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1.
Chemosphere ; 182: 681-690, 2017 Sep.
Artigo em Inglês | MEDLINE | ID: mdl-28528314

RESUMO

The aim of this study was to develop and calibrate a macroporous ceramic passive sampler (MCPS) for the monitoring of anticancer drugs in wastewater. This system was designed by the Spanish Research Council (CSIC) and consists in a porous ceramic tube to allow a high diffusion of contaminants. The MCPS has been calibrated for 16 cytostatic drugs over time periods up to 9 d in spiked water under controlled laboratory conditions. Optimal uptake was accomplished for 7 compounds, namely ifosfamide, cyclophosphamide, capecitabine, prednisone, megestrol, cyproterone and mycophenolic acid, whereas cytarabine was not adsorbed in the receiving phase and the rest were hydrolyzed over the deployment period. The sampling rate for these 7 compounds was between 0.825 and 3.350 mL day-1 and the diffusion coefficients varied from 1.01E-07 to 4.12E-07 cm2 s-1. To prove the applicability of the MCPSs, samplers (n = 3) were deployed in influent and effluent waters of a WWTP for a period of 6 d and results were compared to grab sampling and extraction with Solid Phase Extraction (SPE). In influent waters, MCPS were clogged due to the high amount of suspended solids in these waters. In effluents, MCPS detected cyclophosphamide and mycophenolic acid at concentrations of 19 ± 3 and 136 ± 28 ng L-1 with a good agreement with the levels obtained by grab sampling. The study discusses the use and performance of the MCPS for the monitoring of stable cytostatic compounds in a complex matrix such as wastewater.


Assuntos
Antineoplásicos/química , Cerâmica/química , Citostáticos/química , Monitoramento Ambiental/métodos , Poluentes Químicos da Água/química , Extração em Fase Sólida , Eliminação de Resíduos Líquidos , Águas Residuárias/química , Água
2.
Opt Express ; 20(10): 10879-87, 2012 May 07.
Artigo em Inglês | MEDLINE | ID: mdl-22565713

RESUMO

The availability of macroscopic, nearly periodic structures known as eutectics opens a new path for controlling light at wavelength scales determined by the geometrical parameters of these materials and the intrinsic properties of their component phases. Here, we analyze the optical waveguiding properties of eutectic mixtures of alkali halides, formed by close-packed arrangements of aligned cylindrical inclusions. The wavelengths of phonon polaritons in these constituents are conveniently situated in the infrared and are slightly larger than the diameter and separation of the inclusions, typically consisting on single-crystal wires down to submicrometer diameter. We first discuss the gap mode and the guiding properties of metallic cylindrical waveguides in the visible and near-infrared, and in particular we investigate the transition between cylinder touching and non-touching regimes. Then, we demonstrate that these properties can be extended to the mid infrared by means of phonon polaritons. Finally, we analyze the guiding properties of an actual eutectic. For typical eutectic dimensions, we conclude that crosstalk between neighboring cylindrical wires is small, thus providing a promising platform for signal propagation and image analysis in the mid infrared.


Assuntos
Nanotecnologia/métodos , Óptica e Fotônica , Fônons , Ressonância de Plasmônio de Superfície/métodos , Desenho de Equipamento , Fluoretos/química , Ouro/química , Raios Infravermelhos , Luz , Compostos de Lítio/química , Nanopartículas Metálicas/química , Cloreto de Potássio , Espalhamento de Radiação
3.
Opt Express ; 17(6): 4382-7, 2009 Mar 16.
Artigo em Inglês | MEDLINE | ID: mdl-19293865

RESUMO

Site-selective spectroscopy and stimulated emission experiments performed in the (4)F(3/2)-->(4)I(11/2) laser transition of Nd(3+)-doped 0.8CaSiO(3-) 0.2Ca(3)(PO(4))(2) eutectic glass are presented. The spectral features of the excitation spectra and those of spontaneous and stimulated emissions reveal the existence of a very complex crystal field site distribution for Nd(3+) ions. As a consequence, the stimulated emission of Nd(3+) in this glass shows a tunability of about 10 nm as a function of excitation wavelength.

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