2011
Authors
Szczurowski, MK; Frazao, O; Baptista, JM; Nielsen, K; Bang, O; Urbanczyk, W;
Publication
21ST INTERNATIONAL CONFERENCE ON OPTICAL FIBER SENSORS
Abstract
We experimentally studied several sensing characteristics of a birefringent microstructured polymer optical fiber. The fiber exhibits a birefringence of the order 2x10(-5) at 1.3 mu m because of two small holes adjacent to the core. In this fiber, we measured spectral dependence of phase and group modal birefringence, bending losses, polarimetric sensitivity to strain and temperature. The sensitivity to strain was also examined for intermodal interference observed in the spectral range below 0.8 mu m. Finally, we showed that the material transmission windows shift as function of the applied strain. This shift has an exponential character and saturates for greater strain.
2011
Authors
Ferreira, MS; Baptista, JM; Roy, P; Jamier, R; Fevrier, S; Frazao, O;
Publication
OPTICS LETTERS
Abstract
A highly birefringent photonic bandgap Bragg fiber loop mirror configuration for simultaneous measurement of strain and temperature is proposed. The group birefringence and the sharp loss peaks are observable in the spectral response. Because the sensing head presents different sensitivities for strain and temperature measurands, these physical parameters can be discriminated by using the matrix method. It should be noted that this Bragg fiber presents high sensitivity to temperature, of similar to 5.75 nm/degrees C, due to the group birefringence variation. The rms deviations obtained are +/- 19.32 mu e and +/- 0.5 degrees C, for strain and temperature measurements, respectively. (C) 2011 Optical Society of America
2011
Authors
Baptista, JM; Correia, C; Marques, MB; Frazao, O;
Publication
LASER PHYSICS
Abstract
In this work, a laser sensor is described that uses the multipath interference produced inside a ring cavity to measure the power loss induced by a moving taper intensity sensor. The laser is created due to the virtual distributed mirror formed by the Rayleigh scattering produced in a dispersion compensating fiber when pumped by a Raman laser. Two laser peaks were formed, one of them is obtained by the Raman gain (1555 nm) inside the ring and the second is created by the combination of the Raman gain and the Rayleigh scattering (1565 nm). A taper sensor is used as displacement sensor and when the losses is applied in the taper the second laser peak is reduced and the first peak is maintained constant and can be used as reference level.
2011
Authors
Frazao, O; Baptista, JM; Kobelke, J; Schuster, K;
Publication
Photonic Crystals: Optical Properties, Fabrication and Applications
Abstract
The index-guiding PCF basic structure is a solid core surrounded by a microstructured cladding. Owing to the presence of air holes, the effective refractive index of the cladding is below that of the core and the light is guided along the core by the principle of total internal reflection. Several authors have presented different geometries for this type of fibre and one of them is the suspended-core structure, where relatively large holes surround the fibre core that looks suspended along the fibre axis by small width silica walls. The chapter is divided in two parts. The first is about the fabrication of suspended core fibre and the second part is about the main applications of this type of fibres as interferometers.
2011
Authors
Fernandes, LA; Grenier, JR; Kim, JH; Herman, PR; Aitchison, JS; Marques, PVS;
Publication
Optics InfoBase Conference Papers
Abstract
Femtosecond laser fabrication of optical waveguides in bulk silica glass is extended to integrated optical waveplates. Polarization retardation was controlled by laser exposure, providing for trimming of waveguide birefringence between 10-5 and 10-4. © OSA/ CLEO 2011.
2011
Authors
Viegas, J; Mayeh, M; Marques, P; Farahi, F;
Publication
Optics InfoBase Conference Papers
Abstract
An integrated optical refractometer based on multimode interference, with sensitivity enhancement due to sub-micrometer axial features, is demonstrated with experimental sensitivity as high as 3200 nm/RIU and resolution limits on the order of 5 ppm. © OSA/CLEO 2011.
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