Sensitization of singlet delta oxygen (O₂(¹Δ_g)) by bacteriochlorophyll e (BChle) has been investigated to gain a better understanding of the photoprotection mechanism(s) operating in chlorosomes of green photosynthetic bacteria. The sensitization process has been studied in media where BChle forms monomers (acetone and aqueous solutions containing 0.5% Triton X-100 [TX]) and in systems where BChle aggregates, namely, aqueous solutions containing 0.003% monogalactosyl diglyceride (MGDG) and chlorosomes (control as well as hexanol perturbed) from Chlorobium phaeobacteroides strain CL1401. In Ar-purged acetone, BChle triplets (BChle^†) have a lifetime of a few tens of microseconds; however, in air-saturated acetone, quenching of BChle^† by ground-state oxygen (O₂(³Σ⁻_g)) and formation of O₂(¹Δ_g) take place. The O₂(¹Δ_g) so formed is susceptible to quenching by BChle⁰, a ground-state BChle molecule. A Stern–Volmer analysis reveals a linear fit between the decay rate of O₂(¹Δ_g) and the BChle concentration. The rate constants for the quenching of O₂(¹Δ_g) by BChle⁰ and for the deactivation of O₂(¹Δ_g) by the solvent come out to be k_q = (1.4 ± 0.1) × 10⁹ M⁻¹ s⁻¹ and k₀ = (18.5 ± 0.7) × 10³ s⁻¹, respectively. The absolute quantum yield of O₂(¹Δ_g) sensitization by BChle monomers is 0.65 ± 0.15 in air-saturated acetone. In aqueous phase, the triplet lifetime of BChle aggregates in native or hexanol-perturbed chlorosomes shortens by more than two orders of magnitude when compared with the triplet lifetime of BChle monomers in 0.5% TX solution (a few hundreds of microseconds). Quenching by carotenoids (Car) makes only a minor contribution to the decay of BChle^† in aggregates. Because O₂(¹Δ_g) sensitization by BChle^† could be detected neither in MGDG aggregates nor in chlorosomes (control as well as hexanol perturbed), it is concluded that (1) this process is highly likely when BChle is present as a monomer but not when it is tightly packed in artificial aggregates or in chlorosomes; and (2) Car, though vital for the baseplate BChla, are dispensable for BChle.

Resonance energy transfer between tryptophanyl residues and the apolar fluorescent dye 1-anilino-8-naphthalene sulfonate (ANS) occurs when the fluorophore is bound to native folded sperm whale apomyoglobin. The individual transfer contribution of the two tryptophanyl residues (W7 and W14, both located on the A-helix of the protein) was resolved by measuring the tryptophan–ANS transfer efficiency for the ANS–apomyoglobin complexes formed by wild-type protein and protein mutants containing one or no tryptophanyl residues, i.e. W7F, W14F and W7YW14F. The transfer efficiency of W14 residue was found to be higher than that of W7, thus indicating that W14 acts as the main energy donor in the ANS–apomyoglobin complex. This suggests that the plane containing the anilinonaphthalene ring of the extrinsic fluorophore has a spatial orientation similar to that of W14 and, hence, to the heme group in the holoprotein.

The photophysics and photochemical behavior of the phenoxazin-3-one dyes, resazurin and resorufin, have been studied in aqueous solutions. The irradiation of resazurin in the presence of amines leads to deoxygenation of the N-oxide group, giving resorufin. This photoreaction is highly dependent on the amine structure and is efficient only in the presence of tertiary aliphatic amines. The absorption and fluorescence properties of these dyes are dependent on pH. At pH above 7.5 both dyes are in their anionic form. For resorufin this form is highly fluorescent (Φ_F = 0.75). At lower pH the fluorescence is strongly reduced. The N-oxide dye presents a very weak fluorescence quantum yield (0.11), which also is reduced at low pH. Flash photolysis experiments allowed characterization of the triplet state and the transients formed after irradiation of these dyes in the absence and presence of amines. The triplet quantum yields are 0.08 for resazurin and 0.04 for resorufin. The photodeoxygenation of N-oxide in the presence of amines occurs from the triplet state.

