US20090154882A1

US20090154882A1 - Means of Coupling Light Into Optical Fibers and Methods of Manufacturing a Coupler

Info

Publication number: US20090154882A1
Application number: US12/206,577
Authority: US
Inventors: Arto Salokatve
Original assignee: Arto Salokatve
Current assignee: Corelase Oy
Priority date: 2007-12-14
Filing date: 2008-09-08
Publication date: 2009-06-18
Also published as: JP5649973B2; US7991255B2; EP2071375A1; WO2009077636A1; EP2071375B1; US20090154879A1; JP2011507251A

Abstract

The invention relates to a pump coupler (2) and a manufacturing method. The pump coupler (2) comprises a least one signal fiber (50) for outputting optical energy, multiple pump fibers (31) for inputting optical energy into the signal fiber (50), and a coupling structure (40) for coupling the optical energy of the pump fibers (31) into the signal fiber (50). A signal feed-through fiber (32) goes through the coupling structure (40). In accordance with the invention the coupling structure (40) is a tapering capillary tube (40) having a first wide end (65) and a second narrow end (70), the pump fibers (31) are connected to the wide end of the capillary tube (40), and at least the narrow end (70) of the capillary tube (70) is collapsed around the signal fiber (32).

Description

CROSS-REFERENCE TO RELATED APPLICATION

The present application is a continuation of International Application No. PCT/FI2007/050690, filed Dec. 14, 2007 and entitled “Means of Coupling Light Into Optical Fibers and Methods of Manufacturing a Coupler.” The foregoing application is incorporated herein by reference.
The present invention relates to an optical coupler and more particularly to an optical coupler based on optical fiber.
The present invention relates also to methods for manufacturing an optical coupler.
Fiber lasers have many attractive properties that make them suitable for various industrial applications. Such properties can include one or more of good beam quality, easy thermal management, compact size, and good efficiency. Therefore, fiber lasers are continuing to gain market share from more conventional types of lasers, such as solid-state and gas lasers. Fiber lasers are able to produce optical output in the several kW range with excellent beam quality. Thus, these lasers can be used for macro-machining applications like welding and cutting of metal. Furthermore, fiber lasers lend themselves for operation with ultra-short pulses by a method of mode-locking, enabling them to be used in micro-machining applications as well.
In the following discussion it is assumed that the reader has some basic knowledge of the structure of optical fibers. Thus, the concepts of a fiber core, cladding, and coating are not discussed in detail. It suffices here to mention that the laser radiation generated in a fiber laser, here referred to as the signal, is propagating in the core of the fiber, whose diameter is typically between few microns and few tens of microns. A so called double-clad fiber comprises a core, a primary cladding that confines the signal light to the core and guides the pump light, and the secondary cladding that confines the pump light into the primary cladding. The core is typically made of doped fused silica, the primary cladding of fused silica, and the secondary cladding of low-index polymer or doped fused silica. The meaning of pump light is discussed later.
For later reference some further terms or concepts related to fiber processing are also briefly discussed here. Splicing is a well-known term in the art of fiber optics. It refers to joining at least two glass parts together for optical communication, such as, for example, by heating the parts close to the joint to a high temperature to make the glass soft, and then pushing the parts into physical contact with each other. Hence, an intimate and transparent contact is formed between the parts. The heat source for splicing can be an electric arc, a hot filament or a CO₂laser, for instance. Cleaving means cutting a glass part so as to form a flat surface to it. In optical fibers, the cleave plane usually lies essentially perpendicular to the optical axis of the fiber (perpendicular cleave). It may also be essentially non-perpendicular (angle-cleave). Unless otherwise stated, in this document cleaving means producing a perpendicular cleave. An equivalent, although more laborious, means of getting a flat plane to the fiber tip is the well-known method of mechanical polishing. Cleaving can be done by mechanical means by scratching the fiber with a sharp blade made of hard material and applying tension to the fiber to break it, or by a laser. A good cleave for optical fibers makes high quality splicing possible. Stripping means removing the polymer coating from the fiber, usually in a distance of a few centimeters from its end. Collapsing in this document refers to heating a hollow piece of glass, such as a capillary tube, in order to make it soft and to make it shrink. Surface tension forces and/or differential pressure between the inside and outside region of the piece may aid in the shrinking. Heating can be done with the same methods as in splicing.
As any laser, a fiber laser can include a gain medium, an optical resonator, means of coupling energy into the gain medium, and means of extracting light out of the optical resonator. The gain medium in a fiber laser can include a length of an optical fiber, the active fiber, generally made of fused silica. Typically the core of the active fiber is doped with optically active atoms such as rare-earth atoms Er or Yb. The optical resonator can be formed by surrounding the gain medium with mirrors that, when properly aligned with respect to the active fiber, force some of the light emitted by the active atoms to bounce between the mirrors through the gain medium and get amplified. The mirrors can be either bulk optical mirrors, or they can be directly fabricated into optical fibers. In the latter case they are usually fiber Bragg gratings (FBGs), but other fiber-based mirrors exist also. Fiber-based mirrors are attractive since they can be directly attached or spliced to other fibers with very low optical losses. The mirrors, or typically only one of the two mirrors, are made only partially reflective to provide a means of extracting light out of the optical resonator. In fiber lasers, the extracted light can be further guided with a length of optical fiber close to the point of interest, such as the work-piece. The extracted light thus forms the beam of laser light that can be used in the final application.
The gain medium, i.e. active fiber in a fiber laser, is typically an electric insulator. Thus, energy cannot usually be supplied to it directly in the form of electric power. However, the active atoms absorb optical radiation within certain wavelength ranges called the absorption bands. This property is utilized in fiber lasers by feeding or ‘pumping’ the energy into the gain medium in the form of light. This light is called the pump light, and is usually generated by pump diode lasers, which preferably are fiber coupled. Thus, a fiber laser includes a means of coupling the said pump light into the active fiber. It is further desirable, that the coupling means has low optical losses, i.e. almost all of the pump energy can be coupled into the gain medium. It can be desirable that the coupling means has a signal feed-through where the laser signal can pass through it with low optical losses. The latter property greatly helps in the laser cavity construction, and is a favored prerequisite for industrial class fiber lasers.

