The present invention relates to the field of optical fibers and more particularly concerns a microstructured optical fiber having holes arranged in an Archimedean-like lattice surrounding a light-guiding core.
Optical fibers are used in a variety of applications such as telecommunications, illumination, fiber lasers, laser machining and welding, sensors, medical diagnostics and surgery.
A typical standard optical fiber is made of transparent material. It is uniform along its length, and has a cross-section of varying refractive index. For example, the transparent material in the central region, i.e. the core, may have a higher refractive index than the transparent material in the outer region, i.e. the cladding. Light is confined in or near the core and guided along the length of the optical fiber by the principle of total internal reflection at the interface between the core and cladding.
A microstructured optical fiber (MOF), also known as a holey fiber, a photonic crystal fiber or a photonic bandgap fiber, differs from a standard waveguide fiber in that it has a cross-section microstructured from two or more materials. A microstructured fiber has a cladding running the length of the fiber that is microstructured from two or more materials most commonly arranged periodically over much of the cross-section. For example, a microstructured optical fiber may have a cladding made of a transparent material in which a periodic array of holes extends longitudinally, the holes being arranged periodically over much of the cladding cross-section and filled with material which has a lower refractive index than the transparent material of the rest of the cladding, and a core of transparent material consisting of a break in the periodic array of the cladding. MOFs can guide light according to one of two mechanisms. In a microstructured optical fiber with a solid core, or a core with a higher average refractive index than the microstructured cladding, light may be guided along the core by the same index-guiding mechanism of total internal reflection as in standard optical fibers or by a mechanism based on photonic-band-gap effects. With total-internal-reflection guidance, MOFs can have a much higher effective-index contrast between core and cladding, and therefore can have much stronger confinement for specialized applications. With photonic-band-gap guidance, light is confined by a photonic bandgap created by the microstructured cladding. A properly designed bandgap can confine light in a hollow core or a core of lower refractive index than the cladding.
In general, an optical fiber may be multi-mode or single-mode. A multi-mode fiber allows for more than one mode of the light wave, each mode travelling at a different phase velocity, to be confined to the core and guided along the fiber. A single-mode fiber supports only one transverse spatial mode at a frequency of interest. Given a sufficiently small core or a sufficiently small numerical aperture, it is possible to confine a single mode, the fundamental mode, to the core. Single-mode fibers are preferred for many applications because the problem of intermodal dispersion encountered by multi-mode fibers is avoided, and the intensity distribution of the light wave emerging from the fiber is unchanged regardless of launch conditions and any disturbances of the fiber.
For some applications, it is advantageous to carry as much optical power as possible. However, if the light intensity within the fiber exceeds a certain threshold, the material from which the fiber is made will suffer irreversible damage. Increasing the diameter size of the core of the fiber reduces the intensity of the light for a given power and allows a greater power to be carried. Using a larger core fiber also helps to reduce the non-linear effects that appear at high power.
For example, in the field of high-power lasers and amplifiers, the onset of adverse non-linear effects can severely degrade the spectral content and limit the power output of the laser source. Using a single-mode large-mode-area active fiber as the amplifying medium is a relatively easy solution to the problem of non-linear effects which can be detrimental to the operation of the laser.
Most microstructured optical fibers that are reported in the prior art literature—for example, in U.S. Pat. No. 6,334,019 (Birks et al.), U.S. Pat. No. 6,603,912 (Birks et al.), and U.S. Pat. No. 6,888,992 (Russell et al.)—consist of a cladding which has embedded along its length a substantially periodic array of holes and a core defined by the absence of at least one hole in the array, essentially, a triangular lattice of holes surrounding a central defect constituted by the absence of at least one of the holes in the lattice structure. One particular implementation of this design is the case where a seven-missing-holes defect defining a core is surrounded by a triangular lattice of holes defining a microstructured cladding. This is for example reported in Limpert et al., “Low non-linearity single-transverse-mode ytterbium-doped photonic crystal fiber amplifier”, Opt. Express 12(7), 1313 (2004) and in J. Limpert et al., “High-power rod-type photonic crystal fiber laser”, Opt. Express 13(4), 1055 (2005)]. By using such designs, a single-transverse-mode large-mode-area fiber that allows the transportation of high optical power while minimizing the non-linearity can be devised. Core diameters of 45 μm or greater may be achieved with such designs. Such large-mode-area fiber designs are particularly important in the field of high power lasers, where the core of the fiber is doped with active ions permitting a laser effect. However one drawback of the proposed triangular lattice structure of the cladding for the microstructured optical fibers is the quality of the mode profile of the light beam, more particularly the non-circular form of the guided mode profile, which stems from a central core having a cross-section which is more hexagonal than circular. Such sub-optimal beam quality can be detrimental for applications, such as precision laser surgery or micromachining, where light beam quality, i.e. a circular mode profile, is critical.
