Abstract:
A method and apparatus for providing a laser beam that is automatically aligned with a substantially rigid, stabilized platform or frame that can be oriented over a wide angular range, such as by the gimbals of a laser pointing and tracking system. A single-transverse-mode master laser oscillator (12) is mounted on the stabilized platform (13) which is part of the inner gimbal, which can be rotated about an elevation axis (16), and a multipass laser amplifier (21) with a phase conjugation mirror (22) and an optional nonlinear frequency-conversion device (20) are located off the inner gimbal. An outer gimbal or pedestal mount permits rotation about an azimuthal axis (17). The laser oscillator (12) and laser amplifier (21) are coupled by means of a beamsplitter (15) and two reflecting elements (18 and 19). The laser media used for the oscillator (12) and amplifier (21) are either the same, or compatible media having the same wavelength. In an alternative embodiment the two reflecting elements are replaced by a flexible light waveguide such as a glass fiber. The phase conjugation mirror (22) compensates the beam for the effects of optical aberrations caused by thermally induced changes in the amplifier medium and the nonlinear medium (if used) and also compensates the beam for angular tilt and jitter in the beam line of sight due to structural flexibility and motion of the stabilized platform. Four different embodiments are described in which the phase conjugation mirror is based on stimulated Brillouin scattering, degenerate four-wave mixing, three-wave mixing, and photon echo effects, respectively.
Abstract:
A laser apparatus (10) has a coherent master oscillator radiation source (30) for driving a plurality of laser gain elements (20) positioned in a operationally parallel configuration so as receive unamplified radiation (40) from master oscilltor (30) and transmitting amplified radiation (44). Input means (60) couples portion of radiation (40) from master oscillator to each of said gain elements (20). Phase conjugate reflector means (80) operatively coupled to gain elements (20) reflects the phase conjugate of amplified radiation (44) back into the gain elements (20) where it is further amplified. Output coupling means (90) couples amplified radiation from the plurality of gain elements (20) out of the laser apparatus as a single coherent output beam of radiation.
Abstract:
A coherent input beam from a laser (82) is fed into a Brillouin-enhanced four wave mixer (88) which generates a phase conjugated seed beam in counterpropagation with the input beam. A Brillouin amplifier (86) is provided between the laser and four wave mixer to transfer energy from the input beam (Ep) to the seed beam (Ec) and thereby amplify the seed beam to produce a phase conjugated output beam with approximately 50 % of the energy of the input beam and narrow bandwidth which is free from random phase jumps associated with the acoustic noise generally required to initiate and sustain stimulated Brillouin scattering. The phase conjugated output beam can be modulated or steered in direction, as desired. Reference beams for the four wave mixer may be derived from the same laser source as the input beam and have energies one or more orders of magnitude smaller than the energy of the input beam.
Abstract:
The output of an optical device which involves a stimulated Brillouin scattering (SBS) gain medium is enhanced over a range of input beam intensities by providing a gain medium which has a given SBS gain for a given input beam intensity, and modifying the gain medium to reduce its SBS gain coefficient. By lowering the SBS gain coefficient, SBS dominance and suppression of stimulated Raman scattering (SRS) can be mitigated, and the output fidelity of a phase conjugation system with respect to its input can be significantly enhanced. Mechanisms for reducing the SBS gain coefficient include increasing the medium viscosity, thermal conductivity and/or diffusion coefficient, or causing the medium relaxation zone to coincide with the frequency of the phonons involved in the SBS process. Two different media can be mixed together in varying proportions to progressively modify the overall medium SBS gain as the input beam intensity is progressively changed.
Abstract:
The output of an optical device which involves a stimulated Brillouin scattering (SBS) gain medium is enhanced over a range of input beam intensities by providing a gain medium which has a given SBS gain for a given input beam in tensity, and modifying the gain medium to reduce its SBS gain coefficient. By lowering the SBS gain coefficient, SBS dom inance and suppression of simulated Raman scattering (SRS) can be mitigated, and the output fidelity of a phase conjuga tion system with respect to its input can be significantly enhanced. Mechanisms for reducing the SBS gain coefficient including increasing the medium viscosity, thermal conductivity and/or diffusion coefficient, or causing the medium relaxa tion zone to coincide with the frequency of the phonons involved in the SBS process. Two different media can be mixed together in varying proportions to progressively modify the overall medium SBS gain as the input beam intensity is pro gressivelsy changed.