THE PRIOR ART

There are a number of ways of making a pump coupler using free-space optics, such as those shown in U.S. Pat. No. 5,854,865, U.S. Pat. No. 6,529,657 and JP2007156097.
In U.S. Pat. No. 5,864,644 the input fibers, which may include a signal fiber, are simply bundled together and tapered to fuse the fibers together. Then the fused bundle is cleaved from the waist and spliced to an output fiber. This approach also involves tapering of both the pump fibers and the signal fiber. The core diameter of the signal fiber is reduced in the process. Furthermore, the output fiber needs to have the same reduced diameter of the core for low splicing losses. Hence, this coupler unavoidably has different core diameters at the input and at the output.
In U.S. Pat. No. 5,999,673 the coupler is made by tapering the pump fibers, and fusing them to the signal-carrying central fiber from the tapered portion allowing the pump light thus to be coupled to the signal fiber.
US2005105866 describes a coupler, where the pump fibers are essentially in optical contact with the active fiber along the longitudinal axis of the fibers. In this implementation, the pump fibers are manufactured in the same fiber drawing process as the active fiber in order to make and maintain optical contact between them by e.g. coating the whole structure with a polymer coating or by fusing them along their longitudinal axis.
In US2005105854 a fiber bundle includes pump fibers and a central fiber fused together. The bundle is then spliced to an output fiber. Performing such a splice can require careful alignment of the core of the signal fiber with that of the output fiber and also making a good contact of all pump fibers to the output fiber.
US2006251367 describes an optical fiber coupler with at least a first input optical fiber and at least one output optical fiber, said first input optical fibers comprising an antiguiding core.
WO2007090272 describes a multimode fiber coupler that has a structure in which multiple tapered pump fibers are coupled laterally to a multi-clad signal fiber. In the fusing process the bundle of tapered pump fibers and central fiber are twisted, heated and drawn to form a further taper with a waist in the bundle. The fused bundle is then cleaved from the waist and spliced to another multi-clad fiber.
This invention describes a practical means of coupling pump light into an optical fiber and a method of manufacturing it. From here onwards, the term pump coupler is used for the coupling means. In the coupler of this invention coupling can be performed with aid of a tapering capillary tube, to which the pump fibers and the signal fiber are coupled.
One or more of the following benefits may be obtained by the invention.
In this invention the pump coupler can include the property of having a low-loss signal feed-through for the laser radiation generated by the fiber laser. Furthermore, the signal feed-through made by the procedures of this invention can produce minimal degradation of the beam quality for the laser radiation traversing through it. Finally, with the coupler structure of this invention it is possible to achieve very high pump coupling efficiencies to the output fiber.

