Curing depth of composite resin light cured by LED and halogen light-curing units

The purpose of this study was to evaluate the polymerization effectiveness of a composite resin (Z-250) utilizing microhardness testing. In total, 80 samples with thicknesses of 2 and 4 mm were made, which were photoactivated by a conventional halogen light-curing unit, and light-curing units based on LED. The samples were stored in water distilled for 24 h at 37°C. The Vickers microhardness was performed by the MMT-3 microhardness tester. The microhardness means obtained were as follows: G1, 72.88; G2, 69.35; G3, 67.66; G4, 69.71; G5, 70.95; G6, 75.19; G7, 72.96; and G8, 71.62. The data were submitted to an analysis of variance (ANOVA’s test), adopting a significance level of 5%. The results showed that, in general, there were no statistical differences between the halogen and LED light-curing units used with the same parameters.     

Comparative ablation rate from a Er: YAG laser on enamel and dentin of primary and permanent teeth

This study was conducted to analyze the ablation rate and micromorphological aspects of microcavities in enamel and dentin of primary and permanent teeth using a Er: YAG laser system. Micromorphological evaluation has been performed in terms of permanent teeth; however, little information about Er: YAG laser interaction with primary teeth can be found in the literature. Because children have been the most beneficiary patients with laser therapy in our offices, it is extremely necessary to compare the effects of this kind of laser system on the enamel and dentin of permanent and primary teeth. In this study, we used eleven intact primary anterior exfoliated teeth and six extracted permanent molar teeth. We used a commercial laser system: a Er: YAG Twin Light laser system (Fotona Medical Lasers, Slovenia) at 2940 nm, changing average energy levels per pulse (100, 200, 300, and 400 mJ) producing 48 microcavities in enamel and dentin of primary and permanent teeth. Primary teeth are more easily ablated than are permanent teeth, when related to enamel or dentin. However, while this laser system is capable of slowly revealing the enamel’s microstructure, in dentin only the lowest laser energies permit this kind of observation, more easily decomposing the original tissue aspect, when related to primary or permanent teeth. Statistically, the only different factor at the 5% level was an energy per pulse of 400 mJ, confirming the results found in SEM. Our results showed that dentin in both primary and permanent teeth is less resistant to Er: YAG laser ablation; this fact is easily observed under SEM observation and through the ablation rate evaluation.     

Observation of ultracold ground-state heteronuclear molecules

We report the observation of translationally ultracold heteronuclear ground-state molecules in a two-species magneto-optical trap containing 39K and 85Rb atoms. The KRb molecules are produced via photoassociation and detected by multiphoton ionization. We had characterized their temperature and measured their formation rate constant. We believe that the two-species trap could be used as a reliable source of ultracold molecules to be captured by electrostatic, magnetic, or optical traps. This possibility will certainly motivate further investigation of quantum collective effects as well as high-resolution spectroscopy of the rovibrational level structure of cold heteronuclear molecular systems.     

Trap loss rate for heteronuclear cold collisions in two species magneto-optical trap

In this paper we review the present status on heteronuclear trap loss rate ( ) for alkali mixtures held in a magneto-optical trap (Na-K, Na-Rb, Na-Cs, K-Rb, Rb-Cs, Li-Cs). The intensity dependence of the for the mixture Cs-K is also presented for the first time in this report. The measurement techniques and a semiclassical model, considering both excited-ground and doubly excited channels, are reviewed. The comparison between the model and the experimental results indicates that radiative escape may be the dominant loss process for heteronuclear cold collisions. The obtained values for the crossed species trap loss indicate possibilities of future experiments involving such mixtures in a two species condensate.Received: 19 January 2004, Published online: 11 May 2004PACS: 32.80.Pj Optical cooling of atoms; trapping - 33.80.Ps Optical cooling of molecules; trapping - 34.50.Rk Laser-modified scattering and reactions     

Comparative investigation of <Emphasis Type="Bold">39</Emphasis>K and <Emphasis Type="Bold">40</Emphasis>K trap loss rates: alternative loss channel at low light intensities

We report a comparative investigation of trap loss rates in a magneto-optical trap for two potassium isotopes, ³⁹K and ⁴⁰K, as a function of trap light intensity. The isotopes present a quite similar behavior for the loss rates at high intensities, and a sudden increase of the loss rates at low intensities is present in both cases. While for ³⁹K such increase can be explained assuming that the major contribution to the losses comes from hyperfine changing collisions, a different loss mechanism must be considered for ⁴⁰K, which has an inverted ground state hyperfine structure. The experimental results of both isotopes are well reproduced by an alternative model based on radiative escape as the dominant loss mechanism. Received 1st May 2002 / Received in final form 19 October 2002 Published online 4 March 2003 RID="a" ID="a"Alternative address: Dipartimento di Fisica, Universitá di Trento, 38050 Povo (Tn), Italy. RID="b" ID="b"e-mail: marcassa@if.sc.usp.br     

