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Showing papers by "Pietro Ferraro published in 1995"


Patent
08 Mar 1995
TL;DR: In this paper, an embedded optical sensor has a plurality of layers (10-20) and an optical fiber (21) with a fiber grating (28), disposed between the layers (14, 16).
Abstract: An embedded optical sensor has a plurality of layers (10-20) and an optical fiber (21) with a fiber grating (28), disposed between the layers (14, 16). The layers (10-20) comprise filaments (22) and resin (24) which have different thermal expansion coefficients and the filaments (22) are oriented so as to create unequal transverse residual stresses that act through the geometry of a resin-rich region that surrounds on the grating (28) in the fiber (21). The unequal transverse residual stresses cause birefringence in the grating (28), thereby causing the grating (28) to reflect light (32) having two wavelengths with a predetermined separation, each along a different polarization axis. The wavelength separation and average wavelength between such separation have different sensitivities to temperature and strain, thereby allowing independent temperature and strain measurements using only a single grating. The birefringence is maximized when the filaments (22) of the adjacent layers (10, 12) are oriented at 90 degrees with respect to the longitudinal (Z-axis) of the fiber (21).

161 citations


Journal ArticleDOI
S. De Nicola1, Pietro Ferraro1, Andrea Finizio1, Giuseppe Pesce1, Giovanni Pierattini1 
TL;DR: In this paper, a new design of interferometer which makes use of a reflective-type diffraction grating is developed, which is easy to align and compact and it is suitable for measuring the refractive indices of transparent materials.

46 citations



Journal ArticleDOI
TL;DR: In this article, an optical heterodyne polarization interferometer was proposed for the precision measurement of the change in the state of polarization of a light wave induced by polarizing optical devices.
Abstract: We describe an optical heterodyne polarization interferometer that can be efficiently used for the precision measurement of the change in the state of polarization of a light wave induced by polarizing optical devices. This technique is used to measure the change with wavelength of the phase retardation of a quarter-wave plate. A theoretical derivation is presented to permit computation of the wavelength dependence of the phase shift induced by a quarter-wave plate.

4 citations


Journal ArticleDOI
TL;DR: In this article, a simple general method for particle tracking and velocity field determination from the reconstruction of holographic images is reported, and a preliminary experimental application is reported. But this method is limited to the case of holograms.
Abstract: A simple general method is reported for particle tracking and velocity field determination from the reconstruction of holographic images. A preliminary experimental application is reported.

3 citations


Patent
08 Mar 1995
TL;DR: In this paper, a capteur optique integre presente une pluralite de couches (10-20), and a fibre optique dotee d'un reseau de fibre (28) and prevue entre les couches.
Abstract: Un capteur optique integre presente une pluralite de couches (10-20), et une fibre optique dotee d'un reseau de fibre (28) et prevue entre les couches (14-16). Les couches (10-20) sont constituees de filaments (22) et de resine (24) presentant des coefficients de dilatation thermique differents, les filaments etant orientes de sorte que des efforts residuels transversaux inegaux agissant a travers la geometrie d'une region riche en resine entourant le reseau (28) dans la fibre (21) soient crees. Les efforts residuels transversaux inegaux provoquent une birefringence dans le reseau (28), lequel reflechit alors de la lumiere (32) a deux longueurs d'onde a separation predeterminee, chacune le long d'un axe de polarisation different. La separation des longueurs d'onde et la longueur d'onde moyenne de chaque cote de ladite separation presentent des sensibilites differentes a la temperature et aux contraintes, ce qui permet une mesure separee de la temperature et des contraintes au moyen d'un seul reseau. La birefringence est maximisee lorsque les filaments (22) des couches adjacentes (10, 12) sont orientes a 90° par rapport a l'axe longitudinal (axe des Z) de la fibre (21).