WO2014134173A1 - Ultra-high power fiber laser system with multimode-multimode fiber combiner - Google Patents
Ultra-high power fiber laser system with multimode-multimode fiber combiner Download PDFInfo
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- WO2014134173A1 WO2014134173A1 PCT/US2014/018688 US2014018688W WO2014134173A1 WO 2014134173 A1 WO2014134173 A1 WO 2014134173A1 US 2014018688 W US2014018688 W US 2014018688W WO 2014134173 A1 WO2014134173 A1 WO 2014134173A1
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- Prior art keywords
- combiner
- fiber
- cladding
- light
- zone
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Classifications
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/2804—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers
- G02B6/2856—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers formed or shaped by thermal heating means, e.g. splitting, branching and/or combining elements
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/42—Coupling light guides with opto-electronic elements
- G02B6/4296—Coupling light guides with opto-electronic elements coupling with sources of high radiant energy, e.g. high power lasers, high temperature light sources
Definitions
- the disclosure relates to ultra-high power fiber laser systems.
- the disclosure relates to an ultra-high power multimode (“MM") fiber system emitting tens of kWs, MM laser output and configured with a mechanism which is operative to efficiently filter out unwanted forward-propagating and backrefiected cladding light.
- MM ultra-high power multimode
- Mttiti kW fiber laser systems are used in a growing number of applications. As fiber lasers mature towards commercial deployment, an intense focus on thei power, quality, reliability and that of their components is required. To enable the desired power levels, multiple low-mode (“LM' * ) fiber laser systems are optically and mechanically coupled together in a LM ⁇ MM combiner. To efficiently perform at high kW power levels, the combiner should successfully deal with a few structural difficulties some of which, such as mechanical coupling of fibers and power l oses in forward and backreflection directions, are of particular interest hers.
- LM' * low-mode
- a process of fabricati g high power combiner includes fusing aligned output fibers of respective fiber lasers/amplifiers in a bundle, tapering the latter, cleaving and splicing the tapered bundle to a system output delivery fiber,.
- the fabrication of the combiner which initiall assumes a bow-tie configuration, whose waist is further severed in half, may result in structural defects (burrs) of the outer cladding which further, during the combiner's deployment, may detrimentally affect the quali y of the output laser beam and power thereof.
- both forward and backrefiecied propagating core-guided light tends io bleed into the adjacent cladding at air-quartz interfaces and splices between various fibers as it propagates through the system.
- high power signal light induces thermal loads on a polymeric coating surrounding the cladding.
- the coating is configured to minimize the structural damages that a fiber may experience as a result of external mechanical loads applied to the fiber.
- Both forward -propagating signal light and, particularly, backreileeied light - light reflected from the surface to be laser treated - may bled into a cladding which is damaging both to a combiner itself and to system components upstream therefrom which are particularly vulnerable when they are exposed to the backreilecied light. Accordingly, both forward and backward propagating cladding light have be removed from a waveguide.
- the combiner needs a special configuration which would allow the following:
- the fibers guiding outputs of respective individual low mode fiber laser systems each have a multi-layer configuration so as to improve reliable coupling among output fibers and minimize the possibility of damaging their respective cores while fabricating a LM-MM combiner.
- the multi-layer configuration of each double-clad fiber, referred further as input fibers includes inner and outer layers.
- the inner layer includes silicone dioxide (SiO 2 ), whereas the outer layer is made from SiO 2 doped with ions of fluorine ("F”) and having a relatively low melting temperature.
- F fluorine
- the LM/MM combiner is configured with an absorber capable of efficiently removing unwanted forward-propagating and hackrefiected light guided along cladding regions of the disclosed system.
- the absorber is configured with upstream, intermediary and downstream consecutive zones .responsible for removing unwanted light which has two sources of origin.
- One source includes losses of forward propagating signal light as it is guided through splice regions between fibers.
- the other source relates to backreflected light which is coupled into the core and cladding of the feeding fiber upon bouncing back from the workpiece in a counter-propagating direction,
- the upstream zone is configured to predominantly prevent back reflected light from reaching individual LM fiber iaser systems.
- the zone is defined by a polymer having a refraction index higher than that of quartz,
- the intermediary zone is configured to prevent high aperture rays of signal light lost at upstream splices and guided along a cladding in a forward propagating direction from escaping the combiner.
- the polymer constituting this zone is configured with a refraction index substantially the same as or lower than quartz.
- the downstream zone is configured similar to the upstream zone, but operative to remove forward propagating signal light which was not processed in the intermediary zone,
- a further aspect deals with a MM high power fiber laser system including the disclosed combiner.
- the system is configured with a cladding mode absorber which is operative to minimize and provide removal of backreflected light which is coupled into the cladding of the system's output fiber.
