Abstract:
An electrooptical device is provided comprising at least one substrate, at least one pair of electrodes and at least one layer of an electrooptical material. The electrooptical material represents an optically anisotropic thin crystal film and contains molecules having aromatic rings and possessing a lattice with an interplanar spacing (Bragg's reflection) of 3.4null0.2 {acute over (null)} along one of optical axes. The electrooptical material has anisotropic refractive indices and/or anisotropic absorption coefficients that are depended on an electric field strength.
Abstract:
The invention relates to a tuneable optical grid-assisted add/drop filter in codirectional mode of operation, which has the structure of a directional coupler filter with at least two adjacent waveguides having different refractive indices. The inventive filter must exhibit a spectral bandwidth of the filter transmission curve in the range from 50 GHz to 400 GHz for a high resolution in order to be tuneable and it must be producible in a more straightforward and more cost-effective manner, with dimensional tolerances higher than those of InP based add/drop filters. For that purpose, the material of the two waveguides is composed of two different classes of materials having different optical parameters. The thermal refraction index coefficient dn/dT, the electro-optic coefficient dn/dE or the dispersion dn/dnull of these two materials differentiate from each other in such a way that, in case of an action carried out upon the two waveguides with the same technical means with a view to changing the temperature, the electric field or the wavelength, effects with different strength occur and therefore, means for changing these parameters are provided. A polymer and silica are used as wave guide materials arranged vertically or horizontally relative to each other. For changing the optical parameter dn/dT, a device for modifying the temperature is used to influence the whole surface of a chip which contains the filter, said device being possibly identical to a device fore stabilizing the chip temperature.
Abstract:
An optoelectric component has two waveguide layers and a layer with a periodic structure, which layers are arranged parallel to one another and are dimensioned so that a codirectional coupling is produced between modes guided in each of the waveguide layers. In order to prevent undesirable reflections, changes in the effective refractive index in the periodic structure is gradually changed along the direction of propagation. This change can be by the boundary of the periodic structure extending at an angle other than a right angle to the direction of propagation, either in a vertical or a lateral direction. The change can also be accomplished by a gradual change of the composition at the boundary of the periodic structure and adjacent portions or sections.
Abstract:
An optical waveguide (20) is comprised of a core layer (20) fabricated on an interference layer (18). The interference layer (18) is supported by a lower cladding layer (16) deposited on a semiconductor substrate (12), a and Light travels through the core layer and is coupled into the interference layer by a grating. An electronic element in the interference layer modulates the light passing through the interference layer. The modulated light is then coupled back into the core layer by either another portion of the grating, or a separate grating.
Abstract:
An optical apparatus consisting of a laser for producing a coherent polarized beam of electromagnetic radiation of a preselected wavelength. A substrate of silicon has a first transparent cover layer for receiving the polarized beam substantially normally incident thereto, an a second transparent guide layer for receiving the polarized beam from said first layer and for supporting at least one resonant mode. The first and second layers have a preselected index of refraction and a grating is interposed between them, having a grating period less than half the preselected wavelength. The layers and grating interact to produce a standing wave resonance by Bragg reflection. A control obtains a resonance wavelength in the guide layer equal to the predetermined radiation wavelength and thereby high reflectance to modulate the polarized beam.
Abstract:
A controllable, electro-optical grating coupler for the optional switch-over or modulation of optical waves in waveguides includes a substrate with a first areal electrode arranged on the substrate and a first dielectric layer arranged on the electrode and carrying a waveguide. A periodic grating structure is arranged in the waveguide transversely to the direction of propagation of light and either the grating structure of the waveguide consist of electro-optical material in the region of the grating structure. A second dielectric layer is arranged on the waveguide and a second areal electrode is arranged on the dielectric layer. By varying the voltage across the electrodes it is possible to amplify or reduce the interference provided by the grating structure so that the light in the waveguide is modulated, switched, scattered from the waveguide or input coupled to a second waveguide.
Abstract:
An optical coupling system comprises a prism or diffraction grating coupling element in combination with a film waveguide or the like affording high selectivity and high coupling coefficient. A prism when used has a coated, partially reflective and interference inducing face arranged parallel to the film waveguide along a coupling interval wavelength of the latter. The coated face coating includes a partially transparent mirror layer and an interference film. When a grating coupling element is used, multiple interfering beams ordinarily produced are reduced to one output beam per diffraction order. Light beams may be propagated on one or both sides of the film.
Abstract:
Diffracted leaky optical waves are coupled out of a thin film optical waveguide device having one surface which is periodically thickness-modulated or corrugated to form an optical diffraction grating. The waveguide device is constructed such that the average thickness of the waveguide in the complex refractive index of the waveguide or one of the layers surrounding the waveguide is varied when an external power source applied to the device is varied and thereby, a parameter of the leaky wave in accordance with the variable power source. In one embodiment, the waveguide is made of light amplifying material which is suitably excited to produce lasing action and cause an optical wave to propagate in the waveguide. The variable parameter in this case is the wavelength of the leaky wave, and the leaky wave is always normal to the plane of the diffraction grating. Consequently, a tunable laser is provided. In a second embodiment, no lasing occurs, but instead, an external light source is used to cause an optical wave to propagate in the waveguide. The parameter which is varied is the angle between the leaky wave and the normal to the diffraction grating, the wavelength of the leaky wave remaining constant.
Abstract:
An optical modulator includes a carrier and a waveguide disposed on the carrier. The waveguide includes a first optical coupling region, a second optical coupling region, first regions, and second regions. The first optical coupling region is doped with first dopants. The second optical coupling region abuts the first optical coupling region and is doped with second dopants. The first dopants and the second dopants are of different conductivity type. The first regions are doped with the first dopants and are arrange adjacent to the first optical coupling region. The first regions have respective increasing doping concentrations as distances of the first regions increase from the first optical coupling region. The second regions are doped with the second dopants and are arranged adjacent to the second optical coupling region. The second regions have respective increasing doping concentrations as distances of the second regions increase from the second optical coupling region.
Abstract:
A beam-steering device (100) for spatial steering of a light beam comprises a waveguide array (10) being arranged on a substrate (50) and comprising a waveguide array input (12), multiple waveguides (14-1, 14-2, . . . , 14-i) and a waveguide array output (16), wherein the multiple waveguides (14-1, 14-2, . . . , 14-i) are adapted for simultaneously guiding light from the waveguide array input (12) to the waveguide array output (16) and for forming a light beam downstream of the waveguide array output (16) by superimposing the light guided by the waveguides (14-1, 14-2, . . . , 14-i), a phase shifter device (18) being arranged for applying controlled phase shifts to the light guided in each of the waveguides (14-1, 14-2, . . . , 14-i), and a grating array (22) including at least one patterned grating in optical communication with the waveguide array output (16), the grating array (22) being configured to radiate the light beam out of the beam-steering device (100) to a surrounding, wherein the waveguide array output (16) is arranged such that the light beam is formed downstream of the waveguide array output (16) with a main lobe and side lobes and with a beam angle Φ in a plane of the substrate (50), that is determined by the controlled phase shifts applied to the light by the phase shifter device (18) and a wavelength of the light, a slab propagation region (20) is arranged between the waveguide array output (16) and the grating array (22) such that the main lobe of the light beam is angularly relayed to the grating array (22) and the side lobes of the light beam leave lateral sides of the slab propagation region (20) before reaching the grating array (22), and the grating array (22) is arranged to radiate the light beam out of the beam-steering device (100) with a first angular direction with respect to the substrate (50), that is determined by the beam angle Φ. Furthermore, a method of beam-steering a light beam is described.