There is therefore a need for a microstructured optical fiber that enhances the circularity of the profile of the guided light mode.
In accordance with one aspect of the present invention, there is provided a microstructured optical fiber which includes a light-guiding core and a primary cladding surrounding the core. The primary cladding has a plurality of holes arranged in hexagonal unit cells and defining an Archimedean-like lattice.
Preferably, the core is defined by a break in a center of the Archimedean-like lattice, the break being characterized by an absence of at least one of the unit cells.
Also preferably, the Archimedean-like lattice comprises at least one complete ring of the unit cells arranged around the core.
In one preferred embodiment of the microstructured optical fiber, each unit cell has seven holes arranged in a centred hexagon. Preferably, the Archimedean-like lattice includes at least one complete ring of unit cells arranged circumferentially around the core and may further optionally include at least one outer incomplete ring of unit cells.
In accordance with another aspect of the present invention, there is also provided a method for making a microstructured optical fiber which includes a step of fabricating a fiber preform, this fabricating including the sub-steps of:
The method preferably further includes a step of drawing the fiber preform into the desired microstructured optical fiber
Other features and advantages of the present invention will be better understood upon reading of preferred embodiments thereof with reference to the appended drawings.
The aspects of the present invention will be described more fully hereinafter with reference to the accompanying drawings
Microstructured Optical Fiber
In accordance with one aspect of the present invention, there is generally provided a microstructured optical fiber (20) which includes a primary cladding (24) surrounding a light-guiding core (22). The primary cladding (24) has a plurality of holes (26) arranged in hexagonal unit cells (28) and defining an Archimedean-like lattice. The light-guiding core (22) may be defined by a break in the center of the Archimedean-like lattice, the break being characterised by an absence of at least one of the unit cells. Preferably, the MOF (20) includes an overcladding which surrounds the primary cladding (24). The overcladding, in contrast to the primary cladding, often does not have a hole microstructure and may be made of any suitable material, for example substantially solid silica. In general, as with most fibers, the MOF may also have a protective outer coating, for example a coating of acrylate.
An Archimedean two-dimensional (2-D) lattice or tiling is an isogonal edge-to-edge plane tiling by regular polygons, in which every vertex and edge of a tile is a vertex and edge of the tiling. In the case where all of the vertices do not have the same immediate environment, for example in the case of central vertices of the lattice which do not have the same environment as the other vertices, the lattice is best referred to as Archimedean-like or semi-regular. Archimedean-like lattices, or tilings, have periodic structures similar to conventional 2-D photonic crystals, but they possess a higher order of local rotational symmetry than the traditional Bravais lattice—the Bravais lattices having the highest order of rotational symmetry (6) are the triangular and honeycomb lattices [see David et al., “Isotropic Photonic structured: Archimedean-like tilings and quasi-crystals,” IEEE J. Quantum Electron. 37, 1427 (2001)]. The periodic structure of Archimedean and Archimedean-like lattices/tilings can mimic some properties of quasi-crystalline structures. Quasi-crystalline structures are so-named because the pattern of defects is only quasi-periodic, locally the defects are arranged in a fixed regular pattern but this pattern is not periodic globally throughout the entire structure.
In general, a lattice may be described in terms of its unit cell, the simplest repeating unit which when tiled in 2-D or 3-D space yields the lattice. Each unit cell is defined in terms of its lattice points.
