Abstract:
A method and system for reducing optical signal fading in an optical communication system include: dynamically obtaining turbulence-induced divergence and deviations of pointing direction for the atmosphere where an optical signal to be transmitted through; generating a single-transverse-mode laser beam of a predetermined diameter as the optical signal; dynamically varying the diameter of the laser beam to match the obtained turbulence-induced divergence of the atmosphere with a backtrack pointing direction; and transmitting the laser beam with varying diameter to a remote transceiver, as the optical signal.
Abstract:
A spatial filter adapted to increase the angular spread of non-conjugated energy in a beam and suppress this energy to improve the efficiency of a phase conjugate system. In the illustrative embodiment, the filter includes first and second lenses (81, 83) and an aberrator (86) to increase the angular spread. In the specific embodiment, an opaque plate (84), with a pinhole aperture (82) therethrough, is sandwiched between the lenses to suppress the non-conjugated energy. The aberrator may be implemented with an amplifier or other suitable mechanism. Likewise, the aperture may be replaced with a highly angle-selective thick Bragg grating or other suitable arrangement. A phase conjugate master oscillator/power amplifier laser architecture is also disclosed. In an illustrative embodiment, the novel architecture includes a master oscillator adapted to output a laser beam; a power amplifier beam line in optical alignment with the beam; a mechanism for creating a beam having phase conjugate energy and non-conjugated energy; and at least one inventive spatial filter in alignment with the amplifier. The inventive filter is adapted to increase the angular spread of non-conjugated energy in a beam and suppress this energy to improve the efficiency of the system. In a specific implementation, the beamline includes plural amplifiers, each with one of the novel spatial filters disposed therebetween.
Abstract:
A high gain optical amplifier and method. Generally, the inventive amplifier includes a first crystal (14) having an axis (14) and a first index of refraction and a second crystal (16) bonded to teh first crystal (12) about the axis (14) and having a second indey of refraction. The first index is higher that the second index such that light through the first crystal is totally internally reflected. In the illustrative embodiment, the first crystal (12) is Yb: YAG with an index of approximately 1.82m the second crystal (16) is Sapphire with an index of approximately 1.78, and the axis (14) is the propagation axis. The invention is, in its perferred embodiment, a light guide fabricated out of crystalline materials, diffusion bonded together. If the core of the light guide is doped with laser ions, high gain amplifiers made be designed and operable over a large etendue. With a judicious choice of the laser crystal and cladding materials, shape, and bonding technique, the guided amplifier is much less susceptible to parasitic oscillation than amplifiers constructed in accordance with conventional teachings. The clad core is also able to handle larger thermal load without breakage than can an unclad core.
Abstract:
A glaze encapsulated solid-state laser component (30). The novel laser component (30) includes a core (10) and a cladding (32) of ceramic glaze disposed on a surface of the core (10). In an illustrative embodiment, the core (10) is fabricated from a laser gain medium and the cladding material is a multi-oxide eutectic ceramic glaze having a refractivity slighter lower than the refractivity of the gain medium, such that the glaze layer forms a step-index refractivity interface cladding that can effectively suppress parasitic oscillations in the core gain medium. The glaze cladding (32) can be applied by coating the core (10) with the glaze and then firing the glaze coated core, or by fabricating pre-formed cladding strips from the ceramic glaze in a first firing cycle, mounting the pre-formed strips to the core (10), and then fusing the pre-formed strips to the core (10) in a secondary firing cycle.
Abstract:
An optical arrangement (10) comprising a first beam splitter (12) for transmitting light of a first polarization, to provide a first beam, and reflect light of a second polarization; a first spectral filter (16) in optical alignment with the first beam, the filter (16) being adapted to return a second beam thereto; and a first polarization rotator (14) in optical alignment with the beam splitter (12) and the spectral filter (16) for effecting a rotation of the polarization of the second beam relative to the first beam whereby the second beam has the second polarization and is reflected by the beam splitter (12). In a specific implementation, the spectral filter (12) may be a Bragg grating, a quarter-wave plate (22), a Faraday rotator (32) or other suitable device. If a Faraday rotator is used, a polarization adjuster (34) is used in optical alignment therewith. A number of alternative embodiments are disclosed. In a first alternative embodiment, a second polarization rotator (44) is disposed in optical alignment with the first beam splitter (12) for effecting a rotation of the polarization of the light reflected from the beam splitter (12) to provide a third beam. In one variant a second spectral filter (48) is disposed in alignment with the second polarization rotator (44). In another variant, the first spectral filter (52) is adapted to receive the third beam. In another embodiment, a second beam splitter (68) is disposed between the second Faraday rotator (64) and the spectral filter (16).
