Abstract:
An optical add-drop multiplexer which is tunable within a wide tuning range is provided. The device is based on the use of tunable Bragg gratings (2; 20, 21) which form the means for selecting the carrier or carriers to be inserted and extracted, and optical circulators (1, 3) which form input-output ports for the multiplexed stream to be subjected to the extraction and insertion operations and for the multiplexed flow resulting from this operation, and extraction and insertion ports for the carrier or carriers concerned. The gratings (20; 21) are associated with a phase control element (7) which acts in such a way as to disable the extraction function during a tuning transient.
Abstract:
L'invention concerne un dispositif de compensation de la dispersion chromatique comprenant un réseau de Bragg long à pas variable inscrit sur une fibre optique (10) dans laquelle se propage une pluralité de canaux de transmission multiplexés en longueur d'onde, caractérisé en ce que le dispositif comporte des moyens de génération d'un gradient thermique généré par au moins deux moyens de chauffage (20) répartis sur ledit réseau et contrôlés indépendamment l'un de l'autre de manière à compenser simultanément la dispersion chromatique sur plusieurs desdits canaux de transmission.
Abstract:
The present invention proposes optical fiber equipment (10) having a Bragg grating tunable by a piezoelectric actuator, the equipment comprising an optical fiber (1), a Bragg grating (2) photoinduced in said fiber, a support (3) for supporting said fiber and comprising two uprights (30, 31) at opposite ends of said Bragg grating, each upright having a first holding element (32, 33) for holding said fiber, and a piezoelectric actuator (4) held via its ends between the two uprights, said actuator being longitudinally prestressed in compression between said uprights.
Abstract:
Described herein is an integrated optical device (400) having an input path (402) and an output path (420). A waveguide (430) including a Bragg grating is located in the output path (420). A plurality of control elements are located along the waveguide (430) for providing local adjustment of the Bragg grating to compensate for manufacturing errors. The control elements are conveniently thermo-optic elements, for example, resistive elements whose temperature can be changed by supplying current to them.
Abstract:
The invention relates to an electronically adjustable Bragg-grating filter module (FM) which comprises a piezoelectric actuator (1) with which the length of the Bragg-grating filter (3) can be modified. The change in length of the Bragg-grating filter can be precisely measured by means of a strain gauge (4). Since the centre frequency of the Bragg-grating filter (3) depends on its length this permits an indirect adjustment of the frequency. The above filter is especially suitable for remote-controlled add-drop modules (ADM). To eliminate the influences of the piezoelectric element during adjustment of the Bragg-grating filter frequency adjustment is carried out by means of a regulator circuit.
Abstract:
A dynamically tunable filter (10) controls the magnitude of couplings between core (16) and cladding (18) modes of a waveguide by surrounding the waveguide with an overcladding (20) having an adjustable refractive index. The coupled modes are attenuated along the core to produce the desired spectral response. The adjustment to the overcladding (20) index is made in a range that is above the refractive index of the underlying cladding (18) to vary amplitudes of attenuated bands of wavelengths without shifting central wavelengths of the bands.
Abstract:
The invention relates to an electronically adjustable Bragg-grating filter module (FM) which comprises a piezoelectric actuator (1) with which the length of the Bragg-grating filter (3) can be modified. The change in length of the Bragg-grating filter can be precisely measured by means of a strain gauge (4). Since the centre frequency of the Bragg-grating filter (3) depends on its length this permits an indirect adjustment of the frequency. The above filter is especially suitable for remote-controlled add-drop modules (ADM). To eliminate the influences of the piezoelectric element during adjustment of the Bragg-grating filter frequency adjustment is carried out by means of a regulator circuit.
Abstract:
A wavelength selective resonant grating exhibits transmission resonances when a single gap between two sections of a split gratings is used to provide a phase shift which is not a quarter wavelength in length or π/2 in phase. When the phase is changed to non -π/2 values (or the gap differs from a quarter wave), the transmission resonance moves from the center of the stop band. Appropriate adjustments of the phase over a π interval allow tuning of the resonance across the entire stop band. The resonant optical wavelength grating can, illustratively, be used as wavelength filter, wavelength monitor, or as part of an Add/Drop arrangement.
Abstract:
Disclosed is an optical system (312) and an imaging and display system using the optical system. The optical system has at least first (330) and second (332) optical elements aligned on a common axis (334). In one embodiment, each of the first and second optical elements can operate in an active state or in inactive state and comprise a photopolymer and liquid crystal combination (12). Each of the first and second optical elements is configured to transmit incident light substantially unaltered when each of the first and second optical elements operates in the inactive state. In the active state, however, each of the first and second optical elements does not transmit incident light substantially unaltered. Rather each of the first and second optical elements substantially alters light incident thereon when each of the first and second optical elements operates in the active state.