Patent Application
20100232745
This invention concerns improvements relating to waveguides. More particularly, the invention relates to waveguides terminated so as to be suitable for connection to other waveguides, or for coupling radiation into or out of the waveguide. The invention also relates to a method of terminating a waveguide, to a connector for a waveguide, and to a method of attaching a connector to a waveguide. The invention is particularly concerned with photonic crystal fibre waveguides.
Photonic crystal fibres are optical fibres that have a core surrounded by a cladding region in which there is an array of holes that run along the length of the fibre. The core region typically has a diameter of ranging from 2 μm upwards, and the cladding region typically comprises holes having a diameter in the range from sub-micron to several microns. The overall diameter of the fibre depends on, for example, the core diameter and guiding properties, but typically may extend up to hundreds of microns. Typically, the holes are arranged to have a periodic structure when viewed in cross-section through the fibre. Such fibres can also be described in the art as “holey fibres” or “microstructured fibres”.
In one type of photonic crystal fibre, known as ‘holey fibre’, guidance occurs as a result of the contrast between the core refractive index and the effective refractive index in the ‘holey’ material surrounding the core region. Light is thus guided along the fibre by refraction, as is the case in more standard optical fibres. In other photonic crystal fibres, the core is either of lower refractive index than the cladding, or is hollow. In these fibres, guidance occurs as a result of photonic bandgap effects arising from the periodicity of the hole structure. In both these types of photonic crystal fibre, the holes are key to the light-guiding properties of the fibre.
Photonic crystal fibres have been found to exhibit a number of advantageous properties in comparison to standard optical fibres, such as are disclosed by J. C. Knight, T. A. Birks, P. St. J. Russell, and D. M. Atkins in the paper “All-silica single-mode fiber with photonic crystal cladding”, published in volume 21, Optics Letters, pages 1547-1549 (1996) and followed by the publication of an erratum in volume 22, Optics Letters, pages 484-485 (1997); and by T. A. Birks, J. C. Knight and P. St. J. Russell in the paper “Endlessly single-mode photonic crystal fibre”, published in volume 22, Optics Letters, pages 961-963 (1997).
In order to make use of the advantageous properties of photonic crystal fibres, it is necessary to couple light into and out of such fibres. At an end-facet of a length of photonic crystal fibre, the holes that are necessary for guiding light along the core of the fibre are exposed to the ambient atmosphere. Ingress of moisture and debris can therefore occur. However, the presence of moisture and debris in the holes can alter the guiding properties of the photonic crystal fibre. For example, the refractive index of the holes may be altered, or they may become blocked with opaque material. In either event, the guiding properties of the photonic crystal fibre are adversely affected. Such problems are particularly severe where it is desired to attach a photonic crystal fibre to a connector, so that the fibre can be connected and disconnected at will. In these circumstances, the end-facet of the photonic crystal fibre is exposed to the atmosphere for some time, and the risk of the holes becoming fouled is unacceptably large.
There are currently two known methods in which the above problems can be overcome. Either a short length of solid, coreless fibre is spliced directly onto the end of the photonic crystal fibre, or the end of the fibre is heated to a temperature near its melting point, causing the holes to collapse in the region near the end-facet of the photonic crystal fibre. In both cases, holes are not present in the region near the end of the resulting structure, as is illustrated schematically in
It is therefore an aim of the present invention to overcome, or at least partially mitigate, the above-identified problems. It is a further aim of the invention to provide a method of terminating a photonic crystal fibre that allows light to be efficiently coupled into photonic crystal fibres, and that enables such fibres to be butt-coupled without incurring such significant losses as are incurred using currently known techniques. It is a yet further aim of the invention to provide connectors suitable for photonic crystal fibres.
In accordance with a first aspect of the invention, there is provided a waveguide comprising photonic crystal fibre terminated by a re-imaging device. The output of the re-imaging device is light intensity distribution that comprises an image of a light intensity distribution input into the re-imaging device. Therefore, where light is transmitted through a waveguide in accordance with the first aspect of the present invention, exiting through the re-imaging device that terminates the photonic crystal fibre, there is less divergence than would occur should the photonic crystal fibre be terminated by a non-guiding region in which the holes were sealed. Thus such waveguides can be butt-coupled more efficiently than has previously been possible using the above-described prior known techniques. Moreover, since the end-facet of the terminated waveguide is formed by the re-imaging device, moisture and other debris is prevented from entering the holes of the photonic crystal fibre, and the guiding properties of the photonic crystal fibre are preserved.