- FIG. 1 is an elevated view of the di sclosed high power fiber laser system:
- FIG. 2 is a diagrammatic view of a LM/MM-MM combiner component of the system of
- FIG, 1
- FlGs. 2a -2d are respective cross-sectional views along respective lines in FIG. 2;
- FIG. 3 is a diagrammatic view of a cladding mode absorber of system of FIG. .1.
- FIG. 1 illustrates a diagrammatic view of high power fiber laser system 10 capable of emitting a high quality beam of up to about 50 kWs.
- the system 10 is configured with a plurality of low mode (“SM- LM/MM”) fiber combiners 12 each of which is operative io emit, radiation in low mode or multiple transverse mode system output.
- SM ⁇ LM/MM combiner The configuration of SM ⁇ LM/MM combiner is disclosed in concurrently filed US Provisional Application Serial incorporated, herein by reference in its entirety.
- the SM -LM/MM laser combiners 12 are provided with respective LM/MM output passive fibers 16 each of which is spliced directly or via an intermediary passive fiber with an input MM passive fiber 19.
- the fusion region forms thereby an upstream splice surrounded by a splice filter 20.
- the LM input fibers 19 are then aligned and further mechanically and optically coupled to one another in a LM/MM-MM combiner 22.
- the system 10 is completed with a. downstream system clad mode absorber 80.
- LM-MM combiner 22 is formed by Initially aligning multiple LM/MM passive, input fibers 19, each of which is configured with a large diameter M.M core 32 (FIG, 2a) and outer cladding 34, with one another to define a large diameter input end of the bundle as shown in FIG. 2a. Thereafter, aligned LM/MM input fibers 19 are simultaneously fused and stretched Into a. small diameter downstream end 24 of the tapered bundle, The downstream end 24 of the bundle includes a single core formed upon fusing and stretching individual input fiber 19. The stretching is performed so that the diameters of downstream end 24 of the fused bundle and MM combiner output passive fiber 26, respectively, substantially, but not ideally, match one another. As a result, fusing these elements forms a splice region 30 configured so that light experiences low splice losses as it propagates through this splice region 30.
- a combined beam output may reach of up to about 50 kW and have a BPP, for example, below 20 and as low as 10.
- the downstream end 24 of the tapered bundle and an upstream portion of combiner's output fiber 26 are placed in a housing 23 which, in turn, is coupled to a heat sink not shown, here.
- the input fibers 19 entering housing 23 are fixed to one another by any suitable adhesive. Due to high powers and therefore elevated temperatures, the adhesive includes a temperature resistant component which may be, for example, UV-15-TK.
- combiner 22 critically depends on how effectively unwanted cladding- guided light, which propagates along the combiner in opposite directions, is utilized.
- mechanisms dealing with, light removal from the waveguide's cladding are called light strippers or clad mode absorbers ("CMA").
- the CMA is provided over a length including a portion of the tapered bundle and a portion of combiner's output fiber 26.
- the CMA is configured with three consecutive - " upstream, intermediary and downstream ⁇ zones 38, 40 and 42, respectively, and is operative to minimize the amount of cladding light.
- the cladding light propagates in. opposite propagating and counter-propagating directions and, as known to one of ordinary skill in the fiber laser art, negatively affects the fiber and other optical components of laser system 10. Even a hundred- watt back reflected cladding light, which in the disclosed system may easily reach kWs, can be damaging to combiner 22. but even more so to individual SM systems that may receive this light through respective fibers 19 and other waveguides upstream from combiner 22.
- the upstream zone 38 extending along a portion 24 of the tapered bundle and terminating at a short distance from splice 30, is configured to at least minimize propagating of back reflected light before this light will reach individual LM laser systems 18 (FIG. 1) and other components upstream therefrom.
- the back reflected light has several regions of origin, For example, workpiece 21 partially reflects signal light which is coupled both into the cladding and core of a feeding fiber 82 (FIG. 1) fused to combiner output fiber 26.
- the zone 38 is structured to deal with backreflected light that initially is coupled into core of feeding fiber 82 and further into core 44' of output fiber 26 (FIG. 2d) which guides the light to splice region 30. Since the overlap between cross-sectional areas of respective downstream end 24 and output fiber 26, w hich define region 30, is not ideal, back reflected light fills up a greater area of the downstream end of the bundle than core 44 (FIG. 2). Hence the light not confined to the core of the downstream end of the tapered bundle bleeds out. To remove this light, cladding 34 of each fiber 19 is replaced with a protective polymeric layer 36 which is thus in direct, contact with the core of downstream end 24 of the tapered bundle and has a refractive index higher than that of both core 32 and protective coating 34.
