摘要:
A zipper actuator for optical beam control has an optical port formed through the substrate. The cantilevered beam of the actuator preferably includes a paddle for switching the optical signal. Mirror structures can be provided on the paddle for beam switching. In some embodiments, MEMS or electrode latches are further provided.
摘要:
A multi-cavity micro-optical Fabry-Perot filter uses electrostatically deflected MEMS membranes. The filter comprises a first electrostatically deflectable membrane device. A curved mirror structure is formed on its optical membrane. Similarly, a second electro-statically deflectable membrane device is provided, which has a second curved mirror structure on the membrane. The spacer is used to separate the first membrane device from the second membrane device. The spacer supports a mirror between the first and second curved mirror structures. Wafer-level and device level assembly techniques are also described.
摘要:
A semiconductor tunable laser system includes a tunable Fabry-Perot cavity and a cavity length modulator, which controls an optical length of the cavity at least over a distance corresponding to the spacings between the longitudinal modes of the laser cavity. Thus, the tunable Fabry-Perot cavity allows the laser cavity to have gain at the desired wavelength of operation while the cavity length modulator tunes the cavity length such that a longitudinal cavity mode exists at the desired wavelength of operation. Also, in one embodiment, a wavelength locker system is further provides that has a differential wavelength filter, e.g., stepped etalon, and a multi-element detector, e.g., a quad-detector. The controller then modulators the Fabry-Perot cavity to control the wavelength in response to the signal received from the multi-element detector.
摘要:
A process for fabricating an optical membrane from polycrystalline silicon comprises first forming a sacrificial layer on a handle wafer. Concavities are etched into the sacrificial layer. Polycrystalline silicon membrane layer is then formed on the sacrificial layer. The polycrystalline membrane layer is subsequently polished to achieve the predetermined membrane thickness and surface smoothness, annealed, and then patterned. Finally, the sacrificial layer is removed to release the membrane. The concavities in the sacrificial layer yield convexities in the polysilicon layer to prevent stiction adhesion to the handle wafer. During processing, a mask used to pattern the membrane layer functions to protect an highly reflecting (HR) coating for the membrane.
摘要:
A distributed feedback (DFB) type laser and a method and apparatus for forming same wherein a quaternary semiconductor active lasing strip of material is buried between a substrate of binary compound of one type conductivity material and a mesa binary compound body of opposite type conductivity and a periodic grating structure is etched into the plateau of the mesa. In one embodiment, ohmic contacts are provided on either side of the grating structure and the mesa is undercut adjacent the active strip to partly isolate the ohmic contacts from the homojunction formed when the active strip is buried, preferably using a mass-transport process. In another embodiment, the ohmic contacts are formed on the top of a deeply etched grating structure. A buried layer double heterostructure (DH) laser is also described with DFB grating formed on the side wallsGOVERNMENT SUPPORTThe Government has rights in this invention pursuant to Contract No. F19628-85C-0002, awarded by the Department of the Air Force.
摘要:
A lens or fiberoptic cable focuses energy from a collimated helium neon laser beam upon a point on a mask. Some of the focused energy is reflected from the mask upon a photodetector array in an image plane, and some of this energy is reflected from a substrate closely adjacent to the mask after passing through the mask upon the photodetector array to produce an interference pattern that is sensed and characterized by a spatial frequency representative of the distance between the mask and substrate.
摘要:
A frequency swept laser source that generates an optical signal that is tuned over a spectral scan band at single discrete wavelengths associated with longitudinal modes of the swept laser source. Laser hopping over discrete single cavity modes allows long laser coherence length even under dynamic very high speed tuning conditions. A ramp drive to the laser is used to linearize laser frequency tuning. A beam splitter is used to divide the optical signal between a reference arm leading to a reference reflector and a sample arm leading to a sample. A detector system detects the optical signal from the reference arm and the sample arm for generating depth profiles and images of the sample.
摘要:
Optical coherence tomography (OCT) probe and system designs are disclosed that minimize the effects of mechanical movement and strain to the probe to the OCT analysis. It also concerns optical designs that are robust against noise from the OCT laser source. Also integrated OCT system-probes are included that yield compact and robust electro-opto-mechanical systems along with polarization sensitive OCT systems.
摘要:
An optical coherence analysis system comprising: a first swept source that generates a first optical signal that is tuned over a first spectral scan band, a second swept source that generates a second optical signal that is tuned over a second spectral scan band, a combiner for combining the first optical signal and the second optical signal for form a combined optical signal, an interferometer for dividing the combined optical signal between a reference arm leading to a reference reflector and a sample arm leading to a sample, and a detector system for detecting an interference signal generated from the combined optical signal from the reference arm and from the sample arm. In embodiments, the swept sources are tunable lasers that have shared laser cavities.
摘要:
A near infrared (NIR) semiconductor laser system is shown for gas sensing. An embodiment is centered on the use of a system with a much wider tunable laser, which today has a scan band of more than 150 nanometers (nm) to as much as 250 nm or more. In some cases the scan band is about 400 nm or more. This is achieved in the current embodiment through the use of a widely tunable microelectromechanical system (MEMS) based Fabry-Perot filter as an integral part of the laser cavity. Using this technology, these systems are capable of capturing a variety of gases in the any of the well-known spectroscopic scan bands, such as the OH, NH or CH. For example, a single laser with a 250 nm scan band window between 1550-1800 nm can capture ten or as many as twenty hydrocarbon-based gases simultaneously.