Optionally, the re-imaging device is a multimode transmission device. Multimode transmission devices are able to support the transmission of light in a plurality of spatial modes. Interference between the individual spatial modes can cause re-imaging of the input to the device.
Conveniently, the multimode transmission device may be a length of multimode fibre. Multimode fibre is readily commercially available in a number of standard sizes, so that waveguides according to the present invention can be used in combination with standard connectors. Advantageously, therefore, the present invention enables photonic crystal fibres to be used with standard connectors more efficiently than has previously been possible. For example, the terminated end of the waveguide may be housed within a ferrule, which ferrule is housed within a connector body. The ferrule may be positioned such that the terminated end of the waveguide is flush with one end of the ferrule. This facilitates butt coupling of the waveguides. The ferrule may be positioned such that the join between the photonic crystal fibre and the re-imaging device is housed within the ferrule. Such an arrangement advantageously strengthens the join between the photonic crystal fibre and the re-imaging device. Optionally, the ferrule is made of a material selected from the group consisting of ceramic, metallic, and zirconate materials.
The multimode fibre may be spliced onto the photonic crystal fibre. Preferably, the length of the multimode fibre is selected such that, in use of the waveguide to guide light of a predetermined wavelength, a first light intensity distribution at a first end of the multimode waveguide comprises an image of a second light intensity distribution at the other end of the multimode waveguide. The multimode transmission device may alternatively comprise any device able to guide a number of spatial modes of light and support multimode interference such that a multimode interference image can be formed. For example, rectangular or cubic devices, that are transparent at the operational wavelength of the waveguide, can be configured, by selection of appropriate dimensions, to support a number of spatial modes and exhibit the re-imaging property, and may also therefore be used as multimode transmission devices.
The output of the re-imaging device may be a one-to-one image of the input to the re-imaging device. Alternatively the output of the re-imaging device is a multiple image of the input to the re-imaging device. Thus the waveguide may be used either in combination with standard connectors, where a one-to-one image is formed, or, where a multiple image is formed, the waveguide can be used as an optical splitter.
The invention extends to a connector for a waveguide as described above, the connector comprising a connector body, and a ferrule configured to fit within the connector body and to accommodate both the re-imaging device and at least a part of the photonic crystal fibre.
According to a second aspect of the present invention, there is provided a pair of waveguides, each waveguide of the pair of waveguides being terminated by a multimode transmission device, the dimensions of the multimode transmission devices being complimentary such that, when the pair of waveguides are connected together, the input to one of the pair of waveguides is a one-to-one re-image of the output of the other of the pair of waveguides, and such that, at the interface between the waveguides, a multiple image of the output of said one of the waveguides is formed. Optionally, the waveguides each comprise photonic crystal fibre. It is expected that such pairs will find application where it is necessary to connect together waveguides used for transmitting high intensity light, since a reduced intensity is obtained at the interface between the two waveguides. Such a reduced intensity is expected to result in a reduction in the risk of damage to the interface caused by imperfections in the optical quality of the interface.
According to a third aspect of the invention, there is provided a waveguide comprising a photonic crystal fibre terminated by a multimode transmission device, wherein the multimode transmission device is configured such that, in use of the waveguide to guide light of a predetermined wavelength, a first light intensity distribution at a first end of the multimode transmission device comprises an image of a second light intensity distribution at an opposing end of the multimode transmission device.
According to a fourth aspect of the present invention, there is provided a method of terminating a photonic crystal fibre comprising the step of attaching a multimode transmission device to a first end of the photonic crystal fibre. The multimode transmission device may be configured such that, in use of the terminated photonic crystal fibre to guide light of a predetermined wavelength, a first light intensity distribution at the output of the multimode transmission device comprises an image of a second light distribution at the first end of the photonic crystal fibre. The first light intensity distribution may be a one-to-one image of the second light intensity distribution. Alternatively, the first light intensity distribution may be a multiple image of the second light intensity distribution.
