High-power CW fiber-laser
View Patent ↗A CW ytterbium-doped fiber-laser includes a gain-fiber having a reflector proximity-coupled to one end, with the other end left uncoated. A laser resonator is defined by the reflector and the uncoated end of the gain-fiber. Pump-radiation from fast-axis diode-laser bar-stacks emitting at 915 nm and 976 nm is combined and focused into the uncoated end of the gain-fiber for energizing the fiber. Laser radiation resulting from the energizing is delivered from the uncoated end of the gain-fiber and separated from the pump-radiation by a dichroic mirror.
1. Optical apparatus, comprising:
a gain-fiber having first and second opposite ends and having a fundamental emission wavelength for laser radiation;
a source of optical pump-radiation including a plurality of diode-laser bars, each thereof having a plurality of diode-laser emitters therein, with each emitter delivering radiation into a corresponding one of a plurality of optical fibers having a rectangular core, with sides of the rectangular core aligned with the fast- and slow-axes of the emitter at a proximal end of the fiber, and wherein distal ends of the fibers are formed into a two-dimensional array of columns and rows and with sides of the rectangular cores in each column and each row parallel to each other to create a two dimensional array of radiation beams;
collimating optics arranged to collimate the individual radiation beams emitted from the distal ends of each of the rectangular-core fibers while maintaining the propagation of the beams in the two dimensional array; and
a focusing lens arranged to focus the collimated radiation beams from rectangular-core fibers into the first end of the gain-fiber.
2. The apparatus of claim 1 , wherein the collimating optics includes a first plurality of cylindrical lenses arranged to collimate radiation from the rectangular-core fibers in the fast-axis direction and a second plurality of cylindrical lenses arranged to collimate the radiation from the rectangular-core fibers in the slow-axis direction.
3. The apparatus of claim 1 , wherein the collimating optics includes a plurality of lenses corresponding in number to the plurality of rectangular-core fibers and arranged to collimate distal ends of the rectangular-core fibers in both the fast-axis and the slow-axis.
4. Optical apparatus, comprising:
a gain-fiber having first and second opposite ends and having a fundamental emission wavelength for laser radiation;
first source and second sources of optical pump-radiation each of the sources of optical pump radiation including a plurality of diode-laser bars, each thereof having a plurality of diode-laser emitters therein, with each emitter delivering radiation into a corresponding one of a plurality of optical fibers having a rectangular core, with sides of the rectangular core aligned with the fast- and slow-axes of the emitter at a proximal end of the fiber, and wherein distal ends of the fibers are formed in to a two-dimensional array of columns and rows with sides of the rectangular cores in each column and row parallel to each other to create a two dimensional array of radiation beams;
collimating optics arranged to collimate the individual radiation beams emitted from the distal ends of each of the rectangular-core fibers while maintaining the propagation of the beams in the two dimensional array;
a beam-combiner arranged to combine the collimated radiation beams from rectangular-core fibers of the first and second pump-radiation sources; and
focusing lens arranged to focus the combined collimated radiation beams from the rectangular-core fibers into the first end of the gain-fiber.
5. The apparatus of claim 4 , wherein the pump-radiation from the first source has a wavelength different from that of the pump radiation from the second source and the beam combiner is a dichroic beam combiner.
6. The apparatus of claim 4 , wherein pump-radiation from the distal ends of the rectangular-core fibers of both pump-radiation sources is plane-polarized, with the polarization-orientation from the rectangular-core fibers of the first source of pump-radiation being perpendicular to the polarization-orientation from the rectangular-core fibers of the second source of pump radiation, and wherein the beam-combiner is a polarization-selective beam-combiner.
7. The apparatus of claim 6 , wherein pump-radiation from both sources has the same wavelength.
8. The apparatus of claim 4 , wherein the collimating optics includes a first plurality of cylindrical lenses arranged to collimate radiation from the rectangular-core fibers in the fast-axis direction and a second plurality of cylindrical lenses arranged to collimate the radiation from the rectangular-core fibers in the slow-axis direction.
9. The apparatus of claim 4 , wherein the collimating optics includes a plurality of lenses corresponding in number to the plurality of rectangular-core fibers and arranged to collimate distal ends of the rectangular-core fibers in both the fast-axis and the slow-axis.