DETAILED DESCRIPTION OF THE INVENTION

FIG. 1 shows schematically one example of a fiber laser, which can be used in connection with the invention.

FIG. 2 shows schematically a second example of a fiber laser, which can be used in connection with the invention.

FIG. 3 shows schematically a third example of a fiber laser, which can be used in connection with the invention.

FIG. 4 shows schematically a fourth example of a fiber laser, which can be used in connection with the invention.

FIG. 5 a shows as a partially cross sectioned side view of one pump coupler in accordance with the invention.

FIG. 5 b shows cross section A of FIG. 5 a.

FIG. 6 shows a cross section of 6 pump fibers and a signal feed-through fiber, which can be used in a method in accordance with the invention.

FIG. 7 shows a side view of FIG. 6.

FIG. 8 shows as a side view a structure of FIGS. 6 and 7 in a next phase of the method in accordance with the invention.

FIG. 9 shows as a side view a structure of FIGS. 6, 7 and 8 in a next phase of the method in accordance with the invention.

FIG. 10 shows as a side view a pump coupler preliminary structure relating to a method step of a method in accordance with the invention.

FIG. 11 shows as a side view a structure of FIG. 10 in a next phase of the method in accordance with the invention.

FIG. 12 shows as a side view a structure of FIGS. 10 and 11 in a next phase of the method in accordance with the invention.