According to a fifth aspect of the present invention, there is provided a method of attaching a connector to a photonic crystal fibre, the method comprising the steps of:
The step (ii) may further comprise locating the ferrule such that a portion of the multimode fibre projects beyond the output end of the ferrule, and wherein the method further comprises the step of removing the portion of multimode fibre projecting beyond the output end of the ferrule such that the output end of the multimode fibre is flush with the output end of the ferrule. The predetermined length may be selected such that, in use of the photonic crystal fibre to guide light of a predetermined wavelength, a first light intensity distribution at the output end of the terminated photonic crystal fibre comprises an image of the light intensity distribution at the spliced end of the multimode fibre.
The above and further features of the invention are set forth with particularity in the appended claims and will be described hereinafter with reference to various exemplary embodiments and to the accompanying drawings in which:
a to 3c illustrate a method of attaching a connector to a photonic crystal fibre in accordance with a further embodiment of the invention; and
The various embodiments to be described below each make use of a re-imaging property of multimode waveguide. Multimode waveguide, as opposed to single mode waveguide, is able to guide a number of different spatial modes. The re-imaging property results from multimode interference, and causes single and multiple images of the input to a multimode waveguide to appear at periodic intervals along the waveguide. The phenomenon is known, for example, from the paper “Optical Multi-Mode Interference Devices Based on Self-Imaging: Principles and Applications” by L. B. Soldano and E. C. M. Pennings, published in Journal of Lightwave Technology, Volume 13 pages 615-627 (1995). Each mode carried by such a waveguide will propagate with a different propagation constant, resulting in phase differences building up between the different modes. The re-imaging property can be analysed in terms of the variation of the propagation constant with mode number. More particularly, it can be shown that length LN of the multimode waveguide required in order for an image of order N of the input to be formed at the output is:
where n1 is the refractive index of the core medium of the multimode waveguide, W is the width of the multimode core region and λ is the wavelength of the radiation input into the multimode waveguide. Thus, a multimode waveguide of length L1 will form a one-to-one image of its input at its output. A description of the re-imaging property can be found in the above-referenced paper.
This re-imaging property of multimode waveguides is used, in accordance with embodiments of the present invention, in conjunction with photonic crystal fibre.
For wavelengths in the range 400 nm to 1550 nm, where it is currently thought that most applications for photonic crystal fibre will be found, a suitable material for the multimode fibre 220 and photonic crystal fibre 210 is silica, which has a refractive index in the range from 1.44 to 1.47. Multimode fibre made from silica is commercially available with core sizes of 62.5 μm and 105 μm. The diameter of multimode fibre used is selected to achieve a good splice between the photonic crystal fibre 210 and the multimode fibre 220. The length of multimode fibre 220 required for the output of the fibre to comprise an image of the input to the fibre is dependent on the wavelength λ of the input radiation. For a wavelength of 532 nm, obtained from a Coherent Inc. Verdi solid state (Nd:YVO4) laser diode, and using commercially available silica multimode fibre of the above sizes, therefore, the length of the multimode fibre needed is either 10.7 mm (for 62.5 μm fibre) or 30.3 mm (for 105 μm core fibre). The tolerance for these lengths will depend on the re-image length achieved, which in turn will depend on the exact core size of the multimode fibre, and the operational wavelength. For the specific numeric examples given above, the tolerance on the re-image length is between 50 μm and 300 μm.
It is clear from the above that photonic crystal fibres terminated with multimode fibre in the manner of waveguide 200 will in general necessarily be configured specifically for one particular wavelength of light. Away from this wavelength, there will be losses at the termination where light is coupled into or out of the fibre. However, since as-supplied photonic crystal fibre is frequently optimised for transmission of a particular wavelength of light, it is not expected that the breadth of application of these waveguides will be limited in any substantial way because of the need to specify a particular wavelength at which the terminated waveguide is to be used. One exception is that such terminations will clearly not be appropriate where photonic crystal fibres are being used for ultra-broadband applications.
Multimode fibre 220 is joined to photonic crystal fibre 210 by splicing. Fusion splicing can be used to obtain a join of suitable quality. A fusion splice is effectively a “permanent weld” between two fibres. Very low insertion losses, typically less than 0.1 dB, can be achieved. Either filament-fusion splicing or arc-fusion splicing can be used. In both splicing techniques, care must be taken to ensure that the environment is clean so as to avoid ingress of foreign matter into the holes of the photonic crystal fibre.
