The role of photosensitizer molecular charge and structure on the efficacy of photodynamic therapy against Leishmania parasites

Photodynamic therapy (PDT) is emerging as a potential therapeutic modality in the clinical management of cutaneous leishmaniasis (CL). In order to establish a rationale for effective PDT of CL, we investigated the impact of the molecular charge and structure of photosensitizers on the parasitic phototoxic response. Two photosensitizers from the benzophenoxazine family that bear an overall cationic charge and two anionic porphyrinoid molecules were evaluated. The photodynamic activity of the photosensitizers decreases in the following order: EtNBSe > EtNBS > BpD > PpIX. The studies suggest that compared to hydrophobic anionic photosensitizers, the hydrophilic cationic benzophenoxazine analogs provide high effectiveness of PDT possibly due to (1) their strong attraction to the negatively charged parasitic membrane, (2) their hydrophilicity, (3) their high singlet oxygen quantum yield, and (4) their efficacy in targeting intracellular organelles.     

Rapid evaluation of the Voigt function and its use for interpreting X-ray photoelectron spectroscopic data

While the Voigt function is recognized as the best function to represent the photoelectron spectroscopic process, it is less frequently used because it cannot be represented as an analytical function and thus has to be evaluated numerically. This paper shows how the true Voigt function can be calculated rapidly with approximately the same speed as pseudo-Voigt functions by using approaches that have been used by the astronomical sciences community. The Voigt function is calculated using code previously published by Wells. The paper describes a method for calculating the function to generate photoelectron peaks for curve fitting X-ray photoelectron spectroscopic data. An appendix is provided with the listing of a Fortran 90 program which uses the subroutine HUMDEV published by Wells. Examples of using this approach for the fitting of experimental core X-ray photoelectron spectroscopic data are presented, and the fits compared with fits using a pseudo Voigt product function. The use of the true Voigt function in the calculation of spectra in the core and valence band region is also described and illustrated by comparing the calculated spectra with experimental spectra.     

A rapid and precise probe for measurement of liquid xenon polarization

The relaxation time of liquid (129)Xe is very long (>15 min) and the signal at thermal equilibrium is weak. Therefore, determination of the absolute polarization enhancement of hyperpolarized (129)Xe by direct measurement is tedious. We demonstrate a fast and precise alternative, based on the dipolar field created by liquid hyperpolarized (129)Xe contained in a cylindrical sample tube. The dipolar field is homogeneous in the bulk of the tube and adds to the external field, causing a shift in the Larmor frequencies of all nuclear spins. We show that the frequency shift of the proton in CHCl(3) (chloroform), which dissolves homogeneously in xenon over a fairly broad temperature range, is an excellent probe for (129)Xe polarization. Frequency measurements are precise and the experiment is much faster than by direct measurement. Furthermore the (129)Xe polarization is minimally disturbed since no rf pulses are applied directly to (129)Xe and since chloroform is a fairly weak source of (129)Xe relaxation. The experiments are reproducible and require only standard NMR instrumentation.     

PHOTODYNAMIC DESTRUCTION OF LYSOSOMES MEDIATED BY NILE BLUE PHOTOSENSITIZERS

Previous studies have established that a number of Nile blue derivatives are potent photosensitizers and that they are localized primarily in the lysosomes. The present study examines whether the lysosome is a main target of the photocytotoxic action mediated by these sensitizers. Chosen for this study were NBS-61 and sat-NBS, which represented, respectively, derivatives with high and moderate degrees of lysosomal selectivity. Overall results indicated that both derivatives are very effective in mediating a photodestruction of lysosomes. This is indicated by the light-and drug-dose-dependent losses of acid phosphatase staining particles, reduction of hexosaminidase in the lysosomecontaining subcellular fraction, and impairment of the lysosomes to take up and sequester acndine orange. Ultrastructurally, swollen and ruptured lysosomes were seen as one of the first evidences of cell damage mediated by these photosensitizers. However, the study also showed that sat-NBS, which is less lysosomal selective, was less effective in mediating lysosomal destruction. Also, the degree of lysosomal destruction mediated by sat-NBS did not parallel the degree of cytotoxicity generated. This implies that for derivatives that are not exclusively localized in the lysosome, other subcellular sites may also be damaged by the photodynamic action and may play a role in the photocytotoxic process.     

The Primary Electroviscous Effect: Thin Double Layers (akappa>1) and a Stern Layer

The primary electroviscous effect due to the charge clouds surrounding spherical charged particles suspended in an electrolyte was studied by Hinch and Sherwood (J. Fluid Mech. 132, 337 (1983)) in the limit of double layers thin compared to the particle radius a. Here we introduce the effect of a dynamic Stern layer into that analysis, in order to explain the numerical results of Rubio-Hernández et al. (J. Colloid Interface Sci. 206, 334 (1998)) in terms of the ratio of the tangential ionic fluxes within the charge cloud to those within the Stern layer. The predictions of the asymptotic analysis are compared with those of numerical computations. The thickness of the charge cloud is characterized by the Debye length kappa(-1). If akappa>10 the predictions of the asymptotic analysis exhibit the same qualitative behavior as the numerical results, but akappa>1000 is required to achieve quantitative agreement to within 2.5%. Copyright 2000 Academic Press.