HIGH POWER OPTICAL FIBER LASER COMBINER
20190199055 ยท 2019-06-27
Inventors
- JIAN-HUNG LIN (Taoyuan City, TW)
- CHIANG-HSIN LIN (Taoyuan City, TW)
- PO-TSE TAI (Taoyuan City, TW)
- WEI-CHUNG YEN (TAOYUAN CITY, TW)
Cpc classification
H01S3/094007
ELECTRICITY
H01S3/06708
ELECTRICITY
G02B6/4296
PHYSICS
G02B6/02066
PHYSICS
G02B6/2804
PHYSICS
G02B6/2856
PHYSICS
International classification
H01S3/23
ELECTRICITY
G02B6/28
PHYSICS
Abstract
A high power optical fiber laser combiner includes a plurality of input port fibers; an output port fiber including a cladding and a propagating layer, the cladding being used to clad the propagating layer, and the cladding including a micro-nano structure on a surface thereof for removing a residual power in the cladding; and a bundling portion for bundling the input port fibers, and the input port fibers spliced to the output port fiber. The heat effect accumulation of laser power on the cladding can effectively be reduced by the micro-nano structure of the high power optical fiber laser combiner. The tolerant power and bundling power of the optical fiber laser combiner can be raised to increase the output power of the optical laser.
Claims
1. A high power optical fiber laser combiner, comprising: a plurality of input port fibers; an output port fiber including a cladding and a propagating layer, the cladding being used to clad the propagating layer, and the cladding including a micro-nano periodic grating structure on a surface thereof for removing a residual power in the cladding by using the diffraction principle of the grating; a bundling portion for bundling the input port fibers, and the input port fibers spliced to the output port fiber.
2. The high power optical fiber laser combiner of claim 1, wherein the input port fibers are single mode or multiple mode optical fiber.
3. The high power optical fiber laser combiner of claim 1, wherein the output port fiber is made from glass tube technology.
4. The high power optical fiber laser combiner of claim 1, wherein the cladding has a range of working temperature from room temperature to 80 C.
5. The high power optical fiber laser combiner of claim 1, wherein the micro-nano structure has a range of thickness from 1 nm to 20 m, and a range of length from 1 mm to 10 cm.
6. The high power optical fiber laser combiner of claim 1, wherein the micro-nano structure is an embedded type or an attached type.
7. The high power optical fiber laser combiner of claim 1, wherein the output port fiber propagates a light power of 200 W to 12 kW.
8. The high power optical fiber laser combiner of claim 1, wherein the output port fiber is single mode or multiple mode optical fiber.
9. A high power optical fiber laser combiner, comprising: a plurality of input port fibers; an output port fiber including a cladding and a propagating layer, the cladding being used to clad the propagating layer, and the cladding including a micro-nano aperiodic structure on a surface thereof for removing a residual power in the cladding by changing or destroying a full reflection angle of the laser light that propagates in the cladding of the output port fiber; and a bundling portion for bundling the input port fibers, and the input port fibers spliced to the output port fiber.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0019]
[0020]
[0021]
[0022]
[0023]
[0024]
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0025] The advantages and effects of the present disclosure will be apparent from the following detailed description for the specific embodiments when a person having ordinary skill in the art reads the disclosure of the specification.
[0026] Please refer to
[0027] Please refer to
TABLE-US-00001 7 proximal single mode double-clad optical fibers Diameter of fiber 20 1.5(m)/130 1.0(m) Numerical aperture (NA) 0.08 0.005/0.46 Refractive index of fiber core (n.sub.core) 1.446 Refractive index of inner cladding 1.444 (n.sub.cladding) Diameter of outer cladding optical 245 10(m) fiber 1 multiple mode optical fiber Diameter of fiber 105 3.0(m)/125 2.0(m) Numerical aperture (NA) 0.22 0.02 Refractive index of fiber core (n.sub.core) 1.446 Refractive index of inner cladding 1.429 (n.sub.cladding) Diameter of outer cladding optical 245 15(m) fiber
Referring to the relevant parameters of the glass tube, the glass tube is made from a material of ground glass tube doped with ions of fluorine (F) and has a refractive index of 1.429 as well as a numerical aperture of 0.22. The refractive index of 1.429 is smaller than a refractive index (1.444) of inner cladding of 7 proximal single mode cladding optical fibers so that the laser light can effectively be limited in the proximal single mode optical fiber. The outer diameter and the inner diameter of the ground glass tube respectively are 1100 m20 m and 800 m10 m.
