Abstract:
A vertical cavity surface emitting laser (VCSEL) has a shortened overall laser cavity by combining the gain section with a distributed Bragg reflector (DBR). The overall cavity length can be contracted by placing gain structures inside the DBR. This generally applies to a number of semiconductor material systems and wavelength bands, but this scheme is very well suited to the AlGaAs/GaAs material system with strained InGaAs quantum wells as a gain medium, for example.
Abstract:
An optoelectronic device includes a carrier substrate and a lower distributed Bragg-reflector (DBR) stack disposed on an area of the substrate and including alternating first layers. A set of epitaxial layers disposed over the lower DBR includes a quantum well structure. An upper DBR stack disposed over the set of epitaxial layers includes alternating second layers. Electrodes apply an excitation current to the quantum well structure. At least one of the electrodes includes a metal ring disposed at an inner side of at least one of the DBR stacks in proximity to the quantum well structure. One or more metal vias pass through the at least one of the DBR stacks so as to connect the metal ring at the inner side of the at least one of the DBR stacks to an electrical contact on an outer side of the at least one of the DBR stacks.
Abstract:
A laser device, a light source module and a laser radar. The laser device comprises: a light-emitting lamination, comprising a first reflector (105), an active region (104) and a second reflector (102), which are sequentially arranged in a light emergence direction, wherein the light-emitting lamination comprises one or more light-emitting units (200), and each of the light-emitting units (200) comprises a plurality of regularly arranged light-emitting points (203); and electrode units (107) located on the side of the first reflector (105) that is away from the active region (104), wherein each of the electrode units (107) corresponds to one light-emitting unit (200) and is used for loading a driving signal to the light-emitting unit (200). The laser device can improve the uniformity of luminous intensity.
Abstract:
Described here is a platform for supporting a fiber optic cable. The platform may be made on a silicon wafer using silicon lithographic processing techniques. The platform may include a substrate having a top planar surface; a trench formed in the substrate in the top planar surface and dimensioned to accept a fiber optic cable carrying radiation; and a reflecting surface formed in the top planar surface, wherein this reflecting surface is configured to reflect the radiation by total internal reflection, wherein the reflecting surface is configured to direct radiation travelling in a first direction into a second direction, substantially orthogonal to the first direction.
Abstract:
A surface emission laser includes a first beam, a second reflector disposed in an opening portion formed in the first beam, and a second beam disposed in the opening portion, and extending in a widthwise direction of the first beam to connect the second reflector and the first beam, wherein a length, in a longitudinal direction of the first beam, of the second beam is smaller than a length, in the longitudinal direction of the first beam, of the second reflector.
Abstract:
A wavelength tunable gain medium with the use of micro-electromechanical system (MEMS) based Fabry-Perot (FP) filter cavity tuning is provided as a tunable laser. The system comprises a laser cavity and a filter cavity for wavelength selection. The laser cavity consists of a gain medium such as a Semiconductor Optical Amplifier (SOA), two collimating lenses and an end reflector. The MEMS-FP filter cavity comprises a fixed reflector and a moveable reflector, controllable by electrostatic force. By moving the MEMS reflector, the wavelength can be tuned by changing the FP filter cavity length. The MEMS FP filter cavity displacement can be tuned discretely with a step voltage, or continuously by using a continuous driving voltage. The driving frequency for continuous tuning can be a resonance frequency or any other frequency of the MEMS structure, and the tuning range can cover different tuning ranges such as 30 nm, 40 nm, and more than 100 nm.
Abstract:
Optical systems employ a tunable source which includes a short cavity laser with a large free spectral range cavity, fast tuning response, and single transverse and longitudinal mode operation. Systems for optical spectroscopy with optimized scanning, a system for optical beam steering and a system for a tunable local oscillator are disclosed.
Abstract:
In order to provide a wavelength tunable surface emitting laser capable of improving a wavelength tuning efficiency, provided is a surface emitting laser, including: a first reflector; a semiconductor cavity including an active layer; and a second reflector, the first reflector, the semiconductor cavity, and the second reflector being formed in the stated order, a gap portion being formed between the first reflector and a semiconductor layer, a cavity length being tunable, in which the surface emitting laser has a high reflectivity structure formed between the gap portion and the semiconductor cavity, and an expression of “(λ/2)×m+λ/8
Abstract:
Configurations for in-situ gas detection are provided, and include miniaturized photonic devices, low-optical-loss, guided-wave structures and state-selective adsorption coatings. High quality factor semiconductor resonators have been demonstrated in different configurations, such as micro-disks, micro-rings, micro-toroids, and photonic crystals with the properties of very narrow NIR transmission bands and sensitivity up to 10−9 (change in complex refractive index). The devices are therefore highly sensitive to changes in optical properties to the device parameters and can be tunable to the absorption of the chemical species of interest. Appropriate coatings applied to the device enhance state-specific molecular detection.
Abstract:
A surface emitting laser operable to change a wavelength of emitted light includes a first reflecting mirror, a second reflecting mirror, wherein a cavity is formed between the first reflecting mirror and the second reflecting mirror along the optical axis of the surface emitting laser, an active layer formed within the cavity, a region formed within the cavity, and a movable part situated within the region, the movable part having a refractive index different from a refractive index of the region. The wavelength of emitted light is changeable by changing the position of the movable part along the direction of the optical axis in the region.