Scalable High Power Fiber Laser
US-2015349481-A1 · Dec 3, 2015 · US
US9627839B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9627839-B2 |
| Application number | US-201113981440-A |
| Country | US |
| Kind code | B2 |
| Filing date | May 13, 2011 |
| Priority date | Jan 24, 2011 |
| Publication date | Apr 18, 2017 |
| Grant date | Apr 18, 2017 |
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Official abstract text for this publication.
A fiber gain medium provided by a rare-earth doped fiber ( 10 ) is contained in a first resonant cavity by end reflectors ( 12, 18 ). The reflector ( 12 ) is wavelength selective to limit the frequency band of the first resonant cavity. The first resonant cavity also contains a second resonant enhancement cavity ( 16 ) with multiple transmission bands lying within the first resonant cavity's frequency band. Multiple standing wave modes of the first resonant cavity lie within both the frequency band of the first resonant cavity and the transmission bands of the second resonant cavity, and it is these standing wave modes that support laser action when the rare-earth doped fiber is suitably pumped by pump lasers ( 40 ).
Opening claim text (preview).
What is claimed is: 1. A device comprising: a portion of optical fiber providing an amplifying medium; a first resonant cavity containing the portion of optical fiber and having a frequency selective element which limits the frequency band of the first resonant cavity to cover a subset of axial modes of the first resonant cavity; a second resonant cavity arranged in the first resonant cavity and having a transmission response that includes a plurality of transmission bands within the frequency band of the first resonant cavity, so that there are a plurality of axial modes which lie within both the frequency band of the first resonant cavity and at least two of the transmission bands of the second resonant cavity, wherein the second resonant cavity is configured to increase intracavity power within the second resonant cavity to a power output that is higher relative to a power outputted from the optical fiber, and wherein the second resonant cavity includes a plurality of mirrors arranged within the second resonant cavity for circulating light received from the first resonant cavity within the second resonant cavity, at least one of the plurality of mirrors being curved; a pump source having an output directed to excite light within the first frequency band from the amplifying medium and induce lasing at multiple ones of said plurality of axial modes that lie within both the frequency band of the first resonant cavity and the transmission bands of the second resonant cavity, wherein the second resonant cavity has arranged therein a non-linear optical medium which supports a frequency mixing process in the second resonant cavity. 2. A device according to claim 1 , wherein the first resonant cavity is a linear cavity bounded by a first reflector and a second reflector. 3. A device according to claim 1 , wherein the first resonant cavity is a ring cavity. 4. A device according to claim 2 , wherein the frequency selective element comprises a grating. 5. A device according to claim 2 , wherein the frequency selective element comprises a filter. 6. A device according to claim 1 , wherein the optical fiber is single mode. 7. A device according to claim 1 , wherein the optical fiber is multi-mode comprising a fundamental mode and at least one higher order mode. 8. A device according to claim 7 , wherein the first resonant cavity is a linear cavity bounded by a first reflector and a second reflector, the first reflector being a fiber Bragg grating written into the optical fiber and having a mode-dependent effective period, and the second reflector being a volume Bragg grating having a period matched to the effective period of the fiber Bragg grating for the fundamental mode so that lasing is restricted to the fundamental mode. 9. A device according to claim 7 , wherein the multi-mode output of the optical fiber at the end optically adjacent to the second resonant cavity is spatially matched to the fundamental transverse mode TEM 00 of the second resonant cavity so that the first resonant cavity is resonant for multi-mode amplification in the optical fiber. 10. A device according to claim 1 , wherein each transmission band of the second resonant cavity has a width greater than the separation between the standing wave modes of the first resonant cavity. 11. A device according to claim 1 , wherein the optical fiber is doped with active laser ions, thereby to provide the amplifying medium. 12. A device according to claim 1 , wherein the optical fiber has a vibrational mode with a Stokes energy bridging the energy difference between the pump frequency band and the first frequency band, so that stimulated Raman scattering generates gain in the first frequency band, thereby to provide the amplifying medium. 13. A device according to claim 12 , comprising a further pump source which acts as a pump for said pump source.
using a diffraction grating · CPC title
using parametric generation · CPC title
with pump light recycling, i.e. with reinjection of the unused pump light, e.g. by reflectors or circulators · CPC title
Fibre ring lasers (fibre laser gyrometers G01C19/72) · CPC title
of a fibre laser · CPC title
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