[0028] In order to calculate the laser power that diverges to the glass layer of the glass tube and in the cladding of output multiple mode optical fiber, the integral calculation of the photoelectric field power of the bundling portion and the output port fiber (42) is performed first, the bundling portion is divided into a tapering zone (43) and a belt zone (44), a tapering and splicing are respectively performed for the output port fiber (42), and the output port fiber (42) can be divided into a cladding and a propagating layer, wherein the propagating layer is coated with the cladding, the tapering zone (43) and the belt zone (44) are constant respectively on 12 mm and 5 mm in length, Y axis coordinate is set to 0, and the results of which are calculated as the following table:
TABLE-US-00002 Power integral region Integral power efficiency Inner of glass tube (7 proximal single 0.9915 mode optical fibers and inner air portion) glass layer of glass tube and inner of 0.9972 glass tube Propagating layer of output multiple 0.9879 mode optical fiber (core) Propagating layer of output multiple 0.9929 mode optical fiber (core) and cladding
The power efficiency of the glass tube inner (7 proximal single mode optical fibers and inner air portion) in the belt zone (44) is 0.9915, and the glass layer of the glass tube included is 0.9972. After coupling to the output multiple mode optical fiber, the power efficiency of a propagating layer of output multiple mode optical fiber (core) is 0.9879, and the cladding included is 0.9929. There is about 0.43% of the power from the belt zone (44) to the output multimode optical fiber diverged into the air, having about 0.5% of the power in the cladding of the output multiple mode optical fiber. With an application of a four kilowatts (4 kW) laser combiner, 0.5% laser power of which is diverged nearly the power of 20 W at a site of the belt zone (44) spliced with the output multiple mode optical fiber, and the laser power of 20 W remains in the cladding of the output multiple mode optical fiber, and the present disclosure can treat the laser power that is remained in the cladding of the output multiple mode optical fiber.
[0029] In an embodiment of the application of the present disclosure, a high power fiber laser combiner is configured with an input port fiber (10) of 7 proximal single mode double-clad optical fibers bundled by glass tube technology, then heating tapered by a welding machine, and finally spliced with an output port multiple mode optical fiber having a micro-nano structure. The structural parameters of design as follows: the tapering rate of bundling fiber is 3, the tapering length is 10 mm, the belt length is 5 mm, and the output port fiber is far from the site of splicing the input port bundling fiber about 2-3 mm. The micro-nano structure is made on a surface of the cladding of the output port fiber by a chemical etching method. Because the thickness of the cladding of the output port multiple mode optical fiber is only 20 m, the etching time must be controlled properly to ensure the etching being less than 20 m and the coupling efficiency being kept to the best. In an experiment, a set of optical fiber lasers with 300 W and 1 kW is used as a laser light source, the laser light is propagated from an input port to an output port of a laser combiner of the present disclosure, the power of the laser light outputted from the output port is determined by a power meter for quantifying the coupling efficiency of the element. During the determination, a thermographer is used to determine and record the temperature change of the combiner.
[0030] To highlight the advantages of using the micro-nano structure, two commonly used methods of a thermal pad and a glue having a high refractive index are used to compare with, of which the thermal pad directly helps the heat dissipation of the outer cladding of the output port, and the glue having a high refractive index is coated on the inner cladding with the principle of the same as the micro-nano structure by mainly removing the residual laser power in the inner cladding of the output port to reduce power load of the outer cladding of the output port. Basically, common outer claddings are polymer materials that can only withstand 20 W of laser power, and the temperature must not exceed its glass transition temperature (Tg), about 80 C.
[0031] Please refer to
[0032] In order to further determine the property and the performance of temperature rise of the laser combiner of the present disclosure having the micro-nano structure, the injection power is raised to 202 W, and all the 7 input port have the coupling efficiency more than 98%. It is found that the element of the present disclosure can withstand the injection power of 1 kW by the previous determination of hundreds of Watts injection. Please refer to
[0033] The experiment has demonstrated that the present disclosure relating to a laser combiner having a micro-nano structure can be applied to multi-kW level optical fiber laser combiner. The high power optical fiber laser combiner of the present disclosure has advantages as follows: the laser combiner has a higher tolerant power, and can remove the power on the cladding of 200 W that is demonstrated by the experiment; the laser combiner has a high augmentation of the power, and can raise the optical fiber laser to ten something kW and above by a distribution mechanism; the laser combiner is easy to integrate with a process of laser combiner without increasing the original volume of the device; except that the laser combiner can be applied in a pump or laser combiner of the high power optical fiber laser system, and the laser combiner of the design can be directly applied to directly couple the power of multiple bundles into a high kW level multiple mode optical fiber laser.
[0034] The above embodiments of the present disclosure made only by way of example to describe the feature and effect of the present disclosure, and it should not be considered as the scope of substantial technical content is limited thereby. Various possible modifications and alternations of the embodiments could be carried out by those of ordinary skill in the art without departing from the spirit and scope of the present disclosure. Therefore, the scope of the present disclosure is based on the appended claims.