The light-guiding core (22) of the MOF (20) may be substantially solid across its entire cross-section. Even if the core (22) is substantially solid, it may have holes (27) along its circumferential perimeter as shown in
The primary cladding (24) of the MOF (20) surrounding the core (22) comprises a substantially transparent material in which a number of holes (26) extends longitudinally. As mentioned above, the holes (26) are arranged in hexagonal unit cells (28) and define an Archimedean-like lattice over much of the cross-section of the primary cladding (24). Although the holes (26) are preferably substantially circular in shape and of practically the same diameter, each hole (26) need not be perfectly circular nor have the exact same diameter as the other holes (26). Preferably, the Archimedean-like lattice has at least one complete ring (30) of the unit cells (28) arranged circumferentially around the core, as shown in
The transparent material of the primary cladding (24) may consist of a doped or undoped polymer (e.g. polymethylmethacrylate (PMMA), etc.) or glass (e.g. silica, chalcogenide glass, soft glass, etc.). It may be different or the same as that of the core (22). The holes (26) may be empty (vacuum) or filled with a transparent material that has a refractive index which is different from the refractive index of the material of the primary cladding (24). Moreover, all of the holes (26) of the unit cell need not be filled with the same material; some of the holes (26) may be filled with one material while others are filled with a different material. The hole material may be a solid (e.g. a glass such as silica, polymer, etc.), liquid (e.g. water, dye solution, etc.) or gas (e.g. air, nitrogen, hydrogen, etc). In the case of a MOF with total-internal-reflection guidance, the holes may be filled with air, the primary cladding material may be silica, and the core material may also be silica, as shown in
Referring to
The novel cladding structure proposed here created using A7 unit cells is particularly well suited for a seven-missing-holes fiber design as the cladding structure is composed of hexagonal unit cells (28) comprising seven (7) holes (26) (
As it can be seen in
where MFD refers to the Mode Field Diameter, defined as the root-mean-square (rms) width of the fundamental guided mode. A value of C=3% was obtained for the guided mode of the AL-MOF shown in
To demonstrate further the improvement in the quality of the guided mode profile, the far-field profiles of the modes are presented in
A passive AL-MOF made of a single bulk material in which the primary cladding consists of a plurality of low-index regions disposed in an Archimedean-like lattice defined by type A7 unit cells could be fabricated to have a large-mode-area (core diameter larger than 15 μm, ideally more than 25 μm) and be singlemode by a careful adjustment of the hole diameter. In that case, the fiber could be suitable for high power delivery.
Alternatively, the dimensions of the guiding structure of an AL-MOF could be scaled down, which would reduce the effective area of the guided mode as well as reduce the zero-dispersion wavelength (ZDW) of the fiber below the material ZDW, which would make the fiber “highly nonlinear” around the ZDW and suitable for different nonlinear processes such as supercontinuum generation.
Quite possibly the most important application targeted by the AL-MOF design is the high-power fiber laser. As mentioned previously, using the AL-MOF design in a large mode area configuration can lead to a much better beam quality, especially in terms of beam circularity, as compared to a similar conventional TL-MOF. By adding active dopants in the core of an AL-MOF, it could be possible to take advantage of the improved beam quality offered by the AL-MOF in order to fabricate high-power fiber lasers or amplifiers as well as rod-type lasers or amplifiers.
In the case of such active fibers, it is often desirable to have a double-clad fiber design where this secondary cladding could be made of a low-index polymer or an air-cladding surrounding the Archimedean-like-lattice primary cladding. That way, the double-clad AL-MOF would have a profile similar to a double-clad conventional MOF, except that the inner microstructured cladding would form an Archimedean-like lattice.
Another possible application of the Archimedean-like lattice cladding structure would be to use it instead of a triangular lattice to form an air-guiding photonic bandgap fiber. In that particular case, the solid central core is removed and guidance is ensured by the creation of a photonic bandgap that prevents light from escaping the core. The design of the conventional “state-of-the-art” hollow-core photonic bandgap fiber consists of a TL microstructured cladding, while the AL microstructured cladding could also be used to form the cladding disposed around the central hollow core.
