The present invention relates to a leakage light removal structure, and more particularly to a leakage light removal structure for removing leakage light produced at a fusion splicing point of an optical fiber in a fiber laser or the like.
Generally, when optical fibers are to be connected to each other by fusion splicing, a covering material is removed from an end of each optical fiber by a predetermined length to expose a cladding. In such a state, those two optical fibers are, connected to each other by fusion splicing. (See, e.g., Patent Literature 1.)
At the fusion splicing point 700 between the optical fibers 510 and 610, light propagating through the core of the optical fiber 510 may leak out to the cladding 630 of the output optical fiber 610 due to microbend or axial misalignment caused at the fusion splicing point 700. When general optical fibers are fused together, significant problems do not occur because the power of light propagating through the core is not so high. In optics through which high-power light propagates, such as a fiber laser, however, high-power leakage light is produced in the cladding 630 of the output optical fiber 610 even if only slight misalignment is caused to the fusion splicing point 700.
If the covering material 620 of the output optical fiber 610 has a refractive index higher than a refractive index, of the cladding 630, the leakage light produced in the cladding 630 of the optical fiber 610 is introduced into the covering material 620 from the cladding 630 and absorbed therein.
With the structure shown in
Patent Literature 1: JP 2009-116076 A
The present invention has been made in view of the above drawbacks of the prior art. It is, therefore, a first object of the present invention to provide a leakage light removal structure that can efficiently remove leakage light produced in an optical fiber without causing local heat generation or fire.
A second object of the present invention is to provide a fiber laser capable of emitting a high-quality laser beam with high reliability.
According to a first aspect of the present invention, there is provided a leakage light removal structure that can efficiently remove leakage light produced in an optical fiber without causing local heat generation or fire. The leakage light removal structure is used to remove leakage light in an optical fiber having a core, a cladding covering the core and having a refractive index lower than the core, and a covering material covering the cladding having a refractive index higher than the cladding. The leakage light removal structure has a fiber housing that houses part of the optical fiber, a covering material extension portion covering part of a whole circumference of the cladding by extending part of the covering material along a longitudinal direction of the optical fiber within the fiber housing, and a cladding exposure portion in which a portion of the whole circumference of the cladding other than the covering material extension portion is exposed within the fiber housing. The cladding exposure portion is covered with a medium or a resin having a refractive index lower than the refractive index of the cladding.
With such a configuration, when leakage light produced in the cladding in the optical fiber reaches an interface between the cladding and the covering material extension portion, it enters the covering material extension portion because the refractive index of the covering material extension portion is equal to or higher than the refractive index of the cladding. Thus, the leakage light is emitted to the covering material extension portion. Accordingly, it is possible to prevent generation of heat or fire that would be caused by leakage light. Thus, the reliability of the emission optics can be improved.
Furthermore, the covering material extension portion extends only over part of the whole circumference of the cladding. Therefore, the amount of the leakage light emitted into the covering material at the most upstream part of the covering material extension portion can be reduced as compared to a conventional structure in which the whole circumference of the cladding is covered with the covering material. Accordingly, it is possible to suppress local heat generation caused by leakage light absorbed in the covering material and thus to improve the reliability of the leakage light removal structure.
According to a second aspect of the present invention, there is provided a fiber laser capable of emitting a high-quality laser beam with high reliability. The fiber laser has a signal light generator operable to generate signal light, a pump laser diode operable to generate pump light, and a clad pumping fiber. The clad pumping fiber has a core through which the signal light propagates, a cladding which covers the core and through which the pump light propagates, and a covering material covering the cladding and having a refractive index higher than a refractive index of the cladding. The fiber laser has an output optical fiber connected to the clad pumping fiber by fusion splicing and the aforementioned leakage light removal structure configured to remove leakage light produced in the cladding of the output optical fiber.
In order to suppress local heat generation more effectively, it is preferable to form the covering material extension portion with a range of angles equal to or less than 180° about an axis of the optical fiber in a cross-section perpendicular to the axis. The refractive index of the medium or the resin covering the cladding exposure portion should preferably be lower than the refractive index of the covering material. The fiber housing should preferably include a heat radiator plate having a good thermal radiation characteristic, which is disposed so as to face the cladding exposure portion.