FIG. 1 describes one example of a configuration of a fiber laser. It includes a fiber-based laser resonator 1, which is composed of an active fiber 11, a high-reflective (HR) FBG mirror 12 and a low-reflective (LR) FBG mirror 13. The LR FBG 13 furthermore provides a means of extracting laser radiation out of the laser resonator 1 by having an optical reflectivity significantly smaller than 100%. Typical reflectivities for HR and LR FBGs are >90% and 10%, respectively. FIG. 1 also depicts a pump coupler 2, which interfaces to the pump sources via the pump fibers 31 and to exterior world and the fiber laser resonator via the signal feed-through fiber 32 and output signal fiber 50, respectively. The fiber laser cavity of FIG. 1 has a so-called counter-pumped configuration where the pump light and the output signal light are counter-propagating. Furthermore, in the example of FIG. 1 the pump coupler 2 lies outside the laser resonator 1. The cross marks in FIG. 1 denote splices between different fibers.
FIG. 2 describes another example of a fiber laser, the notations having the same meanings as in FIG. 1. The only difference to the resonator of FIG. 1 is that the pump-coupler 2 now resides inside the laser resonator 1, i.e. between the HR mirror 12 and LR mirror 13. In the configuration of FIG. 2 it is preferable for the pump coupler to have a low-loss signal feed-through, since it directly contributes to optical losses of the laser resonator 1.
FIG. 3 describes yet another configuration of a fiber laser. In this example the fiber laser resonator is pumped with two pump couplers 2 a and 2 b from both ends of the laser resonator 1. It is evident that by extensions or modifications of the shown configurations other configurations can be constructed.
As the power coupling capacity of each pump coupler is limited, higher power fiber lasers can be constructed by cascading pump couplers with multiple sections of active fibers. FIG. 4 shows an example for a fiber laser that has four pump couplers 2 a, 2 b, 2 c and 2 d, connected to two active fiber sections 11 a and 11 b. The section 11 a is pumped from both ends with pump couplers 2 a and 2 b, while the active fiber section 11 b is pumped from both ends with pump couplers 2 c and 2 d. The HR mirror 12 and LR mirror 13 are attached to the signal feed-through fibers of pump couplers 2 a and 2 d, respectively.
The examples discussed above show that flexible and power scalable fiber lasers can be manufactured with low-loss pump couplers. The present invention describes a concept of a low-loss pump coupler and a method of manufacturing such pump couplers.
FIG. 5 a shows one embodiment of the pump coupler 2. The coupler 2 can comprise a number of pump fibers 31 arranged so that their optical axes are essentially parallel and their cleaved or polished ends lie essentially on the same plane, which is perpendicular to the optical axis 22 of the coupler 2. Note that only two pump fibers 31 are drawn in this cross-section, but it should be understood that the number of pump fibers can be larger, e.g. four or six. Typically, no pump fiber is located at the center of the pump fibers. The pump fibers 31 are then spliced to the cleaved or polished end of a tapered capillary tube 40 having the initial outer diameter of D₁and inner diameter of D₂. In this embodiment the capillary taper 40 is formed by the well-known methods of glass drawing. Thus, both the outer and inner diameters of the capillary taper 40 change along the taper, but their ratio remains essentially constant. For low optical losses for the pump light in the coupler 2, the wall thickness W_cof the capillary tube at the entrance end for the pump light is preferably equal to or larger than the diameter D₅of the pump fibers. This ensures that all of the pump light from the pump fibers can be coupled to the glass portion of the capillary tube 40. The capillary taper 40 is preferably adiabatic, meaning that the lateral dimensions of the tube change slowly along its length so that the brightness of light traveling along the tapered capillary is essentially constant. Brightness here means the product of the wall thickness of the capillary and the numerical aperture (NA) of the light at any longitudinal location inside the taper. The capillary 40 has a wide first end 65 with an outer diameter D₁and inner diameter D₂and a narrow second end 70 with outer diameter D₃and inner diameter D₄. At the center of the pump fibers and inside the central hole of the capillary taper 40 a signal feed-through fiber 32 is located. The diameter D₆of the signal feed-through fiber 32 is slightly smaller than that of the inner hole D₄of the tapered capillary 40. It should be clear that this restriction does not have to apply to the whole length of the signal feed-through fiber 32, but only to the portion that is fixed into the waist region of the capillary taper 40. The capillary tube 40 is collapsed onto the signal feed-through fiber 32 within region 45 of length L_c, thus making the capillary 40 and the signal feed-through fiber 32 to merge to form solid glass in the said region 45. The