Method for Manufacturing a Microstructured Optical Fiber
In accordance with another aspect of the present invention, there is provided a method for making a microstructured optical fiber which includes the following steps.
(I) Fabricating a Fiber Preform
A microstructured optical fiber may be made by using a stack and draw process. The method of making the microstructured optical fiber is simplified by first fabricating a fiber preform. Fabricating the fiber preform preferably includes the following steps.
To define the light-guiding core of the microstructured optical fiber, a rod made of a transparent material—e.g. a polymer or glassy material such as silica—which may or may not be doped is provided. The core rod may have a uniform or varying refractive index. It may be solid across its entire cross-section or it may have holes along its circumferential perimeter, consistent with the circularized core of a microstructured optical fiber, as shown in
Preferably and advantageously, the rod has a cross-section profile which is substantially circular or hexagonal, but of course may have any appropriate cross-section profile conducive to the fabrication of the fiber perform.
The fabrication of the fiber preform next includes fabricating a plurality of canes, each of the plurality of canes having a substantially hexagonal cross-section and being provided with a number of holes arranged in a unit cell defining an Archimedean-like lattice. These canes are used to define the primary cladding surrounding the core of the microstructured optical fiber. A schematic representation of a length of one such cane (34) is given in
One technique for fabricating the plurality of canes includes the following steps:
Another technique for fabricating the plurality of canes, which foregoes the need for drilling and milling, includes the following steps:
In a preferred embodiment of the MOF, each of the canes (34) used to fabricate the fiber preform has seven holes (26) arranged in a centred hexagon, as shown in
It is obvious from the above description that the meaning of the term “holes” is not limited to regions of absence—the term “holes” being used to denote specific regions having different optical properties than the surrounding material.
(c) Stacking the Plurality of Canes Concentrically Around the Rod
Once the required number of canes has been fabricated, the next step is to stack the canes concentrically around the rod defining the light-guiding core. Preferably, at least one ring of canes is stacked around the core rod. Additional rings of canes may be stacked, in which case one or more of the outermost rings need not be complete. Advantageously, the hexagonal elongated shape of the canes lends itself to the stacking. The rod forming the core of the structure need not be hexagonal, although a rod of similar hexagonal cross-section dimensions as the canes would facilitate the stacking of the canes and fabrication of the preform. The actual stacking may be done manually or through some automated process which may be computer-guided. For ease of stacking, a ring, tie or other holding means may be used to temporarily bundle the tubes.
Following the step of stacking, it may be preferable to include an additional step of overcladding the fiber preform (41), as shown in
Depending on the desired dimensions of the resulting MOF, the fiber preform (41) may either be directly drawn into a fiber (20) having the desired dimensions (
As mentioned earlier, according to one embodiment of the invention, the rod provided to define the core may have a number of holes arranged in a unit cell of an Archimedean-like lattice (e.g. the rod may be just another one of the canes constituting the primary cladding). Some or all of the holes within the core rod may be made to collapse during the drawing process to thereby form a substantially solid core in the resulting MOF by ensuring that the holes of the core rod have a sufficiently lower internal pressure than the holes of the surrounding canes. An example of an Archimedean-like lattice microstructured optical fiber (20) with a solid core (22) is shown in
The method of making a MOF may further include a step after the drawing process of evacuating the holes or filling the holes with a material of different refractive index than the primary cladding. The holes may be filled with a fluid such as a gas (e.g. air, hydrogen, etc.) or a liquid (water, solutions of dyes, etc.) or with a solid material (e.g. a polymer, a glass, etc.). The filling of the holes with a fluid may be accomplished using a number of methods: capillary action, suction, a pump, injection with a syringe, etc. The filling of the holes with a solid material may basically be carried out in the same manner as the filling of the holes in the primary cladding canes.
Numerous modifications could be made to any of the embodiments described above without departing from the scope of the present invention as defined in the appended claims.
