Marina V. Parkhats

Toward understanding the high PDT efficacy of chlorin e6-polyvinylpyrrolidone formulations: Photophysical and molecular aspects of photosensitizer-polymer interaction in vitro

It is recognized that chlorin e6-polyvinylpyrrolidone (Ce6-PVP) formulations are characterized by a high efficacy in photodynamic therapy of malignant tumors. Currently, a commercially available formulation of this type is Photolon (Fotolon) with Ce6:PVP=1:1 (w/w) and the weight-average molecular weight of PVP is 1.2x10(4). To gain a better understanding of the role played by PVP in Ce6-PVP formulations, we carry out experiments on IR and UV-VIS absorption, steady-state and time-resolved fluorescence, time-resolved triplet-triplet absorption, octanol-water partitioning, and solubility of chlorin e6 in buffer solutions at pH 6.3, 7.4, and 8.5 in presence of PVP with Ce6:PVP ratios ranging from 1:0 to 1:1000 (w/w) for PVP samples with weight-average molecular weights of 8x10(3), 1.2x10(4), and 4.2x10(4). We show that Ce6 interacts with PVP by forming molecular complexes via hydrophobic interactions and determine the Ce6-PVP binding constant, as well as the mean number of PVP monomers per binding site. We find that complexation of Ce6 with PVP prevents Ce6 aggregation in aqueous media and leads to an enhancement of Ce6 fluorescence quantum yield, while keeping the quantum yield of the intersystem crossing essentially unchanged. Possible scenarios of how the presence of PVP can favorably affect the PDT efficacy of chlorin e6 in Ce6-PVP formulations are discussed.

Photosensitized Singlet Oxygen Luminescence from the Protein Matrix of Zn-Substituted Myoglobin

A nanosecond laser near-infrared spectrometer was used to study singlet oxygen ((1)O2) emission in a protein matrix. Myoglobin in which the intact heme is substituted by Zn-protoporphyrin IX (ZnPP) was employed. Every collision of ground state molecular oxygen with ZnPP in the excited triplet state results in (1)O2 generation within the protein matrix. The quantum yield of (1)O2 generation was found to be equal to 0.9 ± 0.1. On the average, six from every 10 (1)O2 molecules succeed in escaping from the protein matrix into the solvent. A kinetic model for (1)O2 generation within the protein matrix and for a subsequent (1)O2 deactivation was introduced and discussed. Rate constants for radiative and nonradiative (1)O2 deactivation within the protein were determined. The first-order radiative rate constant for (1)O2 deactivation within the protein was found to be 8.1 ± 1.3 times larger than the one in aqueous solutions, indicating the strong influence of the protein matrix on the radiative (1)O2 deactivation. Collisions of singlet oxygen with each protein amino acid and ZnPP were assumed to contribute independently to the observed radiative as well as nonradiative rate constants.

Dynamics and efficiency of the photosensitized singlet oxygen formation by chlorin e6: The effects of the solution pH and polyvinylpyrrolidone

The effects of the solution pH and polyvinylpyrrolidone on the dynamics and efficiency of the formation of singlet oxygen 1O2 in buffer media (pH 6.3–8.5) photosensitized by chlorin e6 are studied. It is demonstrated that the quantum yield of the 1O2 formation photosensitized by chlorin e6 decreases with decreasing solution pH due to the aggregation of photosensitizer molecules. Polyvinylpyrrolidone facilitates the disaggregation of chlorin e6, thus increasing its photosensitizing ability. For a complex of chlorin e6 with this polymer, the luminescence kinetics of singlet oxygen is inverted, which should be taken into account in the determination of the lifetime of 1O2 in real biological systems.

Does photodissociation of molecular oxygen from myoglobin and hemoglobin yield singlet oxygen

Time-resolved luminescence measurements in the near-infrared region indicate that photodissociation of molecular oxygen from myoglobin and hemoglobin does not produce detectable quantities of singlet oxygen. A simple and highly sensitive method of luminescence quantification is developed and used to determine the upper limit for the quantum yield of singlet oxygen production. The proposed method was preliminarily evaluated using model data sets and confirmed with experimental data for aqueous solutions of 5,10,15,20-tetrakis(4-N-methylpyridyl) porphyrin. A general procedure for error estimation is suggested. The method is shown to provide a determination of the integral luminescence intensity in a wide range of values even for kinetics with extremely low signal-to-noise ratio. The present experimental data do not deny the possibility of singlet oxygen generation during the photodissociation of molecular oxygen from myoglobin and hemoglobin. However, the photodissociation is not efficient to yield singlet oxygen escaped from the proteins into the surrounding medium. The upper limits for the quantum yields of singlet oxygen production in the surrounding medium after the photodissociation for oxyhemoglobin and oxymyoglobin do not exceed 3.4×10(-3) and 2.3×10(-3), respectively. On the average, no more than one molecule of singlet oxygen from every hundred photodissociated oxygen molecules can succeed in escaping from the protein matrix.

Molecular oxygen migration through the xenon docking sites of human hemoglobin in the R-state.

A nanosecond laser flash-photolysis technique was used to study bimolecular and geminate molecular oxygen (O2) rebinding to tetrameric human hemoglobin and its isolated α and β chains in buffer solutions equilibrated with 1atm of air and up to 25atm of xenon. Xenon binding to the isolated α chains and to the α subunits within tetrameric hemoglobin was found to cause a decrease in the efficiency of O2 escape by a factor of ~1.30 and 3.3, respectively. A kinetic model for O2 dissociation, rebinding, and migration through two alternative pathways in the hemoglobin subunits was introduced and discussed. It was shown that, in the isolated α chains and α subunits within tetrameric hemoglobin, nearly one- and two-third escaping molecules of O2 leave the protein via xenon docking sites, respectively. The present experimental data support the idea that O2 molecule escapes from the β subunits mainly through the His(E7) gate, and show unambiguously that, in the α subunits, in addition to the direct E7 channel, there is at least one alternative escape route leading to the exterior via the xenon docking sites.

Dependence of the spontaneous emission of singlet oxygen on the refractive index and molecular polarizability of the surrounding dielectric media

The rate constants (kr) for singlet oxygen O2 (a1Δg) luminescence in several selected solvents and in binary solvent mixture (acetone-toluene) were measured. All data have been normalized such that krrel = 1.0 in toluene. It has been demonstrated that the changes in these rate constants were caused both by optical properties of a medium (the local field factor and density of photon states) and by an inherent property of the emitter of 1O2 (the square of transition moment). In its turn, the value of the transition moment is directly proportional to molecular polarizability of the medium molecules.

A comparative analysis of photoinduced tumors necrosis with/without a photosensitizer

The results of an irradiation of sensitized and non-sensitized tumors Pliss lymphosarcoma are presented in the paper. The experimental data and the theoretical calculations show, that hemoglobin can be considered as a primary agent, the photoexcitation of which induces cytotoxic reactions resulting in a tumors destruction without an exogenous singlet oxygen photosensitizer. Several mechanisms of a laser action on biological tissues, which can hypothetically influence on PDT efficiency, are discussed in the paper.