According to a leakage light removal structure of the present invention, it is possible to efficiently remove leakage light and to suppress local heat generation due to emission of the leakage light to improve the reliability. Furthermore, according to a fiber laser of the present invention, there can be provided a fiber laser capable of emitting a high-quality laser beam with high reliability.
Embodiments of a leakage light removal structure according to the present invention will be described in detail below with reference to
With a clad pumping fiber 40 thus constructed, signal light from the signal light generator 10 propagates within the core 60, and pump light from the pump LDs 20 propagates within the cladding 62 and the core 60. While the pump light propagates through the core 60, ions of the rare earth element doped in the core 60 absorbs the pump light to cause excitation. Thus, the signal light propagating through the core 60 is amplified by stimulated emission.
At the fusion splicing point 180, light propagating through a core of the clad pumping fiber 40 may leak out to the cladding 162 of the output optical fiber 140 due to microbend or axial misalignment caused at the fusion splicing point 180. In the present embodiment, a leakage light removal structure 70 is provided for removing such leakage light.
Specifically, on a downstream side of the fusion splicing point 180 within the fiber housing 72, a portion of the covering material 164 is removed over a part of the whole circumference of the output optical fiber 140, for example, within a range of angles equal to or more than 180° (e.g., 180°) about an axis of the output optical fiber 140 in a cross-section perpendicular to that axis (
Furthermore, an interior of the fiber housing 72 is filled with a resin (e.g., UV curable resin) 76 having a refractive index that is lower than the refractive index of the cladding 162 of the output optical fiber 140 and the refractive index of the covering material 164 at a wavelength being used. The cladding exposure portion 174 and the covering material extension portion 175 are covered with this resin 76. The reference numeral 77 in
With such a configuration, when light propagating through a core of the clad pumping fiber 40 leaks out to the cladding 162 of the output optical fiber 140 due to a minute bend or an axial misalignment caused at the fusion splicing point 180, the leakage light propagates through the cladding 162 because the cladding 162 is covered with the resin 76 having a refractive index that is equal to or lower than the refractive indexes of the air cladding 182 and the cladding 162. When the leakage light that has propagated through the cladding 162 reaches an interface between the cladding 162 and the covering material extension portion 175, it enters the covering material extension portion 175 because the refractive index of the covering material extension portion 175 is equal to or higher than the refractive index of the cladding 162. Thus, the leakage light is emitted to the covering material extension portion 175. Accordingly, it is possible to prevent generation of heat or fire that would be caused on a downstream side of the leakage light removal structure 70 by leakage light. Thus, the reliability of the emission optics can be improved.
In the present embodiment, only part of the whole circumference of the cladding 162 is covered with the covering material extension portion 175. Therefore, the amount of the leakage light emitted into the covering material 164 at the most upstream part of the covering material extension portion 175 can be reduced as compared to the conventional structure shown in
In the present embodiment, the resin 76 covering the covering material 164 has a refractive index lower than that of the covering material 164. Therefore, leakage light emitted into the covering material 164 is confined in the covering material 164 and absorbed in the covering material 164 while it propagates through the covering material 164. However, since part of the whole circumference of the cladding 162 is covered with the material extension portion 175 as described above, the amount of leakage light per unit length can be reduced as compared to the conventional structure. Thus, the total amount of generated heat can be reduced.
As shown in
For example, the aforementioned covering material extension portion 175 can be formed with use of an apparatus 80 as shown in
When the covering material extension portion 175 is formed with use of this apparatus 80, the output optical fiber 140 is first held by the holders 82. In that state, the blade 84 is brought into contact with the surface of the output optical fiber 140 and moved in a longitudinal direction of the output optical fiber 140 by a certain distance. Thus, the covering material 164 present on the surface of the output optical fiber 140 is peeled by the certain distance so as to expose the cladding 162 from the covering material 164.