Photodynamic activity of different dyes

Photodynamic therapy (PDT) is a technique for inducing tissue damage with light irradiation of a drug selectively retained in malignant tissue. Many kinds of compounds are known with photosensitizing properties including dyes, drugs, cosmetics, chemicals, and many natural substances. There are different classes of sensitizers used for medical purposes such as tetrapyrroles (porphyrins and derivatives, chlorophyll, phylloerythrin, phthalocyanines), tricyclic dyes with different meso-atoms (acridine orange, proflavine, riboflavine, methylene blue, fluorescein, eosine, erythrosine, rose bengal), and furocoumarins (psoralen and its methoxyderivatives xanthotoxin, bergaptene). In this work, we performed one comparative cytotoxic study of the photodynamic activity presented by tricyclic dyes (methylene blue, fluorescein and erythrosine) and the commercial Russian photosensitizer Photogem® (hematoporphyrin derivative). For this purpose, three cell lines were used: HEp-2 (tumor cells), VERO and McCoy (nontumor cells), and a yeast strain. The wavelength used for irradiation was 630 nm, the same as used in PDT for medical purposes, since it is in the therapeutic window, i.e., where light can penetrate more into the tissues. The results suggest that Photogem® is more cytotoxic and more photocytotoxic than the studied tricyclic dyes in nontumor and tumor cells. These dyes present less cytotoxicity (around half) in normal cells (dark and light) than in tumor cells. In the experiments with microorganisms, methylene blue presented a better photodynamic effect than Photogem®. These results can be explained by the fact that it is more difficult for Photogem® to penetrate in microorganism membranes than mammalian cell membranes. As for Photogem®, these tricycle dyes present a higher cytotoxicity in tumor cells. These data suggest that methylene blue can be an option in photodynamic inactivation as well as in photodynamic therapy, mainly for superficial lesions.     

Cellular and tissue effects induced by photogem® and red LED in photodynamic therapy

In order to consider the photodynamic therapy (PDT) as a clinical treatment for candidosis, it is necessary to know its cytotoxic effect on normal cells and tissues. Therefore, this study evaluated the toxicity of PDT with Photogem® associated with red light-emitting diode (LED) on L929 and MDPC-23 cell cultures and healthy rat palatal mucosa. In the in vitro experiment, the cells (30000 cells/cm²) were seeded in 24-well plates for 48 h, incubated with Photogem® (50, 100, or 150 mg/l) and either irradiated or not with a red LED source (630 ± 3 nm; 75 or 100 J/cm²; 22 mW/cm²). Cell metabolism was evaluated by the MTT assay (ANOVA and Dunnet’s post hoc tests; p < 0.05) and cell morphology was examined by scanning electron microscopy. In the in vivo evaluation, Photogem® (500 mg/l) was applied to the palatal mucosa of Wistar rats during 30 min and exposed to red LED (630 nm) during 20 min (306 J/cm²). The palatal mucosa was photographed for macroscopic analysis at 0, 1, 3, and 7 days posttreatment and subjected to histological analysis after sacrifice of the rats. For both cell lines, there was a statistically significant decrease of the mitochondrial activity (90–97%) for all Photogem® concentrations associated with red LED regardless of the energy density. However, in the in vivo evaluation, the PDT-treated groups presented intact mucosa with normal characteristics both macroscopically and histologically. From these results, it may be concluded that the association of Photogem® and red LED caused severe toxic effects on normal cell cultures, characterized by the reduction of mitochondrial activity and morphological alterations, but did not cause damage to the rat palatal mucosa in vivo.     

PANI–WO3·2H2O Nanocomposite: Phase Interaction and Evaluation of Electronic Properties by Combined Experimental Techniques and Ab-Initio Calculation

The development of conjugated polymer-based nanocomposites by adding metallic particles into the polymerization medium allows the proposition of novel materials presenting improved electrical and optical properties. Polyaniline Emeraldine-salt form (ES–PANI) has been extensively studied due to its controllable electrical conductivity and oxidation states. On the other hand, tungsten oxide (WO₃) and its di-hydrated phases, such as WO₃·2H₂O, have been reported as important materials in photocatalysis and sensors. Herein, the WO₃·2H₂O phase was directly obtained during the in-situ polymerization of aniline hydrochloride from metallic tungsten (W), allowing the formation of hybrid nanocomposites based on its full oxidation into WO₃·2H₂O. The developed ES–PANI–WO₃·2H₂O nanocomposites were successfully characterized using experimental techniques combined with Density Functional Theory (DFT). The formation of WO₃·2H₂O was clearly verified after two hours of synthesis (PW₂ nanocomposite), allowing the confirmation of purely physical interaction between matrix and reinforcement. As a result, increased electrical conductivity was verified in the PW₂ nanocomposite: the DFT calculations revealed a charge transfer from the p-orbitals of the polymeric phase to the d-orbitals of the oxide phase, resulting in higher conductivity when compared to the pure ES–PANI.     

Photobleaching Kinetics and Effect of Solvent in the Photophysical Properties of Indocyanine Green for Photodynamic Therapy

Indocyanine green is an attractive molecule for photodynamic therapy due to its near infrared absorption, resulting in a higher tissue penetration. However, its quantum yields of the triplet and singlet state have been reported to be low and then, reactive oxygen species are unlikely to be formed. Aiming to understand the ICG role in photodynamic response, its photobleaching behavior in solution has been studied under distinct conditions of CW laser irradiation at 780 and 808 nm, oxygen saturations and solvents. Sensitizer bleaching and photoproduct formation were measured by absorption spectroscopy and analyzed using the PDT bleaching macroscopic model to extract physical parameters. ICG photobleaching occurs even at lower oxygen concentrations, indicating that the molecule presents more than one way of degradation. Photoproducts were produced even in solution of less than 4 % oxygen saturation for both solvents and excitation wavelengths. Also, the amplitude of absorption related to J-dimers was increased during irradiation, but only in 50 % PBS solution. The formation of photoproducts was enhanced in the presence of J-type dimers under low oxygen concentration, and the quantum yields of triplet and singlet states were one order of magnitude and two times higher, respectively, when compared to ICG in distilled H₂O.