied Chemistry with the caveat that it is designed to measure only germicidal radiation (i.e. wavelengths less than 290 nm).     

Quantum yield of the iodide-iodate chemical actinometer: dependence on wavelength and concentrations

The quantum yield (QY) of the iodide-iodate chemical actinometer (0.6 M KI-0.1 M KIO3) was determined for irradiation between 214 and 330 nm. The photoproduct, triiodide, was determined from the increase in absorbance at 352 nm, which together with a concomitant measurement of the UV fluence enabled the QY to be calculated. The QY at 254 nm was determined to be 0.73 +/- 0.02 when calibration was carried out against a National Institute of Standards and Technology traceable radiometer or photometric device. At wavelengths below 254 nm the QY increased slightly, leveling off at -0.80 +/- 0.05, whereas above 254 nm the QY decreases linearly with wavelength, reaching a value of 0.30 at 284 nm. In addition, the QY was measured at different iodide concentrations. There is a slight decrease in QY going from 0.6 to 0.15 M KI, whereas below 0.15 M KI the QY drops off sharply, decreasing to 0.23 by 0.006 M KI. Calibration of the QY was also done using potassium ferrioxalate actinometry to measure the irradiance. These results showed a 20% reduction in QY between 240 and 280 nm as compared with radiometry. This discrepancy suggests that the QY of the ferrioxalate actinometer in this region of the spectrum needs reexamination.     

PHOTOCHEMISTRY OF RETINOCHROME

Abstract— Retinochrome is a photopigment found in the visual cells of cephalopods. It has been considered to act as a supplier of the 11- cis -retinal required for synthesis of rhodopsin, because its all-trans chromophore is isomerized to 11- cis form in the light. Light and thermal reactions of squid retinochrome were investigated by low-temperature spectrophotometry.
On irradiation with green light at liquid-nitrogen temperature, retinochrome (λ_max 496 nm, – 190°C) is converted mainly to an intermediate lumiretinochrome (λ_max 475 nm, – 190°C), its chromophore being changed to 11- cis -retinal. On irradiation with blue light at - 190°C, retinochrome is changed to a photosteady–state mixture (λ_max 487 nm, – 190°C) composed mainly of retinochrome and lumiretinochrome, since lumiretinochrome is partially regenerated back to retinochrome. Similarly, irradiation of lumiretinochrome with blue light also results in the same photosteady-state mixture, which can be completely reverted to lumiretinochrome on re-irradiation with green light.
Lumiretinochrome is stable at a wide range of temperatures from – 190°C to about – 20°C. Above – 20°C, it is further converted, thermally, into metaretinochrome (λ_max 470 nm), which is the same bleached product as has been observed on irradiation of retinochrome at room temperatures. Thus, the light-bleaching process of retinochrome is rather simple compared with that of rhodopsin.     

Singlet Oxygen Generation by Metallotexaphyrins

Abstract. Metallotexaphyrins have clinical applications as photo-sensitizers of photodynamic therapy (PDT). The singlet oxygen quantum yield (φ>_Δ) was determined for a series of metallotexaphyrin derivatives (Lu [III], Y [III], Cd [II], In [III] and Gd [in]) under conditions where the agents are believed to exist in monomeric form. The results show φ_Δ of metallotexaphyrins vary with the medium and the metal cation. Measurements on the Lu (III) texaphyrin led to φ_Δ= 0.38 in unbuffered 5% Tween 20 and φ_Δ= 0.58 in pH 7.4 phosphate buffer plus 1% Triton X-100 (±10%). The in vitro photodynamic efficiency calculated from φ_Δ is compared to in vivo PDT efficacy in an animal tumor model.     

DIRECT DETECTION OF SINGLET OXYGEN SENSITIZED BY HAEMATOPORPHYRIN AND RELATED COMPOUNDS

Abstract— Direct time-resolved detection of the luminescence at 1270 nm from 'singlet oxygen' was used to estimate the quantum yield of singlet oxygen production (Φ_Δ) from a series of related porphyrins in benzene and in D₂O. From this and available data the fraction of oxygen quenching interactions leading to singlet oxygen production (S_Δ) was derived in most cases. A marked increase in Φ_Δ value was observed for di-haematoporphyrin ester (DHE) in cetyltrimethyl ammonium bromide/D₂O solution in comparison to D₂O alone, this increase is attributed to a major structural alteration of DHE on introduction of the detergent.     