collapsed region 45 facilitates making a high quality cleave to the end of the taper. Cleaving of the taper is done with any of the methods used in fiber cleaving. The said cleaved end 70 of the taper 40 is spliced to an output signal fiber 50, preferably a double-clad fiber, so that the core 33 of the signal fiber 32 is essentially aligned with the core 53 of the output signal fiber 50. The core diameters and numerical apertures of the fibers 32 and 50 are preferably chosen to be essentially the same. This ensures that the laser radiation or signal can pass through the coupler 2 with minimal loss of power and beam quality. For good pump light transmission through the coupler 2, the waist diameter D₃of the capillary taper 40 is chosen to be essentially equal to or smaller than the diameter D₇of the output signal fiber 50.
FIG. 5 b shows a cross-section along the direction A of FIG. 5 a showing totally eight pump fibers 31 around the signal fiber 32. The number of pump fibers 31 is typically from 6 to 8.
FIG. 9 shows another embodiment of the pump coupler 2 according to this invention. In this embodiment the capillary taper 40 is formed by chemically etching the outer surface of the capillary tube 40. Thus, only the outer diameter changes along the capillary taper 40, and D₄=D₂. Other features in this embodiment are essentially similar to that of FIG. 5 a.
The numerical aperture (NA) of a fiber is equal to, in a first approximation, the maximum angle the cone of radiation makes with the fiber axis when it exits the fiber into air. As a person skilled in the art can easily understand from the above description, the numerical aperture NA₁of the pump light that is entering the capillary taper 40 from the pump fibers 31 will be increased, to a first approximation, by the capillary taper 40 to the value NA₂according to the formula NA₂=NA₁*D₁/D₃. Thus, the coupler 2 should be designed so that NA₂does not exceed the maximum numerical aperture NA₃of the pump waveguide of the output signal fiber 50. For a double clad output signal fiber the value for NA₃is typically about 0.46, which is achieved with a low-index polymer coating. Hence, by observing the design rule NA₂≦NA₃a coupler with good transmission from the pump fibers 31 into the output signal fiber 50 can be realized. This is the first task of the coupler 2. The second task is to transmit the laser radiation traveling inside the core of the signal feed-through fiber 32 and output signal fiber 50 through the coupler with minimal losses and degradation in the beam quality. This is achieved preferably by choosing the fibers 32 and 50 so that their core diameters and numerical apertures are essentially the same.
In accordance with FIG. 6 the first method in accordance with the invention begins with aligning the pump fibers 31 with the signal fiber 32. As can be seen from FIG. 7, the cleaved ends of the pump fibers 31 are aligned to end at the same level.
The waist to the capillary tube is formed by etching such that only the outer diameter of the capillary tube 40 is reduced and the inner diameter of the capillary remains the same.
This structure is further connected in accordance with FIG. 8 to the capillary tube 40 e.g. by splicing. The area 45 of the capillary tube 40 is then collapsed onto the signal fiber 32 from the waist.
In accordance with FIG. 9 the capillary tube 40 is cleaved from the collapsed portion 45 and another double clad output signal fiber 50 is spliced to the cleaved capillary tube 40 so that cores of signal fibers are aligned.
A second method in accordance with the invention is described in connection with FIGS. 10-12. In this solution both the inner diameter and the outer diameter of the capillary tube 40 are reduced at the taper.
In accordance with FIG. 10 pump fibers 31 are formed around an aid fiber 60, the diameter of which is about the same as the inner diameter of the capillary tube 40. The aid fiber 60 does not extend as far as the pump fibers 31. The pump fibers 31 are spliced to the capillary tube 40 and the aid fiber 60 is removed and replaced by a signal feed-through fiber 32 typically with a smaller diameter than the aid fiber 60, at least at the portion that is pushed through the waist of the capillary tube 40. Aid fiber 60 may be also some other structure than fiber, e.g. a metallic wire. Therefore a term aid tool can also used in this connection. In a first implementation of fitting the signal feed-through fiber 32 to the capillary tube 40, the outer surface of the signal feed-through fiber 32 is etched chemically so that it just goes through the inner hole of diameter D₄of the capillary tube 40. In another implementation of fitting the signal feed-through fiber 32 to the capillary tube 40, the fiber 32 is designed to have its original diameter slightly smaller than D₄.
As shown in FIG. 11 the capillary tube 40 is collapsed from the taper waist 45 onto the signal feed-through fiber 32.
In accordance with FIG. 12 the capillary tube is cleaved from the collapsed waist 45 portion and double clad output signal fiber 50 is spliced to the cleaved capillary tube 40.

