The operation of organic thin-film distributed feedback lasers at repetition rates up to 5MHz is studied. The active organic medium consists of a highly efficient, modified poly(9,9-dioctylfluorene) derivative containing 12% of statistical intrachain 6,6′ -(2,2′-octyloxy-1,1′-binaphthalene) binaphthyl spacer groups. The threshold energy density of these pulsed optically pumped lasers remains virtually unaltered at elevated repetition rates up to 5MHz. Therefore, we conclude that on this time scale photoinduced absorption which might affect the waveguide loss or the overall quantum efficiency is negligible in our active polymer. These results state an organic solid-state laser operating at repetition rates in the megahertz range which for many applications can be considered as quasi-cw.
High power, high brightness diode lasers are beginning to compete with solid state lasers, i.e. disk and fiber lasers. The core technologies for brightness scaling of diode lasers are optical stacking and dense spectral combining (DSC), as well as improvements of the diode material. Diode lasers have the lowest cost of ownership, highest efficiency and most compact design among all lasers.Multiple Single Emitter (MSE) modules allow highest power and highest brightness diode lasers based on standard broad area diodes. Multiple single emitters, each rated at 12 W, are stacked in the fast axis with a monolithic slow axis collimator (SAC) array. Volume Bragg Gratings (VBG) stabilizes the wavelength and narrow the linewidth to less than 1 nm. Dichroic mirrors are used for dense wavelength multiplexing of 4 channels within 12 nm. Subsequently polarization multiplexing generates 450 W with a beam quality of 4.5 mm*mrad.Fast control electronics and miniaturized switched power supplies enable pulse rise times of less than 10 µs, with pulse widths continuously adjustable from 20 µs to cw. Further power scaling up to multi-kilowatts can be achieved by multiplexing up to 16 channels. The power and brightness of these systems enables the use of direct diode lasers for cutting and welding. The technologies can be transferred to other wavelengths to include 793 nm and 1530 nm. Optimized spectral combining enables further improvements in spectral brightness and power.Keywords: High power diode laser, high brightness diode laser, fiber coupling, spectral combining, narrow bandwidth, wavelength stabilization, short pulses BACKGROUNDHigh power diode lasers find an increasing number of applications in materials processing and pumping of solid state lasers as their brightness increases. Beyond improvements in the design of the diodes themselves -for minimum slow axis divergence, highest power from a given size aperture and improved wall plug efficiency -optical and spectral stacking are deployed to scale power and brightness. Single emitters and minibars allow the highest brightness from the diode aperture. Single emitters typically deliver 12 W from a 100 µm aperture with 11 o slow axis divergence resulting in a similar brightness per emitter as minibars with up to 8 W from the aperture. Minibars require additional optics for beam shaping that can be omitted for single emitters. Single emitters also require low drive currents up to 15 A, which can be easily modulated with more than 100 kHz. Due to the low current cost effective power supplies are available. Furthermore, single emitter chip on submount (COS) is an established component that is available from various suppliers at a variety of different wavelengths and with exceptional ensemble reliabilities of tens of thousands of hours.Optical stacking is state of the art for power scaling, and many different configurations are available for bars and single emitters. Spectral stacking allows scaling of brightness and power. A narrow and stable spectrum of individual diodes is require...
Eye safe laser radiation at 1.6 µm is realized by a resonantly pumped Er:YAG laser operating in cw-and q-switched mode employing high brightness laser diode modules. These modules provide high power and narrow bandwidth emission at 1.5 µm from a 100 µm fibers providing high pump efficiency.
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