Although according to the International Radiological Protection Association–International Non-Ionizing Radiation Committee recommendation (1991) the use of sunbeds for cosmetic purposes is not recommended, tanning devices are used widely. Ten different types of commercially available sunbed tubes have been studied using a uracil biological UV dosimeter, and three of them were analyzed in detail. Dimerization effectiveness of the tubes was measured directly, whereas efficiency of erythema induction was calculated weighting the emission spectra by the Commission Internationale de l'Eclairage erythema action spectrum. The data obtained demonstrate that quality control of sunbed tubes has to include not only the determination of the UV doses administered but also the assessment of the health risk due to the UVB and UVA components of the lamp. A method of quality control using the uracil biological dosimeter was elaborated, and the estimation of the “acceptable” exposure time was checked/controlled on 15 volunteers by assessing individually the erythema induction threshold. A correct classification of the sunbed tubes is proposed by characterizing the erythema induction versus DNA-damaging effectiveness of tubes.

Narrowband UVB (NB-UVB) is a newly developed UVB source that, in addition to the previously used broadband UVB (BB-UVB), has been effectively used in phototherapy of various skin diseases. Besides its therapeutic effectiveness, NB-UVB also has some adverse effects that should be evaluated. As with all phototherapies, the photocarcinogenic potential of NB-UVB is the major concern. To assess the carcinogenic potential we measured the DNA damage induced by the two UVB sources because exposure of cells to UVB directly or indirectly induces DNA damage such as cyclobutane pyrimidine dimers (CPD) or 8-oxo-7,8-dihydro-2′-deoxyguanosine (8-oxodGuo), respectively. These types of DNA damage cause mutations of oncogenes and tumor suppressor genes, which can lead to photocarcinogenesis. In the present study we measured the yield of CPD and the oxidative DNA damage marker, 8-oxodGuo, in organ-cultured human skin and in mouse skin after exposure to NB-UVB or BB-UVB at therapeutically equivalent doses. We show that a 10-fold higher dose of NB-UVB yields a similar amount of CPD compared with BB-UVB in two types of samples examined. In contrast to CPD, the formation of 8-oxodGuo after irradiation with NB-UVB at a 10-fold higher dose is 1.5–3 times higher than that caused by BB-UVB. These results suggest that although NB-UVB at equivalent erythema–edema doses is not more potent in inducing CPD formation than is BB-UVB, NB-UVB may generate a higher yield of oxidized DNA damage.

Single suberythemal exposures of UVA radiation have been shown to block the immunosuppressive effects of UVB radiation in the mouse. The immunoprotection is dependent both on the presence of the cytokine, IFN-γ, and on the induction of the antioxidant stress enzyme, heme oxygenase (HO), in the skin. Recently, the transcriptional response of the HO-1 gene to UVA radiation in cultured human skin fibroblasts was reported to be refractory to a second UVA irradiation. In this study on the hairless mouse, we demonstrate that the inducibility of HO enzyme activity in the skin similarly became refractory to a second UVA irradiation at 24 h but, like the fibroblast response, was restored when the interval between the UVA exposures was increased to 96 h. Under the conditions of refractory HO enzyme induction, the protective effect of UVA radiation against the suppression of contact hypersensitivity induced by UVB radiation or cis-urocanic acid was strongly attenuated but was restored when the interval between UVA exposures was increased to 96 h. The results thus confirm the strong relationship between HO induction and photoimmunoprotection by UVA radiation, and describe a new phenomenon of immunological refractoriness that develops with rapidly repeated UVA exposures.

Norwalk and Norwalk-like viruses (NLV) are major causes of food- and water-related disease in the United States. There is no host cell line in which the NLV can be tested for infectivity. Feline calicivirus (FCV) and NLV both belong to the family Caliciviridae. FCV can be assayed for infectivity in the Crandell Reese feline kidney cell line, so FCV serves as a surrogate for NLV. This study is the first report of UV inactivation of FCV and also of using the plaque technique, in contrast to the 50% tissue culture infectious dose end point technique, to determine the FCV infectivity titer. The infectivity titers (log₁₀ plaque-forming units/mL) of UV-inactivated FCV, hepatitis A virus (HAV), poliovirus type 1 (PV1) and two small, round coliphages were plotted as a function of UV dose and analyzed by regression analysis and analysis of variance. These fitted straight-line curves represent exponential inactivation, so UV inactivation can be said to show “one-hit kinetics.” The decimal inactivation doses of UV for FCV, HAV, PV1, MS2 and ϕX174 were 47.85, 36.50, 24.10, 23.04 and 15.48 mW s/cm², respectively. FCV appears to be the most UV resistant among the tested viruses.