Number | Name | Date | Kind |
---|---|---|---|
4815079 | Snitzer et al. | Mar 1989 | A |
5332681 | Tonucci et al. | Jul 1994 | A |
5526449 | Meade et al. | Jun 1996 | A |
5802236 | DiGiovanni et al. | Sep 1998 | A |
5907652 | DiGiovanni et al. | May 1999 | A |
6097870 | Ranka et al. | Aug 2000 | A |
6243522 | Allan et al. | Jun 2001 | B1 |
6301420 | Greenaway et al. | Oct 2001 | B1 |
6334019 | Birks et al. | Dec 2001 | B1 |
6404966 | Kawanishi et al. | Jun 2002 | B1 |
6418258 | Wang | Jul 2002 | B1 |
6539155 | Broeng et al. | Mar 2003 | B1 |
6574383 | Erchak et al. | Jun 2003 | B1 |
6603912 | Birks et al. | Aug 2003 | B2 |
6608955 | Fukuda et al. | Aug 2003 | B2 |
6788865 | Kawanishi et al. | Sep 2004 | B2 |
6845204 | Broeng et al. | Jan 2005 | B1 |
6847771 | Fajardo et al. | Jan 2005 | B2 |
6888992 | Russel et al. | May 2005 | B2 |
7228041 | Kim et al. | Jun 2007 | B2 |
7348603 | Erchak et al. | Mar 2008 | B2 |
7359603 | Large et al. | Apr 2008 | B2 |
20010026667 | Kawanishi et al. | Oct 2001 | A1 |
20010029756 | Paek et al. | Oct 2001 | A1 |
20020122644 | Birks et al. | Sep 2002 | A1 |
20020126370 | Broderick et al. | Sep 2002 | A1 |
20020131741 | Bayart et al. | Sep 2002 | A1 |
20020131742 | Bayart et al. | Sep 2002 | A1 |
20020181911 | Wadsworth et al. | Dec 2002 | A1 |
20030059185 | Russell et al. | Mar 2003 | A1 |
20030136154 | Tajima et al. | Jul 2003 | A1 |
20030180018 | Hasegawa | Sep 2003 | A1 |
20040091224 | Baumberg et al. | May 2004 | A1 |
20040096173 | Fekety et al. | May 2004 | A1 |
20040105640 | Hasegawa | Jun 2004 | A1 |
20040105641 | Russell et al. | Jun 2004 | A1 |
20040151450 | Wadsworth et al. | Aug 2004 | A1 |
20040158381 | Strelioff et al. | Aug 2004 | A1 |
20040175084 | Broeng et al. | Sep 2004 | A1 |
20040222480 | Weisbuch et al. | Nov 2004 | A1 |
20040258381 | Borrelli et al. | Dec 2004 | A1 |
20050034484 | Large et al. | Feb 2005 | A1 |
20050147366 | Large et al. | Jul 2005 | A1 |
20050180710 | Oh et al. | Aug 2005 | A1 |
20050276556 | Williams et al. | Dec 2005 | A1 |
20050286847 | Arimondi et al. | Dec 2005 | A1 |
20060204865 | Erchak et al. | Sep 2006 | A1 |
20080112678 | Kim et al. | May 2008 | A1 |
20090212265 | Steinhardt et al. | Aug 2009 | A1 |
Number | Date | Country |
---|---|---|
2002277666 | Sep 2002 | JP |
2003227941 | Aug 2003 | JP |
WO 2004019092 | Mar 2004 | WO |
WO 2004019092 | Mar 2004 | WO |
WO 2004057394 | Jul 2004 | WO |
Entry |
---|
Proulx et al., “Design, fabrication, and characterization of holey fibers,” 2003. Proc. SPIE 4833, pp. 696-704. |
Bourliaguet et al., “Microstructured fiber splicing,” 2003. Opt. Express 11, pp. 3412-3417. |
Proulx et al., “Low-loss splicing of microstructured fibers with conventional electric-arc splicers,” 2004. Proc. SPIE 5577, 519-526. |
Wang, Yiquan, “Coupled-resonator optical waveguides in photonic crystals with Archimedean-like tilings,” Europhys. Lett., 74 (2), pp. 261{267 (2006). |
David et al. “Wide angularly isotropic photonic bandgaps obtained from two-dimensional photonic crystals with Archimedean-like tilings;” Optics Letters, vol. 25, Iss. 14, pp. 1001-1003 (2000). |