Then the output optical fiber 140 held by the holders 82 is rotated through 20° about its axis, and the blade 84 is moved back to the original position. Thereafter, the blade 84 is brought into contact with the surface of the output optical fiber 140 again and moved in the longitudinal direction of the output optical fiber 140 by the same distance as moved previously. Thus, the covering material 164 is similarly peeled by the certain distance so as to expose the cladding 162 from the covering material 164. For example, the above operation is repeated nine times in total to expose the cladding 162 from the covering material 164 with a range of 180° about the axis of the output optical fiber 140 in the cross-section perpendicular to that axis (
The present embodiment describes an example in which the cladding exposure portion 174 and the covering material extension portion 175 are covered with the resin 76. The cladding exposure portion 174 and the covering material extension portion 175 may not be covered with the resin 76. The cladding exposure portion 174 and the covering material extension portion 175 may be covered with a medium (air or the like) that has a refractive index lower than the refractive index of the cladding 162 (and the refractive index of the covering material 164). In order to prevent the covering material extension portion 175 from being peeled from the surface of the cladding 162 and to promote absorption of heat from leakage light absorbed in the covering material extension portion 175, it is preferable to cover the cladding exposure portion 174 and the covering material extension portion 175 with the resin 76 as in the present embodiment. Furthermore, this resin 76 may be filled into the air cladding 182 within the fiber housing 72.
First, a conventional leakage light removal structure shown in
Within a reinforcement member 500 formed of a ceramic member having a coefficient of linear expansion that was adjusted to that of quartz glass, the claddings 530 and 630 of the optical fibers 510 and 610 were jointed and fused to each other. Opposite ends of the reinforcement member 500 and the optical fibers 510 and 610 were fixed with a hard UV curable resin.
In that state, the fiber laser was operated at an output of 600 W. The most upstream part 642 of the covering material 620 was locally heated as expected and increased in temperature to about 90° C. Depending upon the heat resistance of the covering material 620, the covering material 620 suffers from heat deterioration when the temperature of the covering material 620 increases during a production process. Then the amount of absorption of light increases, which causes an increased temperature of the covering material 620. Thus, negative feedback is generated. According to calculation from experiments, the lifetime of the covering material 620 used at that time was about 20,000 hours. It was found that the covering material 620 had a very short lifetime.
A light removal structure 70 as shown in
The covering material extension portion 175 was produced with use of the apparatus shown in
The fiber laser was operated under the same conditions as the test for the conventional leakage light removal structure. The greatest temperature increase of the covering material extension portion 175 was as low as 55° C. Thus, it was found that local temperature increase was reduced. When the lifetime of the covering material 164 was calculated based on this result of the temperature increase, it would be 90,000 hours or more. Thus, it is found that the lifetime can overwhelmingly be extended as compared to the conventional leakage light removal structure.
Although some preferred embodiments of the present invention have been described, the present invention is not limited to the aforementioned embodiments. It should be understood that various different forms may be applied to the present invention within the technical idea thereof.
The present invention is suitable for use in a leakage light removal structure for removing leakage light produced at a fusion splicing point of optical fibers or the like in a fiber laser.
Number | Date | Country | Kind |
---|---|---|---|
2014-018602 | Feb 2014 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
5926600 | Pavlath | Jul 1999 | A |
5970197 | Pavlath | Oct 1999 | A |
5995697 | Byron | Nov 1999 | A |
6317547 | Pavlath | Nov 2001 | B1 |
20020186947 | Abe | Dec 2002 | A1 |
20070065083 | Singh | Mar 2007 | A1 |
20130308661 | Nishimura et al. | Nov 2013 | A1 |
Number | Date | Country |
---|---|---|
63-214630 | Sep 1988 | JP |
11-44823 | Feb 1999 | JP |
2009-69492 | Apr 2009 | JP |
2009-116076 | May 2009 | JP |
2011-186399 | Sep 2011 | JP |
2007148127 | Dec 2007 | WO |
2013001734 | Jan 2013 | WO |
Entry |
---|
International Search Report dated Apr. 28, 2015, issued in counterpart International Application No. PCT/JP2015/052807 (2 pages). |
Search Report dated Oct. 5, 2017, issued in counterpart European Application No. 15743598.3 (6 pages). |
Number | Date | Country | |
---|---|---|---|
20160336711 A1 | Nov 2016 | US |
Number | Date | Country | |
---|---|---|---|
Parent | PCT/JP2015/052807 | Feb 2015 | US |
Child | 15225181 | US |