FLUORESCENCE OF THYMINE IN AQUEOUS SOLUTION AT 300° K

Abstract— –Fluorescence of thymine in neutral aqueous solution at room temperature has been detected using the multiscaling operation of a multichannel analyzer. The emission maximum (2.96 μm^-1) and 0-0 transition energy (3.37-3.45 μm^-1) are close to those determined at liquid nitrogen temperature in mixed solvents. The quantum efficiency of fluorescence excited at 3.77 μm^-1 is calculated to be 1.04 × 10^-4.
The corrected relative excitation spectrum shows significant differences from the absorption spectrum when both are determined under identical conditions of concentration and spectral bandwidth on the same instrument. The quantum yield of fluorescence decreases about 2-fold as the energy of excitation is increased beyond the 0-0' transition and follows the relation 1/φ°α E _excit..
This behavior is discussed in terms of (a) n π* and ππ* states, (b) emission from a minor tautomer and (c) kinetics of competing deactivation processes.     

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.     

MODIFYING FACTORS OF THE CELLULAR CONCENTRATION OF PHOTOLYASE MOLECULES IN Saccharomyces cerevisiae—II. EFFECTS OF PREILLUMINATION WITH LIGHT FLASHES

Abstract The effects of preillumination with photoreactivating light flashes before UV-irradiation on the number of photoreactivable complexes consisting of UV-induced DNA-damages and active photolyase molecules (N_PREact), on the fluence decrements, ΔD_PRE, that are obtained from two UV-survival curves without and with 1 flash photoreactivation and proportional to N_PREact were determined in haploid Saccharomyces cerevisiae cells. ΔD_PRE increased by preillumination from 0.115 Jm^–2 to 0.460 Jm^–2 and from 0.376 Jm^–2 to 0.494 Jm^–2 in cells in logarithmic growth phase and in stationary growth phase, respectively. Δ_PRF in log-cells that were preilluminated before and after resuspension in buffer at 40°C for 60 min was larger than ΔD_PRE in log-cells preilluminated only after resuspension in buffer.     

DNA SYNTHESIS-KINETICS, CELL DIVISION DELAY, AND POST-REPLICATION REPAIR AFTER UV IRRADIATION OF FROZEN CELLS OF E. COLI B/r

Abstract— Previous studies have shown that the relative yields of photoproducts produced in the DNA of Escherichia coli cells UV irradiated at -79°C differ from those produced at +21°C; the yield of DNA-protein cross-links was markedly enhanced at -79°C while the yield of thymine dimers was reduced. In the present studies, cells of E. coli B/r thy were frozen at -79°C, and then UV irradiated (254nm) while frozen(4.7 J m^-2), or after thawing (22 Jm^-2). Essentially the same survival, cell division delay, and DNA synthesis kinetics were observed for these two samples after irradiation, even though the UV fluence differed by a factor of ˜5. This supports previous observations that a correlation exists between the magnitude of the effects of UV radiation upon DNA synthesis kinetics and on cell survival. The weight average molecular weight of the pulse labeled DNA in the sample irradiated at +21°C was one-half that of the sample irradiated at -79°C, and complete repair of daughter-strand gaps was observed in both cases. Thus, UV-induced lesions produced in cells at -79°C (i.e. DNA-protein cross-links) appear to be amenable to post-replicational repair. While the overall DNA synthesis kinetics were the same for the two irradiation procedures, the apparent number of lesions produced per unit length of DNA was not. This suggests that each of the lesions produced in frozen cells, although apparently fewer in number, must cause a longer local delay in DNA synthesis than those lesions produced at +21°C.     

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.     

PHOTOCHEMICAL ALTERATIONS IN DNA REVEALED BY DNA-BASED LIQUID CRYSTALS

Abstract The preparations of chicken erythrocyte linear double-stranded DNA and superhelical plasmid pBR322 DNA were irradiated by continuous low-intensity UV radiation (I = 25-50 W/m², λ= 254 nm) as well as by highintensity picosecond laser UV radiation (I = 10¹¹-10¹³ W/m², λ= 266 nm). The effect of DNA secondary structure alterations on the formation of liquid-crystalline dispersions from UV-irradiated DNA preparations was studied. It was shown that in the case of linear DNA, watching the disappearance of abnormal optical activity characteristic for cholesteric liquid crystal we managed to detect the presence of photochemical alterations in DNA irradiated by low-intensity UV radiation at an absorbed energy of more than 20 quanta per nucleotide. In the case of superhelical DNA using enzyme treatment of liquid-crystalline dispersions and monitoring the appearance of abnormal optical activity, we detected the presence of photochemical alterations in DNA molecules after low-intensity UV irradiation at an absorbed energy of less than 4 quanta per nucleotide. Under the latter approach using picosecond UV laser irradiation at three different light intensities we were able to distinguish the different mechanisms of fine alterations in DNA secondary structure at an absorbed energy value of about 3 quanta per nucleotide.     