Rattier et al. “Omnidirectional and compact guided light extraction from Archimedean photonic lattices”, Appl. Phys. Lett. 83 1283-5 (2003). |
Wang, Yiquan, “Coupled-resonator optical waveguides in photonic crystals with Archimedean-like tilings,” Europhys. Lett., 74(2), pp. 261{267 (2006). |
Fini et al. “High-Efficiency Nitride-Based Solid-State Lighting” Final Technical Progress Report, for Award Period Oct. 1, 2001-Apr. 30, 2005, DoE Award #DE-FC26-01NT41203, High-Efficiency Nitride-Based Solid-State Lighting, pp. 42-43. |
David et al. “Isotropic Photonic Structures: Archimedean-Like Tilings and Quasi-Crystals,” IEEE Journal of Quantum Electronics, vol. 37, No. 11, Nov. 2001, pp. 1427-1434. |
M. Rattier, H. Benisty, E. Schwoob, C. Weisbuch, T. F. Krauss, C. J. M. Smithd, R. Houdre and U. Oesterle “Omnidirectional and compact guided light extraction from Archimedean photonic lattices” Applied Physics Letters—vol. 83, No. 7, Aug. 18, 2003, pp. 1283-1285. |
Aurélien David, Tetsuo Fujii, Elison Matioli, Rajat Sharma, Shuji Nakamura, Steven P. Denbaars, Claude Weisbuchc and Henri Benisty “GaN light-emitting diodes with Archimedean lattice photonic crystals” Applied Physics Letters 88, 073510 (2006). |
J. Limpert, A. Liem, M. Reich, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermannj. Broeng, A. Petersson and C. Jakobsen “Low-nonlinearity single-transverse-mode ytterbium-doped photonic crystal fiber amplifier” Optics Express 1313—vol. 12, No. 7, Apr. 5, 2004, pp. 1313-1319. |
J. Limpert, N. Deguil-Robin, I. Manek-Hönninger, F. Salin, F. Röser, A. Liem, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermann, J. Broeng, A. Petersson and C. Jakobsen “High-power rod-type photonic crystal fiber laser” Optics Express 1055—vol. 13, No. 4, Feb. 21, 2005, pp. 1055-1058. |
D. Mogilevtsev, T. A. Birks, and P. St. J. Russell “Group-velocity dispersion in photonic crystal fibers” Optics Letters 1663—vol. 23, No. 21, Nov. 1, 1998, pp. 1662-1664. |
Jung-Sheng Chiang and Tzong-Lin Wu “Analysis of propagation characteristics for an octagonal photonic crystal fiber (O-PCF)” Optics Communications 258 (2006) 170-176. |
P. Glas, D. Fischer. G. Steinmeyer, A. Husakou, J. Herrmann, R. Iliew, N.B. Skibina, V.I. Beloglasov, Y.S. Skibina “Supercontinuum generation in a two-dimensional photonic kagome crystal” Applied Physics B 81—Lasers and Optics, 209-217 (2005). |
F. Luan, A. K. George, T. D. Hedley, G. J. Pearce, D. M. Bird, J. C. Knight, and P. St. J. Russell “All-solid photonic bandgap fiber” Optics Letters—vol. 29, No. 20, Oct. 15, 2004, pp. 2369-2371. |
F. Couny, F. Benabid, and P. S. Light “Large-pitch kagome-structured hollow-core photonic crystal fiber” Optics Letters 3574—vol. 31, No. 24, Dec. 15, 2006, pp. 3574-3576. |
David et al., Isotropic Photonic Structures: Archimedean-Like Tilings and Quasi-Crystals, IBEE Journal of Quantum Electronics, vol. 37, No. 11, Nov. 2001. |
Number | Date | Country | |
---|---|---|---|
20080199135 A1 | Aug 2008 | US |