The effects of combined photodynamic therapy (PDT) and ionizing radiation are studied in a human glioma spheroid model. The degree of interaction between the two modalities depends in a complex manner on factors such as PDT irradiation fluence, fluence rate and dose of ionizing radiation. It is shown that gamma radiation and PDT interact in a synergistic manner only if both light fluence and gamma radiation dose exceed approximately 25 J cm⁻² and 8 Gy, respectively. Synergistic interactions are observed only for the lower fluence rate (25 mW cm⁻²) investigated. The degree of interaction appears to be independent of both sequence and the PDT or ionizing radiation time intervals investigated (1 and 24 h). Terminal deoxynucleotidyl transferase–mediated deoxyuridine triphosphate nick-end labeling assays show that low-fluence rate PDT is very efficient at inducing apoptotic cell death, whereas neither high-fluence rate PDT nor ionizing radiation produces significant apoptosis. Although the mechanisms remain to be elucidated, the data imply that the observed synergism is likely not due to gamma-induced cell cycle arrest or to PDT-induced inhibition of DNA repair.

To determine the origin of the UV-specific CC to TT tandem mutation at the CC site, we made a duplex DNA decamer containing a uracil cis–syn cyclobutane dimer (CBD) as the deaminated model of a cytosine dimer. Two-dimensional ¹H-NMR spectroscopy studies were performed on this sequence where two adenines (Ade) were opposite to the uracil dimer. Two imino protons of the uracil dimer were found to retain Watson–Crick hydrogen bonding with the opposite Ade, although the 5′-U(NH) of the dimer site showed unusual upfield shift like that of the 5′-T(NH) of the TT dimer, which seemed to be associated with deshielding by the flanking base rather than with reduced hydrogen bonding. (McAteer et al. 1998, J. Mol. Biol. 282:1013–1032). Hydrogen bondings at the dimer site were also supported by detecting typical strong nuclear Overhauser effects (NOE) between two imino protons and the opposite Ade H2 or NH₂. But sequential NOE interactions of base protons with sugar protons were absent at the two flanking nucleotides of the 5′ side of the uracil dimer and at the intradimer site, contrasting with its thymine analog where sequential NOE was absent only at the A4–T5 step. In addition, NOE cross peak for U5(NH) ↔ A4(H2) was detected, although the NOE interactions of U6(NH) with A7(H2) and A17(H2) were not observed in contrast to the thymine dimer duplex. This different local structural alteration may be affected by the induced right-hand twisted puckering mode of cis–syn cyclobutane ring of the uracil dimer in the B-DNA duplex, even though the isolated uracil dimer had left-hand twisted puckering rigidly. In parallel, these observations may be correlated with observed differences in mutagenic properties between cis–syn UU dimer and cis–syn TT dimer.

Photodynamic therapy (PDT) of cancer is a very promising technique based on the formation of singlet oxygen induced by a sensitizer after irradiation with visible light. The stimulation of tumor growth by nitric oxide (NO) was reported recently, and NO was shown to have a protective effect against PDT-induced tumor death. We investigated a putative direct effect of NO on tumor cell death induced by PDT, using the human lymphoblastoid CCRF-CEM cells and bisulfonated aluminum phthalocyanine (AlPcS₂) as a sensitizer. Cells were incubated with AlPcS₂ in the presence or absence of NO donors ((Z)-1-[(2-aminoethyl)-N-(2-ammonioethyl)amino]diazen-1-ium-1,2-diolate, hydroxylamine and S-nitroso-N-acetylpenicillamine) or l-arginine. Under these conditions, in the absence of NO donors or l-arginine the cells died rapidly by apoptosis upon photosensitization. In the presence of NO donors or l-arginine, apoptotic cell death after photosensitization was significantly decreased. Modulation of cell death by NO was not due to S-nitrosylation of caspases and occurred at the level or upstream of caspase-9 processing. The protective effect of NO was reversed by incubating the cells with 1H-[1,2,4]oxadiazolo[4,3-a]quinoxalin-1-one, an inhibitor of guanylyl cyclase, or with KT5823, an inhibitor of protein kinase G (PKG). Incubation with 8-bromo-cyclic guanosine monophosphate, a membrane permeable cyclic guanosine monophosphate analog, also decreased cell death induced by PDT. Although the protective effect of NO against apoptotic cell death in several models has been attributed to an increase in the expression of heme oxygenase-1, heat shock protein 70 or Bcl-2, this was not the case under our experimental conditions. These results show that NO decreases the extent of apoptotic cell death after PDT treatment through a PKG-dependent mechanism, upstream or at the level of caspase activation.

