Abstract:
Two approaches are provided for achieving an optical amplifier system capable of producing high peak power, high energy pulse outputs while suppressing scattering noise. The first approach relates to an optical amplifier system which has at least one laser diode pulsed or cw pumped double clad fiber amplifier utilized for receiving a high frequency modulated injected signal pulse of short duration from the laser diode, via the fiber core, for amplification by coupling pump light into the inner cladding of the fiber. The average signal power is sufficient to saturate the gain of the fiber so as to minimize significant onset and buildup of forward and backward scattering noise. The duty cycle of the injected signal source pulse is chosen to allow adequate gain recovery in the fiber amplifier between pulses. The second approach relates to a cascaded optical amplifier system having at least two optical amplifying stages with two pulsed pump sources provided and two amplifying media, the first of which receives the injection and at least one pump signal wherein the injection pulsed signal is amplified to a first power and energy level. The second amplifying medium, optically coupled to the first, amplifies the first level signal to a second level amplified, injection pulsed signal. The duty cycle of the injection pulsed optical signal is synchronized with the first and second pulsed pump signals with the first pulsed pump signal having a different duration in the duty cycle than the second pulsed pump signal.
Abstract:
An optical coupling system for improving the coupling efficiency of an elliptical light beam into optical fibre (20) consists of a cylindrical concave microlens (10) on the end facet of the optical fibre (20) in conjunction with a pair of bulk optic asphere lenses (50 and 60). A method of producing a cylindrical concave microlens (10) according to the invention consists of translating a fine wire (100) across the end facet of an optical fibre (20) so as to create a cylindrical groove (10).
Abstract:
An infrared laser diode wireless local area network for communication between spatially dispersed terminals (22, 30, 40; 56, 58, 60, 62) such as computers which may be located in a single room (20) or in adjacent rooms (50, 52, 64). The lasers (90, 120, 140, 157) may be tuned to emit at varying frequencies for wavelength multiplexing, or a plurality of lasers (138) each having a different output frequency can be connected with each terminal. A receiver (26, 34, 44; 72, 80, 76, 84) connected to each terminal may similarly detect only a single narrow waveband or may detect a plurality of such wavebands. A transceiver (68, 70) may be employed for signal transmission between separate rooms. High speed data modulation of the carrier waves is provided with MOPA (90) or similar lasers, and broad angular dispersion of the output is achieved by such lasers along with dispersive lenses (132).
Abstract:
A display system in which lasers scanlessly illuminate the pixels of a spatially modulating display panel (11, 13, 15), such as a liquid crystal display or micromirror array. At least three sources at least one of which is a laser with each different wavelengths are used, such as laser diode-based sources (81, 83, 85) producing red, green and blue light. The laser may be pulsed rapidly in sequence to provide time multiplexed illumination of all of the display pixels or may be operated in continuous (cw) mode, using color filters on the display, phase plates (147) or microlens arrays to image light spots (148) of each color only on designated pixels. Two sets of laser sources (123), either orthogonally linearly polarized or at slight different wavelengths, can be used to create 3-D images. Each set may illuminate a different display panel, one for each eye, or the two sets may be time multiplexed using the same display panel (125). A viewer has polarizing or bandpass filters in front of each eye to separate the binocular images. Fiberoptic coupling (99) of the laser sources (81, 83, 85, 87) can be used to physically separate these sources and their power supply from the display panel (115).
Abstract:
An optical transmission link has both a transmitter module and a receiver module operable under uncooled conditions, i.e., without the need of costly cooling equipment, such as thermoelectric coolers. The optical transmission system includes both a semiconductor laser diode source and an optical receiver module that are both designed to operate uncooled under high frequencies (e.g., GHz range) over a wide temperature range without significant changes in signal bandwidth and at temperatures in excess of 125 DEG C. Compensation is provided to reduce the effect of photodiode noise and amplifier noise. In addition, temperature compensation can be provided that provides for overall reduction in receiver noise across the bandwidth of the receiver module through maintenance of a temperature environment optimizing receiver performance.
Abstract:
An optical fibre having a single mode absorptive core (10) whose position, relative to the cross-sectional plane of the inner multimode cladding (12), varies along the length of the fibre. The periodicity and the magnitude of the relative displacement of the core (10) with respect to the cladding (12) are such that the transfer of radiation from the inner multimode cladding (12) to the core (10) is substantially improved over conventional fibres.
Abstract:
A semiconductor light amplifying medium (11; 23) has reduced self-focusing and optical filamentation for providing higher power coherent outputs in broad-area laser and amplifier devices (Figs. 1 and 2). In one embodiment, a longitudinally inhomogeneous active region (13; 25) has alternating segments of first gain portions (15; 27) and second compensating portions (17; 29). The compensating portions have a negative self-focusing parameter [ DIFFERENTIAL n/ DIFFERENTIAL P] (Figs. 3 and 10) and may be light absorbing (negative gain) regions with negative antiguiding factor alpha (Figs. 4A-4C and 5) or light amplifying (positive gain) regions with positive antiguiding factor alpha (Figs. 6A-6B and 7A-7B). The alpha -parameter is defined as the ratio of refractive index change per change in gain, as a function of carrier density. In a second embodiment, the medium may have longitudinally varying peak filament period [Kpk] so that filaments beginning to form in one portion of the active region are subsequently dispersed in a succeeding portion, slowing filament growth. In addition to self-focusing compensation, media with a lower alpha -parameter are provided by increasing the barrier height in quantum well active regions (Figs. 8A-8B), straining (Fig. 9) or p-doping the active region, or a combination of these methods.
Abstract:
A laser system which features a distributed Bragg reflector (DBR) or a distributed feedback (DFB) tunable laser (11) coupled to a quasi-phasematched (QPM) waveguide (31; 16) of nonlinear material (13). The DBR laser is tuned either thermally (14; 51, 53) or via current injection (Itune), or both, converting the output of a red laser into blue. Thermal tuning provides coarse adjustment while injection current tuning provides fine adjustment. Intensity modulation or pulsed output may be provided by application of a modulation signal (Imod) to the DBR laser. Another embodiment provides frequency modulation (Vfsk) of the laser. In yet another embodiment, a high power laser (103) pumped fiber amplifier (101) is disposed between the laser (11) and the waveguide (16).