Abstract:
A solid-state laser beam amplifier with integrated reflective surface. A rectangular slab gain medium (50) receives a first portion of an input laser beam along a first zigzag reflection path within the slab. The gain medium (50) also receives a second portion of the input laser beam that has been reflected from an integral reflective surface (56) such that the two portions traverse the gain medium (50) along complementary zigzag paths. The zigzag paths are defined by total internal reflection of the beam portions as they propagate through the gain medium slab (50). A similar reflective surface (58) may be positioned relative to the exit end of the gain medium slab (50), which redirects all of the output beam portions in a parallel direction. The gain medium (50) may be Ytterbium or neodymium doped yttrium aluminum garnet. The gain medium (50) may be formed as a high aspect ration rectangular slab and may be clad with sapphire. The reflective surfaces may function by total internal reflection or may employ a reflective material, such as a dielectric coating. A section of undoped medium (52) may be applied to the entrance or exit end of the gain medium slab to control angles of incidence and refraction.
Abstract:
A planar laser gain medium (30) and laser system (100) The laser gain medium (30) includes an active core (32) having a high aspect ratio cross-section with a fast-axis dimension and a slow-axis dimension, signal claddings (36, 38) adapted to form reflective boundaries at fast axis boundaries of the core, and a material (50, 52) adapted to minimize reflections at slow axis boundaries of the core. In the illustrative embodiment, the laser gain medium (30) is an optical fiber. The core (32) and signal claddings (36, 38) form a waveguide adapted to control modes propagating in the fast-axis direction. When the laser gain medium (30) is employed as a laser oscillator, a high reflectivity mirror (102) and an outcoupler (104) are positioned at opposite ends of the core (32) to form a laser resonator adapted to control modes in the slow axis direction
Abstract:
A laser system and method. The inventive laser includes an annular gain medium; a source of pump energy; and an arrangement for concentrating energy from the source on the gain medium. In a more specific implementation, a mechanism is included for rotating the gain medium to effect extraction of pump energy and cooling. In the illustrative embodiment, the pump source is a diode array. Energy from the array is coupled to the medium via an array of optical fibers. The outputs of the fibers are input to a concentrator that directs the pump energy onto a pump region of the medium. In the best mode, plural disks of gain media are arranged in an offset manner to provide a single resonator architecture. First and second mirrors are added to complete the resonator, hi accordance with the inventive teachings, a method for pumping and cooling a laser is taught. In the illustrative embodiment, the inventive method includes the steps of providing a gain medium; pumping energy into a region of the gain medium; moving the medium; extracting energy from the region of the medium; and cooling region of the medium.
Abstract:
A system for removing waste energy in the form of sensible heat and fluorescent energy from a solid state laser medium (34) having a broad surface. The system includes a manifold (60) disposed about the laser medium (34) having a plurality of inlet jets (66) interspersed with a plurality of exhaust orifices (64). Coolant fluid is circulated through the manifold (60). The fluid is forced through the plurality of inlet jets (66) to impinge the broad face of the laser medium (34), thereby transferring waste energy by convection from the laser medium (34) to the coolant fluid. The coolant fluid is further circulated to exhaust the pumphead manifold (60) through the plurality of exhaust orifices (64). The fluorescent energy, which is radiated from the laser medium (34), is converted to sensible heat by an absorber (72) disposed within the coolant adjacent to the laser medium (34). The coolant then removes the converted heat by forced convection. The absorber (72) can be suspended particles in the coolant fluid or a porous material supported in the manifold (60) at some distance from the laser medium (34).