To study the mechanism of photodynamic nerve cell killing, isolated crayfish mechanoreceptor neurons were photosensitized by the sulfonated aluminum ophthalocyanine Photosens. Neuron activity was continuously recorded until irreversible abolition. Intense (10⁻⁵ M Photosens) or weak (10⁻⁷ M Photosens) photosensitization induced different bioelectric neuron responses: firing activation followed by irreversible depolarization block or gradual inhibition until firing abolition, respectively. These bioelectric responses were accompanied by different biochemical and morphological changes. In the case of intense photosensitization, neuron nuclei swelled and then shrank. Succinate dehydrogenase (SDH) was inhibited, and the plasma membrane was compromised just after firing cessation. Weak photosensitization did not induce these changes but caused swelling of the endoplasmic reticulum and destruction of the matrix, cristae and membranes in some of the mitochondria. Other mitochondria, however, retained the normal structure. Plasma membrane damage, SDH inhibition, nucleus shrinkage and impairment of the nuclear border occurred after 2–4 h. It is concluded that intense photosensitization induced necrotic processes during irradiation, whereas weaker impact caused delayed necrosis 2–4 h later. The observed electrophysiological neuron responses to photodynamic therapy may be considered as early hallmarks of different modes of forthcoming cell death.

Photodynamic therapy (PDT) uses light to activate a photosensitizer to achieve localized tumor control. In this study, PDT mediated by a second-generation photosensitizer, palladium-bacteriopheophorbide WST09 (Tookad) was investigated as an alternative therapy for prostate cancer. Normal canine prostate was used as the animal model. PDT was performed by irradiating the surgically exposed prostate superficially or interstitially at 763 nm to different total fluences (100 or 200 J/cm²; 50, 100 or 200 J/cm) at 5 or 15 min after intravenous administration of the drug (2 mg/kg). Areas on the bladder and colon were also irradiated. The local light fluence rate and temperature were monitored by interstitial probes in the prostate. All animals recovered well, without urethral complications. During the 1 week to 3 month posttreatment period, the prostates were harvested for histopathological examination. The PDT-induced lesions showed uniform hemorrhagic necrosis and atrophy, were well delineated from the adjacent normal tissue and increased linearly in diameter with the logarithm of the delivered light fluence. A maximum PDT-induced lesion size of over 3 cm diameter could be achieved with a single interstitial treatment. There was no damage to the bladder or rectum caused by scattered light from the prostate. The bladder and rectum were also directly irradiated with PDT. At 80 J/cm², a full-depth necrosis was observed but resulted in no perforation. At 40 J/cm², PDT produced minimal damage to the bladder or rectum. On the basis of optical dosimetry, we have estimated that 20 J/cm² is the fluence required to produce prostatic necrosis. Thus, the normal structure adjacent to the prostate can be safely preserved with careful dosimetry. At therapeutic PDT levels, there was no structural or functional urethral damage even when the urethra was within the treated region. Hence, Tookad-PDT appears to be a promising candidate for prostate ablation in patients with recurrent, or possibly even primary, prostate cancer.