Abstract:
Un faisceau cohérent d'entrée émis par un laser (82) est introduit dans un mélangeur (8) à quatre ondes amélioré par une zone Brillouin qui génère un faisceau-semence à phases conjuguées qui se propage en sens contraire au faisceau d'entrée. Un amplificateur de Brillouin (86) agencé entre le laser et le mélangeur à quatre ondes transfère l'énergie du faisceau d'entrée (Ep) au faisceau semence (Ec), amplifiant le faisceau-semence de façon à produire un faisceau de sortie à phases conjuguées ayant approximativement 50 % de l'énergie du faisceau d'entrée et une bande passante étroite dépourvue des sauts aléatoires de phase associés au bruit acoustique généralement requis pour initier et maintenir une dispersion stimulée de Brillouin. Le faisceau de sortie à phases conjuguées peut être modulé ou dirigé selon les besoins. On peut dériver des faisceaux de référence pour le mélangeur à quatre ondes à partir de la même source laser que le faisceau d'entrée, avec des énergies inférieures d'un ou plusieurs ordres de magnitude à l'énergie du faisceau d'entrée.
Abstract:
A coherent input beam from a laser (82) is fed into a Brillouin-enhanced four wave mixer (88) which generates a phase conjugated seed beam in counterpropagation with the input beam. A Brillouin amplifier (86) is provided between the laser and four wave mixer to transfer energy from the input beam (Ep) to the seed beam (Ec) and thereby amplify the seed beam to produce a phase conjugated output beam with approximately 50 % of the energy of the input beam and narrow bandwidth which is free from random phase jumps associated with the acoustic noise generally required to initiate and sustain stimulated Brillouin scattering. The phase conjugated output beam can be modulated or steered in direction, as desired. Reference beams for the four wave mixer may be derived from the same laser source as the input beam and have energies one or more orders of magnitude smaller than the energy of the input beam.
Abstract:
The output of an optical device which involves a stimulated Brillouin scattering (SBS) gain medium is enhanced over a range of input beam intensities by providing a gain medium which has a given SBS gain for a given input beam intensity, and modifying the gain medium to reduce its SBS gain coefficient. By lowering the SBS gain coefficient, SBS dominance and suppression of stimulated Raman scattering (SRS) can be mitigated, and the output fidelity of a phase conjugation system with respect to its input can be significantly enhanced. Mechanisms for reducing the SBS gain coefficient include increasing the medium viscosity, thermal conductivity and/or diffusion coefficient, or causing the medium relaxation zone to coincide with the frequency of the phonons involved in the SBS process. Two different media can be mixed together in varying proportions to progressively modify the overall medium SBS gain as the input beam intensity is progressively changed.
Abstract:
Un appareil laser (10) comprend une source de rayonnement à oscillateur principal (30) pour commander une pluralité d'éléments de gain laser (20) placés en parallèle de façon à recevoir un rayonnement non-amplifié (40) de l'oscillateur principal (30) et à transmettre un rayonnement amplifié (44). Un organe d'entrée (60) couple une partie du rayonnement (40) émis par l'oscillateur principal à chacun des éléments de gain (20). Un dispositif réflecteur (80) des phases conjuguées, couplé fonctionnellement aux éléments de gain (20), renvoie les phases conjuguées du rayonnement amplifié (44) aux éléments de gain (20), où elles sont amplifiées à nouveau. Un organe de couplage (90) de sortie couple le rayonnement amplifié d'une pluralité d'éléments de gain (20) à la sortie de l'appareil laser sous la forme d'un seul faisceau cohérent de rayonnements de sortie.
Abstract:
A laser apparatus (10) has a coherent master oscillator radiation source (30) for driving a plurality of laser gain elements (20) positioned in a operationally parallel configuration so as receive unamplified radiation (40) from master oscilltor (30) and transmitting amplified radiation (44). Input means (60) couples portion of radiation (40) from master oscillator to each of said gain elements (20). Phase conjugate reflector means (80) operatively coupled to gain elements (20) reflects the phase conjugate of amplified radiation (44) back into the gain elements (20) where it is further amplified. Output coupling means (90) couples amplified radiation from the plurality of gain elements (20) out of the laser apparatus as a single coherent output beam of radiation.