- polymer 36 initially fills up housing 23 and interstices between fibers 19 which still have respective protective coatings 34 (FIG. 2a), Within zone 38, polymer 36 initially removes ' backref!ected light directly from core 44 of downstream end 24 and further irom protective coatings 34 of respective individual fibers 19 where they remain intact. The polymer 36 terminates at a short distance from splice 30 between bundle's downstream end 24 and the upstream end of output fiber 26.
- intermediate zone 40 of the disclosed CMA extends from the end of upstream zone 38 over the downstream end 24 of the tapered bundle and then through splice 30 and terminates at a distance upstream from the downstream end region of output fiber 26.
- the latter is stripped from its protective coating along intermediary zone 40, Instead., it is a polymeric layer 39 (FIG. 2b) that covers inner cladding 43 of output fiber 26 which has a refractive index at least equal to or higher than that of layer 39. Accordingly, layer 39 is configured to minimize losses of forward propagating signal light by preventing its decoupling from cladding 43.
- downstream zone 42 of the absorber is configured with polymeric layer 46 which is configured to minimize the amount of forward propagating signal light guided along cladding 43 of output fiber 26.
- the downstream zone 42 extends over the larger portion of output fiber 26, which is shipped from the protective coating, and partly overlays the downstream end of this fiber still having protective coating 50 (FIG, 2d). The latter is left in tact along the end region of output fiber 26 to improve its coupling to housing 23 (FIG, 2).
- polymeric layer 46 is configured with a host material, such as silicone gel, which has a refractive coefficient substantially equal to that of quartz.
- the host material is doped with a plurality of diffusers including, for example, particles of ⁇ 2 ⁇ 3 .
- the diffusers do not absorb light incident thereupon; they omni-direetiona!ly scatter it with a portion of scattered light being directed outside fiber 26.
- the high NA forward propagating dad-guided light when incident on the diffusers, can be partially guided into a potting materia! covering the absorber in housing 23 and further through the housing to a heat sink not shown here.
- the concentration and distribution of diffusers are selected to provide a substantially uniform removal of high IMA signal.
- the absorbed light, whether it is forward- or back reflected-propagatmg light should be efficiently transferred to a heat sink; otherwise the structural integrity of combiner 22 can be irreversibly compromised.
- the housing 23, enclosing combiner 22 and pari of output fiber 26 which are protected by the absorber, is provided with a semi- spherical groove 25 (FlGs. 2 and 2a) receiving combiner 22 and thus contributing to the mechanical and thermal stability of the entire laser system.
- the material of housing 23 is selected with high heat resistance and low coefficient of thermal expansion so as to minimize the degree of deformation of housing 23 at elevated temperatures during the operation of the disclosed fiber laser system. Otherwise, the housing's elongation may damage fibers and/or negatively affect the optical parameters.
- the material includes copper layered with a strip of gold or a tungsten copper (CuW) pseudo alloy.
- CuW tungsten copper
- system 1.0 may have a reliable monitoring system including several photodiode detectors.
- a sensor 100 is positioned in close vicinity of the upstream of combiner 22 to detect back reflected light propagating along the core 44 (FIG. 2a).
- the photodiode 104 is located to detect remaining back reflected " light not removed by system absorber 80.
- the power losses of signal light can be monitored at any convenient location along the waveguide, for example, a sensor may be positioned to measure power of signal light at the output of combiner 22.
- FIG. 3 illustrates a clad-guided light stripper (“CLS") 80 provided over the downstream end region of system output fiber 26 and feeding fiber assembly which is configured with upstream MM passive fiber 90 and downstream delivery fiber 82. All of the fibers 26, 90 and 82 are uniformly configured with respective cores and claddings being substantially uniformly dimensioned.
- the CLS 80 includes polymer directly coated over the claddings of respective fibers 26, 90 and 82 and thus configured with three zones.
- the upstream zone 86 of CLS 80 covers the area stripped from a protective coating of the downstream end of output fiber 26,
- the refractive index of polymer along zone 86 is higher than that of the inner cladding which allows removing a light portion of signal light guided along the cladding in the propagating direction,
- the intermediary zone 92 of CLS 80 is configured with a relatively low index of refraction which confines the cladding- guided signal light to fiber 90
- downstream zone 88 includes a polymeric layer 94 with a refractive index higher than that of the adjacent cladding.
