Abstract:
Methods and systems for generating and imaging THz electromagnetic radiation using a composite dipole array (150) made up of novel structures of non-linear dipole strings with dual frequency resonances for frequency up conversion and frequency down conversion are disclosed. THz electromagnetic radiation resulting from the frequency down conversion process can be used as an illumination source for imaging, as a carrier for communications, or as an energy source for spectroscopy, for example. Optical electromagnetic radiation resulting from the frequency up conversion process can be used to form images from THz electromagnetic radiation for contraband detection, guidance systems, and medical applications, for example.
Abstract:
There are provided an apparatus and method for friction welding structural members (60, 62). The apparatus -includes a connected shank (20) and probe (22). The probe (22) and the shank (20) defines an absorption surface (32) and a cavity (26) extending thereto. The absorption surface (32) is configured to receive electromagnetic radiation (52) from an electromagnetic radiation source (50) such as a light source or RF generator. The radiation (52) heats the probe (22), supplementing the heat generated by friction between the probe (22) and the structural members (60, 62), and thereby increasing the speed at which the probe (22) can be used to frictionally weld the structural materials (60, 62).
Abstract:
An active mirror amplifier (AMA) laser module incorporating an optically transparent, rigid substrate having a plurality of cooling passages has one surface thereof disposed against a laser gain medium disk. The substrate also has a plurality of microchannels disposed near or at an outer surface thereof which is in contact with an outer surface of the disk. A cooling medium is circulated through the flow passages and the cooling microchannels to help keep the disk cool during use of the laser. This allows the laser module to operate at significantly increased power without overheating. In one preferred embodiment the disk is attached to the substrate using a pressure differential between a front surface of the disk and the pressure of the coolant. This eliminates attachment-induced thermal stresses of prior art designs and allow the laser to operate at increased power without fracturing the substrate. Pre-forming the laser medium to achieve a generally flat condition when lasing in an unrestrained condition is also disclosed, which also reduces thermal attachment stresses and allows the laser to operate at a higher power without fracturing the substrate. A preferred implementation of the laser module in constructing a power amplifier is also disclosed, as is the use of multiple optical pump sources and optical fibers for delivering the optical energy to the laser module.
Abstract:
A laser system thermal management system includes a laser gain assembly and a thermal management assembly. The laser gain assembly includes a laser gain medium and may include laser pump diodes. The thermal management system includes a high pressure gas tank connected to an open-cycle Joule-Thompson refrigerator. Cooled and partially liquefied gas is introduced into a reservoir. The reservoir may be in good direct thermal contact with the laser gain assembly or via a closed loop recirculating fluid heat exchanger. The heat generated by the laser gain assembly is removed by heat exchange with the cooled gas and condensate in the reservoir either by direct thermal contact or via the recirculating heat exchanger loop. Gas evaporating in the reservoir is vented.
Abstract:
Apparatus and method for achieving improved performance n a solid-state laser. The solid-state laser apparatus (10) preferably uses a laser gain medium (12) in the shape of a disk wherein optical pump radiation (36) is injected into the peripheral edge of the disk. In the preferred embodiment the laser gain medium is provided with optical coatings for operation in the active mirror configuration. Furthermore, the laser gain medium is pressure-clamped to a rigid, cooled substrate (46), which allows it to maintain a prescribed shape even when experiencing significant thermal load. A cooling medium (52) can be provided to a heat exchanger internal to the substrate and/or flowed through the passages on the substrate surface, thereby directly cooling the laser gain medium. Sources (68) of optical pump radiation are played around the perimeter of the gain medium. Tapered ducts (20) may be disposed between the sources and the gain medium for the purpose of concentrating optical pump radiation. With the proper choice of laser gain medium doping, pump source divergence and geometry, a uniform laser gain is achieved across large portions of the gain medium.