PHOTOLYSIS OF AQUEOUS SOLUTIONS OF POTASSIUM CIS-DIAQUOBIS (OXALATO) CHROMATE (III)

Abstract— The photolysis of aqueous solutions of cis -[Cr(C₂O₄)₂(H₂O)₂]- at 254 nm and pH 4 produced CO₂ and H₂ in nearly equal yields. The quantum yield of hydrogen, φ², increased by 9% and the yield of carbon dioxide, φ, by 65% as the pH was lowered from 4 to I. The total gas yield, φ_gas, decreased in the presence of added oxalate or chromium (II) ions and when the light intensity was lowered. The gas yield in D₂O was appreciably higher than in H₂O. The variation of φ_gas with pH (D) and with added oxalate ion was roughly parallel in the two liquid media. The gas yield increased in the series:
A tentative mechanism is suggested to explain the results.     

WAVELENGTH-DEPENDENT QUANTUM YIELD OF OH RADICAL FORMATION FROM PHOTOLYSIS OF NITRITE ION IN WATER

Abstract. Photolysis (298- or SCN^- scavenging of OH and ³BP (benzophenone) actinometry. The significance of these results, and their dependence on pH, temperature, and [O₂], for the photolysis of nitrite in seawater is discussed briefly.     

SYNERGISTIC LETHAL ACTION OF ULTRAVIOLET-VIOLET RADIATIONS AND MILD HEAT IN ESCHERICHIA COLI

Abstract— The lethal interaction of far ultraviolet (254nm), near ultraviolet (334 and 365nm) and violet visible (405nm) radiation treatment with mild heat treatment was studied. Except at 254nm, a strong positive radiation dose-dependent interaction (synergism) was always observed. The efficiency of sensitisation to heat, as a function of dose at each wavelength, was found to be directly correlated with the dose necessary to eliminate the shoulder from the survival curve of a repair proficient strain but was apparently unrelated to the relative near-ultraviolet sensitivities of a repair deficient strain. The interaction was independent of the order of treatments. A radiation dose of 10⁶ Jm^-2 at 365nm slightly sensitised a cell population to 45°C incubation (normally non-lethal) and strongly sensitised the cells to 48°C treatment (normally 80 percent survival after 2 hours). It is proposed that in addition to DNA damage, both heat treatment and near ultraviolet treatment interfere with DNA recovery mechanisms so that the combination of the two agents inevitably leads to a strong positive interaction.     

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.     

UV-B RADIATION EFFECTS ON PHOTOSYNTHESIS, GROWTH and CANNABINOID PRODUCTION OF TWO Cannabis sativa CHEMOTYPES

The effects of UV-B radiation on photosynthesis, growth and cannabinoid production of two greenhouse-grown C. sativa chemotypes (drug and fiber) were assessed. Terminal meristems of vegetative and reproductive tissues were irradiated for 40 days at a daily dose of 0, 6.7 or 13.4 kJ m^-2 biologically effective UV-B radiation. Infrared gas analysis was used to measure the physiological response of mature leaves, whereas gas-liquid chromatography was used to determine the concentration of cannabinoids in leaf and floral tissue.
There were no significant physiological or morphological differences among UV-B treatments in either drug- or fiber-type plants. The concentration of Δ⁹-tetrahydrocannabinol (Δ⁹-THC), but not of other cannabinoids, in both leaf and floral tissues increased with UV-B dose in drug-type plants. None of the cannabinoids in fiber-type plants were affected by UV-B radiation.
The increased levels of Δ⁹-THC in leaves after irradiation may account for the physiological and morphological tolerance to UV-B radiation in the drug-type plants. However, fiber plants showed no comparable change in the level of cannabidiol (a cannabinoid with UV-B absorptive characteristics similar to Δ⁹ THC). Thus the contribution of cannabinoids as selective UV-B filters in C. sativa is equivocal.     

POTENTIAL PHOTOSENSITIZERS FOR PHOTODYNAMIC TUMOR THERAPY—I. PHOTOPHYSICAL PROPERTIES OF TWO CHLORIN DERIVATIVES

Abstract— Photophysical properties of two chlorin type molecules (CHLI) and (CHLII) were investigated in different solvents. Quantum yields of fluorescence φ_F of S, → T, intersystem crossing φ_T, and of singlet oxygen (¹Δ_g) formation φ_Δ, as well as the Stern-Volmer constants for the quenching of the S, states by oxygen and the bimolecular rate constants of quenching of ¹Δ_g by the chlorins were measured. The values of φ_T and φ_Λ can be given as 0.57 and 0.58 for CHLI and 0.69 and 0.58 for CHLII. The values of the fluorescence quantum yields, the strong absorption of the chlorins in the red (Λ > 630 nm) and the high values of the quantum yields for ¹Δ_g formation recommend the chlorin derivatives as potential markers and photosensitizers for tumor therapy.