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- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- General Physics & Mathematics (AREA)
- Optical Couplings Of Light Guides (AREA)
- Lasers (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
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Abstract
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Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2015560280A JP6387356B2 (en) | 2013-02-28 | 2014-02-26 | Ultra high power fiber laser system with multimode-multimode fiber coupler |
EP14757695.3A EP2962140B1 (en) | 2013-02-28 | 2014-02-26 | Ultra-high power fiber laser system with multimode-multimode fiber combiner |
KR1020157023314A KR102217718B1 (en) | 2013-02-28 | 2014-02-26 | Ultra-high power fiber laser system with multimode-multimode fiber combiner |
CN201480010628.8A CN105026969B (en) | 2013-02-28 | 2014-02-26 | With multimode-multimode fibre bundling device super high power fiber ring laser system |
ES14757695T ES2886920T3 (en) | 2013-02-28 | 2014-02-26 | Ultra-high power fiber laser system with multimode-multimode fiber coupler |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US201361770607P | 2013-02-28 | 2013-02-28 | |
US61/770,607 | 2013-02-28 |
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WO2014134173A1 true WO2014134173A1 (en) | 2014-09-04 |
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PCT/US2014/018688 WO2014134173A1 (en) | 2013-02-28 | 2014-02-26 | Ultra-high power fiber laser system with multimode-multimode fiber combiner |
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Country | Link |
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US (1) | US9140856B2 (en) |
EP (1) | EP2962140B1 (en) |
JP (1) | JP6387356B2 (en) |
KR (1) | KR102217718B1 (en) |
CN (1) | CN105026969B (en) |
ES (1) | ES2886920T3 (en) |
WO (1) | WO2014134173A1 (en) |
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EP2962141B1 (en) * | 2013-02-28 | 2020-12-16 | IPG Photonics Corporation | Low-mode high power fiber combiner |
US9338915B1 (en) | 2013-12-09 | 2016-05-10 | Flextronics Ap, Llc | Method of attaching electronic module on fabrics by stitching plated through holes |
US10310201B2 (en) * | 2014-08-01 | 2019-06-04 | Nlight, Inc. | Back-reflection protection and monitoring in fiber and fiber-delivered lasers |
ES2959675T3 (en) * | 2015-05-26 | 2024-02-27 | Ipg Photonics Corp | MULTI-BEAM LASER SYSTEM AND WELDING METHOD |
GB2540432A (en) | 2015-07-17 | 2017-01-18 | Spi Lasers Uk Ltd | Apparatus for combining optical radiation |
US10261329B2 (en) * | 2016-08-26 | 2019-04-16 | Nlight, Inc. | Fiber combiner with input port dump |
JP6363680B2 (en) | 2016-11-16 | 2018-07-25 | ファナック株式会社 | Laser equipment |
JP6564418B2 (en) * | 2017-04-20 | 2019-08-21 | ファナック株式会社 | Optical power monitor device and laser device |
JP2018190918A (en) * | 2017-05-11 | 2018-11-29 | 株式会社フジクラ | Combiner, fiber laser device, and method of manufacturing combiner |
JP6596544B1 (en) | 2018-06-22 | 2019-10-23 | 株式会社フジクラ | Photodetection device and laser device |
CN109239848A (en) * | 2018-09-29 | 2019-01-18 | 武汉锐科光纤激光技术股份有限公司 | A kind of optical-fiber bundling device |
CN110429464A (en) * | 2019-07-19 | 2019-11-08 | 东莞理工学院 | A kind of superpower laser bundling device |
US20230258869A1 (en) * | 2020-07-14 | 2023-08-17 | Nlight, Inc. | Combiner housing for optical fiber combiner |
TWI788076B (en) | 2021-10-29 | 2022-12-21 | 財團法人工業技術研究院 | Optical fiber module and manufacturing method thereof |
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2014
- 2014-02-26 ES ES14757695T patent/ES2886920T3/en active Active
- 2014-02-26 EP EP14757695.3A patent/EP2962140B1/en active Active
- 2014-02-26 CN CN201480010628.8A patent/CN105026969B/en active Active
- 2014-02-26 JP JP2015560280A patent/JP6387356B2/en active Active
- 2014-02-26 US US14/191,179 patent/US9140856B2/en active Active
- 2014-02-26 WO PCT/US2014/018688 patent/WO2014134173A1/en active Application Filing
- 2014-02-26 KR KR1020157023314A patent/KR102217718B1/en active IP Right Grant
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Also Published As
Publication number | Publication date |
---|---|
EP2962140B1 (en) | 2020-12-16 |
JP2016513295A (en) | 2016-05-12 |
US20140241663A1 (en) | 2014-08-28 |
ES2886920T3 (en) | 2021-12-21 |
KR20150122663A (en) | 2015-11-02 |
JP6387356B2 (en) | 2018-09-05 |
EP2962140A4 (en) | 2016-10-26 |
CN105026969A (en) | 2015-11-04 |
EP2962140A1 (en) | 2016-01-06 |
KR102217718B1 (en) | 2021-02-19 |
CN105026969B (en) | 2019-01-01 |
US9140856B2 (en) | 2015-09-22 |
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