Abstract:
A laser cooling apparatus and method. Generally, the inventive apparatus includes a mechanism for transporting sensible thermal energy from a solid state laser and for communicating waste fluorescent radiation therefrom as well. In the illustrative embodiment, the apparatus includes an optically transparent manifold (10) with an inlet port (12), an exhaust port (19) and a plurality of spray nozzles (16) therebetween adapted to direct a cooling fluid on the laser medium (20) of a laser (30). In addition, the optically transparent manifold (10) is used to permit waste fluorescent radiation to escape the confines of the laser and cooling system means such that said fluorescent radiation may be optically directed to an external heat sink such as free space.
Abstract:
A high extraction efficiency laser system (30). The novel laser system (30) includes a master oscillator (32) for providing a laser beam, an amplifier (18) adapted to amplify the laser beam, and an aberrator (42) for aberrating the laser beam to prevent the formation of caustic intensity patterns within the amplifier (18). In an illustrative embodiment, the laser system (30) also includes a depolarizer (44) disposed between the master oscillator (32) and the amplifier (18) to reduce the contrast of speckle intensity patterns in the amplifier (18), and a mechanism (46) adapted to rotate or otherwise move the aberrator (42) to time-vary the aberrations in the beam in order to increase the spatial homogenization of saturation and extraction patterns in the amplifier (18). In a preferred embodiment, the coherence length of the beam is also shortened to reduce interference fringes in the amplifier.
Abstract:
A self-adjusting interferometric outcoupler being an optical system (100) comprising a first system (112) for generating a first beam, a second system (122) for receiving the first beam and returning a second beam, and an interferometer (116) positioned to couple the first beam to the second system (122) and to receive and output the second beam, wherein the interferometer (116) is also shared by the first system (112) and/or the second system (122) to control the frequency of the first beam and/or the second beam, respectively. In the illustrative embodiment, the first system (112) is a master oscillator, the second system (122) is a phase conjugate mirror, and the optical system (100) further includes a power amplifier (118) positioned to amplify the first beam during a first pass and to amplify the second beam during a second pass.
Abstract:
A solid-state suspension laser (10). The novel laser (10) includes a gain medium (12) comprised of a plurality of solid-state gain particles (26) suspended in a fluid (28). The laser (10) also includes a pump source (20) for pumping the gain particles (26) and a resonator (14) for amplifying and outputting laser light generated by the gain medium (12). In an illustrative embodiment, the gain medium (12) is adapted to flow, and the pumping of the gain medium (12) occurs outside of the resonator (14). The flow velocities and the densities of the gain particles (26) in the gain medium (12) can be optimized for optimal absorption efficiency during the pumping and/or for optimal extraction efficiency in the resonator (14) as well as for overall laser performance optimization, including power, efficiency and beam quality scalability.
Abstract:
A laser cooling apparatus and method. Generally, the inventive apparatus includes a mechanism for transporting sensible thermal energy from a solid state laser and for communicating waste fluorescent radiation therefrom as well. In the illustrative embodiment, the apparatus includes an optically transparent manifold (10) with an inlet port (12), an exhaust port (19) and a plurality of spray nozzles (16) therebetween adapted to direct a cooling fluid on the laser medium (20) of a laser (30). In addition, the optically transparent manifold (10) is used to permit waste fluorescent radiation to escape the confines of the laser and cooling system means such that said fluorescent radiation may be optically directed to an external heat sink such as free space.
Abstract:
A self-adjusting interferometric outcoupler being an optical system (100) comprising a first system (112) for generating a first beam, a second system (122) for receiving the first beam and returning a second beam, and an interferometer (116) positioned to couple the first beam to the second system (122) and to receive and output the second beam, wherein the interferometer (116) is also shared by the first system (112) and/or the second system (122) to control the frequency of the first beam and/or the second beam, respectively. In the illustrative embodiment, the first system (112) is a master oscillator, the second system (122) is a phase conjugate mirror, and the optical system (100) further includes a power amplifier (118) positioned to amplify the first beam during a first pass and to amplify the second beam during a second pass.
Abstract:
A laser cooling apparatus and method. Generally, the inventive apparatus includes a mechanism for transporting sensible thermal energy from a solid state laser and for communicating waste fluorescent radiation therefrom as well. In the illustrative embodiment, the apparatus includes an optically transparent manifold (10) with an inlet port (12), an exhaust port (19) and a plurality of spray nozzles (16) therebetween adapted to direct a cooling fluid on the laser medium (20) of a laser (30). In addition, the optically transparent manifold (10) is used to permit waste fluorescent radiation to escape the confines of the laser and cooling system means such that said fluorescent radiation may be optically directed to an external heat sink such as free space.
Abstract:
A high extraction efficiency laser system. The novel laser system includes a laser amplifier and a laser source adapted to provide a laser beam to the amplifier such that polarization states for incident and reflected light within the amplifier are perpendicular one to another. In an illustrative embodiment, the laser beam is input to the amplifier such that the beam reflects back and forth between the side walls of the amplifier with an angle of incidence of about 45 degrees, and the laser beam is linearly polarized in the plane of incidence. This arrangement reduces interference fringes in the amplifier. In an alternative embodiment, the system includes an aberrator adapted to add time-varying aberrations in the laser beam at a rate exceeding an inversed lifetime of an inverted population in the amplifier to increase spatial homogenization of saturation and extraction patterns in the amplifier.
Abstract:
A high extraction efficiency laser system. The novel laser system includes a laser amplifier and a laser source adapted to provide a laser beam to the amplifier such that polarization states for incident and reflected light within the amplifier are perpendicular one to another. In an illustrative embodiment, the laser beam is input to the amplifier such that the beam reflects back and forth between the side walls of the amplifier with an angle of incidence of about 45 degrees, and the laser beam is linearly polarized in the plane of incidence. This arrangement reduces interference fringes in the amplifier. In an alternative embodiment, the system includes an aberrator adapted to add time-varying aberrations in the laser beam at a rate exceeding an inversed lifetime of an inverted population in the amplifier to increase spatial homogenization of saturation and extraction patterns in the amplifier.
Abstract:
A solid-state suspension laser (10). The novel laser (10) includes a gain medium (12) comprised of a plurality of solid-state gain particles (26) suspended in a fluid (28). The laser (10) also includes a pump source (20) for pumping the gain particles (26) and a resonator (14) for amplifying and outputting laser light generated by the gain medium (12). In an illustrative embodiment, the gain medium (12) is adapted to flow, and the pumping of the gain medium (12) occurs outside of the resonator (14). The flow velocities and the densities of the gain particles (26) in the gain medium (12) can be optimized for optimal absorption efficiency during the pumping and/or for optimal extraction efficiency in the resonator (14) as well as for overall laser performance optimization, including power, efficiency and beam quality scalability.