Abstract:
A tunable photonic crystal device comprising: alternating layers of a first material and a second material, the alternating layers comprising a responsive material, the responsive material being responsive to an external stimulus, the alternating layers having a periodic difference in refractive indices giving rise to a first reflected wavelength; wherein, in response to the external stimulus, a change in the responsive material results in a reflected wavelength of the device shifting from the first reflected wavelength to a second reflected wavelength.
Abstract:
Disclosed is a photonic crystal semiconductor device which enables to easily form various optical devices having a photonic crystal structure by using a semiconductor and a semiconductor manufacturing process. Also disclosed is a method for manufacturing such a photonic crystal semiconductor device. The photonic crystal semiconductor device has a photonic crystal structure wherein a lower DBR layer (1), a core layer (2), an upper DBR layer (3) and a dielectric multilayer film (6) composed of multiple dielectric layers are sequentially formed on an n-InP substrate (11) in this order. A plurality of vacancies (9) are formed in the core layer (2) and the upper DBR layer (3) in the film thickness direction, and a line defect portion (10) is in the region between the vacancies (9) where no vacancy (9) is present. The line defect portion (10) functions as an optical waveguide.
Abstract:
An optical wavelength converting device is provided with a LiTaO3 substrate, a plurality of inverted-polarization layers periodically arranged in an upper surface of the LiTaO3 substrate, and an optical waveguide crossing the inverted-polarization layers. The upper surface of the LiTaO3 substrate is directed toward a -X-crystal axis direction. The inverted-polarization layers are formed by exchanging Ta ions of the LiTaO3 substrate for H ions, and an extending direction of each inverted-polarization layer is inclined at an angle of theta degrees (6 ions of the LiTaO3 substrate and the inverted-polarization layers for H ions to set a refractive index of the optical waveguide higher than that of the LiTaO3 substrate. The optical waveguide extends in a +Y-crystal axis direction. Fundamental waves polarized in a transverse electric mode induce electric field directed in +/-Y-crystal axis directions and are converted into second harmonic waves in the optical waveguide.
Abstract:
A wavelength converting laser device having a Watt-level power output and high efficiency is obtained. It has a laser diode including an optical resonator having a pair of facing reflectors including a reflecting surface having a shape reducing loss in optical resonator with regard to a specific horizontal transverse mode of a laser as compared to the loss in optical resonator for other horizontal transverse modes; and a wavelength converter for converting the laser into a harmonic.
Abstract:
An optoelectronic integrated circuit comprises a substrate, a multilayer structure formed on the substrate, and an array of thyristor devices and corresponding resonant cavities formed in the multilayer structure. The resonant cavities, which are adapted to process different wavelengths of light, are formed by selectively removing portions of said multilayer structure to provide said resonant cavities with different vertical dimensions that correspond to the different wavelengths. Preferably, that portion of the multilayer structure that is selectively removed to provide the multiple wavelengths includes a periodic substructure formed by repeating pairs of an undoped spacer layer and an undoped etch stop layer. The multilayer structure may be formed from group III-V materials. In this case, the undoped spacer layer and undoped etch stop layer of the periodic substructure preferably comprises undoped GaAs and undoped AlAs, respectively. The undoped AlAs functions as an etch stop during etching by a chlorine-based gas mixture that includes fluorine. The array of multi-wavelength thyristor devices may be used to realize devices that provide a variety of optoelectronic functions, such as an array of thyristor-based lasers that emit light at different wavelengths and/or an array of thyristor-based detectors that detect light at different wavelengths (e.g., for wavelength-division-multiplexing applications).
Abstract:
According to the present invention the tunable optical device comprises a first optical wave guide and a second optical wave guide defining a space between the two wave guides with space comprises the first cell with liquid crystal material and a second cell with liquid crystal material spaced by a third wave guide and the first and the second cell for liquid crystal material having orientation of the liquid crystal material perpendicular to each other.
Abstract:
The present specification describes strain applicators, incorporating two actuators having different actuation characteristics acting in cooperation, and their use in adjustable optical filters and adjustable dispersion devices (such as compensators) to controllably strain fibre Bragg gratings to alter their reflectance characteristics. Preferred examples of the strain applicators are hybrids of a fast response actuator with a slower device, and provide a wide overall range of adjustment with fast response tuning within that range. The strain applicators are used to provide dither, in particular to provide both in-phase and anti-phase dither of the strains applied to FBGs in a twin-grating compensator. The in-phase dithering enables centering on an incoming signal to be performed and the out of phase dithering dithers the dispersion, enabling the compensator to track changes in dispersion rapidly, using an appropriately arranged control loop. An improved method of extracting a dispersion error signal from optical signals is also described, based on a simplified spectral analysis of data carried by the signals.
Abstract:
A variable optical attenuator and an optical power level adjusting method used this variable optical attenuator, which has high reliability and a wide dynamic range, are provided. The variable optical attenuator consists of an optical filter and a temperature control circuit. And the optical filter provides a dielectric multi-layer film and an optical isolator. The dielectric multi-layer film changes its transmitting characteristic of light by the change of temperature. The optical isolator absorbs or removes returned light reflected from the dielectric multi-layer film. The temperature control circuit controls the temperature of the dielectric multi-layer film. The variable optical attenuator controls the transmitting characteristic of light of the dielectric multi-layer film by using the temperature control circuit. And the variable optical attenuator adjusts the power level of the optical signal of each wavelength transmitting between the WDM communication systems to a desiring level at the attenuating region in which the transmitting amount of the dielectric multi-layer film becomes small gradually.
Abstract:
An optical wavelength converting device is provided with a LiTaO3 substrate, a plurality of inverted-polarization layers periodically arranged in an upper surface of the LiTaO3 substrate, and an optical waveguide crossing the inverted-polarization layers. The upper surface of the LiTaO3 substrate is directed toward a -X-crystal axis direction. The inverted-polarization layers are formed by exchanging Ta ions of the LiTaO3 substrate for H ions, and an extending direction of each inverted-polarization layer is inclined at an angle of theta degrees (6 ions of the LiTaO3 substrate and the inverted-polarization layers for H ions to set a refractive index of the optical waveguide higher than that of the LiTaO3 substrate. The optical waveguide extends in a +Y-crystal axis direction. Fundamental waves polarized in a transverse electric mode induce electric field directed in +/-Y-crystal axis directions and are converted into second harmonic waves in the optical waveguide.
Abstract:
An optical wavelength converting device is provided with a LiTaO₃ substrate, a plurality of inverted-polarization layers periodically arranged in an upper surface of the LiTaO₃ substrate, and an optical waveguide crossing the inverted-polarization layers. The upper surface of the LiTaO₃ substrate is directed toward a -X-crystal axis direction. The inverted-polarization layers are formed by exchanging Ta⁺ ions of the LiTaO₃ substrate for H⁺ ions, and an extending direction of each inverted-polarization layer is inclined at an angle of ϑ degrees (6 ≦ ϑ ≦174) to the +C-crystal axis direction toward a -Y-crystal axis direction. The optical waveguide is formed by exchanging Ta⁺ ions of the LiTaO₃ substrate and the inverted-polarization layers for H⁺ ions to set a refractive index of the optical waveguide higher than that of the LiTaO₃ substrate. The optical waveguide extends in a +Y-crystal axis direction. Fundamental waves polarized in a transverse electric mode induce electric field directed in ±Y-crystal axis directions and are converted into second harmonic waves in the optical waveguide.