Claims

1-8. (canceled)

9. An optical coupler, said optical coupler being usable with a first optical fibre and a second optical fibre, said second optical fibre defining a second fibre coupling section and a second fibre transmitting section extending from said second fibre coupling section, said second fibre coupling section defining a radially outwardmost peripheral surface, said radially outwardmost peripheral surface defining a peripheral surface coupling portion, said optical coupler comprising:

a coupler first end section and a substantially opposed coupler second end section, said coupler first end section defining a first coupling surface;

said optical coupler defining a second coupling surface extending along said coupler first and second end sections;

said first coupling surface being optically couplable with said first optical fibre and said second coupling surface being positionable so as to extend substantially parallel to said peripheral surface coupling portion and to be optically coupled with said peripheral surface coupling portion;

wherein said optical coupler has optical and geometrical properties such that substantially all the light guided to said first coupling surface by said first optical fibre is directed towards said second coupling surface and into said second optical fibre through said peripheral surface coupling portion so as to be guided into said second fibre coupling section for transmission into said second fibre transmitting portion.

10. An optical coupler as defined in claim 9, wherein said optical coupler includes a tapered section tapering in a direction leading from said coupler first end section towards said coupler second end section, said tapered section being located substantially distally relatively to said coupler first end section.

11. An optical coupler as defined in claim 10, wherein said second optical fibre includes a second fibre core and a second fibre cladding extending substantially radially outwardly from said second fibre core, said second optical fibre being positionable such that said second coupling surface and said second fibre core are substantially parallel to each other.

12. An optical coupler as defined in claim 10, wherein said second coupling surface is substantially cylindrical

13. An optical coupler as defined in claim 12, wherein said optical coupler defines a coupler passageway extending along said coupler first and second end sections, said second coupling surface being located substantially peripherally relatively to said coupler passageway.

14. An optical coupler as defined in claim 13, wherein

said coupler first end section is substantially cylindrical and extends longitudinally substantially parallel to said second coupling surface;

said coupler second end section is substantially frusto-conical and tapers in a direction leading away from said coupler first end section.

15. An optical coupler as defined in claim 14, wherein said coupler passageway is radially substantially centrally located relatively to said coupler first end section.

16. An optical coupler as defined in claim 13, wherein said coupler passageway has a first diameter substantially adjacent said coupler first end section and said coupler passageway has a second diameter substantially adjacent said coupler second end section, said second diameter being substantially smaller than said first diameter.

17. An optical coupler as defined in claim 10, wherein said second coupling surface and said peripheral surface coupling portion are fused to each other.

18. An optical coupler as defined in claim 9, wherein said first coupling surface extends substantially perpendicularly to said second coupling surface.

19. An optical coupler as defined in claim 9, wherein said second coupling surface extends substantially parallel to said peripheral surface coupling portion.

20. A method for assembling an optical coupling assembly for optically coupling a first and a second optical fibre using an optical coupler, said second optical fibre defining a second fibre coupling section and a second fibre transmitting section extending from said second fibre coupling section, said second fibre coupling section defining a radially outwardmost peripheral surface, said radially outwardmost peripheral surface defining a peripheral surface coupling portion, said optical coupler including a coupler first end section and a substantially opposed coupler second end section, said coupler first end section defining a first coupling surface, said optical fibre defining a second coupling surface extending along said coupler first and second end sections, said method comprising:

positioning said first optical fibre substantially adjacent to said first coupling surface;

optically coupling said first optical fibre and said first coupling surface to each other;

positioning said second optical fibre such that said second coupling surface is substantially adjacent and substantially parallel to said peripheral surface coupling portion;

optically coupling said second coupling surface and said peripheral surface coupling portion to each other.

21. A method as defined in claim 20, wherein optically coupling said first optical fibre and said first coupling surface to each other is performed before optically coupling said second coupling surface and said peripheral surface coupling portion to each other.