Patent application number | Description | Published |
20080273567 | HYBRID WAVEGUIDE SYSTEMS AND RELATED METHODS - A III-V semiconductor waveguide is coupled with a Si waveguide to form a hybrid structure. Spatial location of the optical mode (or supermode) of the hybrid structure is controlled by controlling at least one between the geometry and the refractive index of the structure, e.g., varying width of the Si waveguide. Control of such spatial location allows location of the optical mode either almost entirely in the III-V semiconductor waveguide or almost entirely in the Si waveguide, thus allowing various optical arrangements to be obtained according to the location of the optical mode and the proprieties of the waveguides. For example, if the III-V semiconductor waveguide is amplifying and is provided with a highly reflective mirror at one end, the Si waveguide is provided with a partially reflective mirror at the other end, the optical mode is almost entirely located in the gain region of the III-V semiconductor waveguide, and is also almost entirely located in the coupling region of the Si waveguide, a resonator for laser oscillation is obtained. | 11-06-2008 |
20100085992 | Arbitrary Optical Waveform Generation Utilizing Optical Phase-Locked Loops - This invention relates to opto-electronic systems using semiconductor lasers driven by optical phase-locked loops that control the laser's optical phase and frequency. Feedback control provides a means for precise, wideband control of optical frequency and phase, augmented further by four wave mixing stages and digitally stitched independent optical waveforms for enhanced tunability. | 04-08-2010 |
20120156802 | SWEPT-FREQUENCY SEMICONDUCTOR LASER COUPLED TO MICROFABRICATED BIOMOLECULAR SENSOR AND METHODS RELATED THERETO - An optoelectronic swept-frequency semiconductor laser coupled to a microfabricated optical biomolecular sensor with integrated resonator and waveguide and methods related thereto are described. Biomolecular sensors with optical resonator microfabricated with integrated waveguide operation can be in a microfluidic flow cell. | 06-21-2012 |
20120262721 | Arbitrary Optical Waveform Generation Utilizing Optical Phase-Locked Loops - This invention relates to opto-electronic systems using semiconductor lasers driven by optical phase-locked loops that control the laser's optical phase and frequency. Feedback control provides a means for precise, wideband control of optical frequency and phase, augmented further by four wave mixing stages and digitally stitched independent optical waveforms for enhanced tunability. | 10-18-2012 |
20140029893 | METHODS AND SYSTEMS FOR DELAYING OPTICAL WAVES - Coupled-resonator optical waveguides (CROW) can be used to control a speed of an optical signal. In particular, the coupling distance between the resonators can be adjusted to precisely control a group delay of an optical wave. Systems and methods are described to control such coupling distance in a CROW. | 01-30-2014 |
20140104593 | THREE-DIMENSIONAL TOMOGRAPHIC IMAGING CAMERA BASED ON COMPRESSIVE SENSING - A detection apparatus and method for FMCW LIDAR employ signals that are modified so that low-cost and low-speed photodetector arrays, such as CCD or CMOS cameras, can be employed for range detection. The LIDAR is designed to measure the range to one or more targets and includes a single mode swept frequency laser (SFL), whose optical frequency is varied with time, as a result of which, a target beam which is reflected back by the one or more targets is shifted in frequency from a reference beam by an amount that is proportional to the relative range to the one or more targets. The reflected target beam(s) is/are combined with the reference beam and detected by the photodetector array. In the case of a sparse number of targets to be detected, Compressive Sensing (CS) techniques can be employed by a processor to reduce the number of measurements necessary to determine the range of each target. | 04-17-2014 |
20150177380 | THREE-DIMENSIONAL TOMOGRAPHIC IMAGING CAMERA - A detection apparatus and method for FMCW LIDAR employ signals whose frequencies are modified so that low-cost and low-speed photodetector arrays, such as CCD or CMOS cameras, can be employed for range detection. The LIDAR is designed to measure the range z to a target and includes a single mode swept frequency laser (SFL), whose optical frequency is varied with time, as a result of which, a target beam which is reflected back by the target is shifted in frequency from a reference beam by an amount that is proportional to the relative range z to the target. The reflected target beam is combined with the reference beam and detected by the photodetector array. By first modulating at least one of the target and reference beams such that the difference between the frequencies of the reflected target beam and the reference beam is reduced to a level that is within the bandwidth of the photodetector array, the need for high-speed detector arrays for full-field imaging is obviated. | 06-25-2015 |
20150333480 | HIGH-COHERENCE SEMICONDUCTOR LIGHT SOURCES - A laser resonator includes an active material, which amplifies light associated with an optical gain of the resonator, and passive materials disposed in proximity with the active material. The resonator oscillates over one or more optical modes, each of which corresponds to a particular spatial energy distribution and resonant frequency. Based on a characteristic of the passive materials, for the particular spatial energy distribution corresponding to at least one of the optical modes, a preponderant portion of optical energy is distributed apart from the active material. The passive materials may include a low loss material, which stores the preponderant optical energy portion distributed apart from the active material, and a buffer material disposed between the low loss material and the active material, which controls a ratio of the optical energy stored in the low loss material to a portion of the optical energy in the active material. | 11-19-2015 |