Fourier transform infrared (FTIR) spectroscopy is currently being developed as a new optical approach to the diagnosis and characterization of cell or tissue pathology. The advantage of FTIR microspectroscopy over conventional FTIR spectroscopy in the diagnosis of malignancies is that it facilitates inspection of restricted regions of the cell culture or tissue. In this study, we set out to evaluate FTIR microspectroscopy as a diagnostic tool for identifying retrovirus-induced malignancies. Our study showed significant and consistent differences between cultures of different types of cells of both mouse and human origin, i.e. primary fibroblast cells (one to two passages in cell culture), fibroblast cell lines and malignant cells transformed by murine sarcoma virus. An impressive decrease in the levels of phosphate and other metabolites was seen in malignant cells compared with primary cells. The levels of these metabolites in the cell lines were significantly lower than in the primary cells but higher than in the malignant cells. In addition, the peak attributed to the PO₂⁻ symmetric stretching mode at 1082 cm⁻¹ in primary cells shifted significantly to 1085 cm⁻¹ for the cell line and to 1087 cm⁻¹ for the malignant cells. These differences taken together with differences in the shapes of various bands throughout the spectrum strongly support the possibility of developing FTIR microspectroscopy for the detection and study of malignant—and possibly premalignant—cells.

Significant amounts of protoporphyrin IX (PpIX) are formed after 6 min of topical application of 5-aminolevulinic acid (ALA) and its hexylester derivative, whereas PpIX is formed after 10 min of topical application of ALA-methylester derivative in normal mouse skin at 37°C. Lowering the skin temperature to 28–32°C by the administration of the anesthetic Hypnorm–Dormicum reduces the PpIX fluorescence by a factor of 2–3. Practically no PpIX was formed as long as the skin temperature was kept at 12–18°C. At around 30°C PpIX fluorescence appears later after application of ALA-ester derivatives (14–20 min) than after application of ALA (8 min), indicating differences in their bioavailability (delayed penetration through the stratum corneum, cellular uptake, conversion to ALA, PpIX production) in mouse skin in vivo. The difference in lag time in the PpIX formation after application of ALA and ALA-esters may be partly related to deesterification of the ALA-ester molecules. The temperature dependence of PpIX production may be used for improvement of photodynamic therapy with ALA and ALA-ester derivatives, where accumulation of PpIX can be selectively enhanced by increasing the temperature of the target tissue.

The full-length apoprotein (124 kDa) and the chromophore-binding N-terminal half (66 kDa) of the phytochrome of the unicellular green alga Mougeotia scalaris have been heterologously expressed in the methylotrophic yeast Pichia pastoris. Assembly with the tetrapyrrole phycocyanobilin (PCB) yielded absorption maxima (for the full-length protein) at 646 and 720 nm for red- and far-red absorbing forms of phytochrome (P_r and P_fr), respectively, whereas the maxima of the N-terminal 66 kDa domain are slightly blueshifted (639 and 714 nm, P_r and P_fr, respectively). Comparison with an action spectrum reported earlier gives evidence that in Mougeotia, as formerly reported for the green alga Mesotaenium caldariorum, PCB constitutes the genuine chromophore. The full-length protein, when converted into its P_fr form and kept in the dark, reverted rapidly into the P_r form (lifetimes of 1 and 24 min, ambient temperature), whereas the truncated chromopeptide (66 kDa construct) was more stable and converted into P_r with time constants of 18 and 250 min. Also, time-resolved analysis of the light-induced P_fr formation revealed clear differences between both recombinant chromoproteins in the various steps involved. The full-length phytochrome showed slower kinetics in the long milliseconds-to-seconds time domain (with dominant P_fr formation processes of ca 130 and 800 ms), whereas for the truncated phytochrome the major component of P_fr formation had a lifetime of 32 ms.

pharaonis phoborhodopsin (ppR, also called pharaonis sensory rhodopsin II [psRII]) is a member of the archaeal rhodopsin family and acts as a repellent phototaxis receptor of Natronobacterium pharaonis. Upon illumination, ppR is excited and undergoes a linear cyclic photoreaction, namely, a photocycle that constitutes photointermediates such as M- and O-intermediates (ppR_M and ppR_O, respectively). Under a constant background illumination (>600 nm) that irradiates ppR_O, the decay rate of the flash-induced ppR_O increased with an increase in the background light intensity, indicating the photoreactivity of ppR_O. Azide did not influence the light-accelerated ppR_O decay, but the time required for the cycle to be completed became shortened in an azide concentration–dependent manner because of acceleration of ppR_M decay. Hence, the turnover rate of photocycling increased appreciably in the presence of both the background illumination and the azide. The observation reported previously (Schmies, G. et al. 2000, Biophys. J. 78:967–976) is discussed in connection with the present observations.