The fibres to be spliced are first stripped of any protective polymer or acrylate coating, and cleaved, so as to leave bare fibre ends having a flat, clean end face. A length of multimode fibre much longer than that required for re-imaging is used, since, using conventional splicing machines, it is difficult to splice the required length onto a photonic crystal fibre. The fibres are located in clamps and aligned using a magnifying video camera. The fibre ends are then brought together, and heat is applied to the join region in the presence of a stream of argon gas. In the case of filament fusion splicing, heat is applied through use of a high power filament in close proximity to the join region. The fibre ends are heated to a temperature sufficient to soften the silica fibre ends without damaging the hole structure of the photonic crystal fibre. The applied heat may cause some deformation or collapse in the holes in the cladding region of the photonic crystal fibre 210, although such damage is small in comparison with that caused by the prior known hole-sealing techniques used to terminate photonic crystal fibres. A force is then applied to push the fibre ends together such that the fibres fuse. The Vytran FFS-200 is a commercially available filament fusion splicer that is suitable for carrying out the above process, and is able to carry out some of the above steps automatically. Finally, the multimode fibre is cut back to the required length.
Arc-fusion splicing can also be used to join together a length of photonic crystal fibre with a length of multimode fibre using a method similar to that described above. Arc-fusion splicers, such as the Fujikura SpliceMate, use an electrical discharge to heat the fibre ends, and are also commercially available.
Terminated photonic crystal fibres such as waveguide 200 shown in
It is preferable, in connector assemblies 300 and 400 described above, for the splice between the multimode fibre and the photonic crystal fibre to be within the ferrule. It is therefore further necessary to select the multimode fibre thickness so that the fibre assembly will fit into the ferrule, and so that there is sufficient adhesion between the fibre assembly and the ferrule. It is possible for ferrules to be customised in order to have appropriate dimensions. However, standard ferrules having a variety of hole diameters and a length of 12.7 mm are available. Thus it is preferable to use multimode fibre of width 62.5 μm, for which the one-to-one image length calculated from formula (1) above is 11 mm for radiation of wavelength 532 nm, since the standard length ferrule can be used. Moreover, it is also evident from (1) above that increasing the length of the multimode fibre relaxes the tolerance in that length.
Further embodiments of the present invention are envisaged that exploit the higher order images resulting from the multimode interference properties of waveguides in other ways. For example, those skilled in the art will appreciate that the re-imaging devices could be used to terminate photonic crystal fibres so as to provide optical splitters, where the re-imaging device is arranged such that its output comprises a multiple image of its input. It is currently envisaged that multimode waveguides with rectangular geometry would be most appropriate for such an application. Multimode waveguides having a rectangular geometry are expected to output discrete images of their input, as is necessary if the resulting structure is to be useful as an optical splitter. For example, for a rectangular waveguide having a core of height approximately equal to the diameter of the input PCF core, but with a greater width, and a length selected to produce a re-image in accordance with equation (1) above for N=2, a double image of the input would be expected at the output end of the rectangular waveguide. Square waveguides will exhibit re-imaging in both directions perpendicular to the beam axis, so that, for N=2 in equation (1) above, four images of the input beam will be formed. In the case of multimode fibre, or other waveguides of cylindrical geometry, higher order images of a single mode input are expected to be in the form of rings around a central peak. It will be noted that, whilst the size of the core of the multimode transmission device will be selected in dependence on the core size of the photonic crystal fibre, the overall dimensions of the multimode waveguide will be selected in order to achieve a good splice with the photonic crystal fibre.
The intensity profile of the beam will therefore vary significantly at higher order re-imaging points in dependence on a number of factors including the geometry of the multimode fibre. It may be possible to increase the on-axis intensity. Such an increased intensity will be advantageous in non-linear optics applications where high intensity beams are highly desirable. Alternatively, it may be possible that the maximum intensity of the beam is reduced. Such a reduced intensity would be advantageous where connections between different fibres carrying high energy beams are required, since, at high intensities, even small imperfections can result in severe damage to the optical system.
Such damage can frequently occur where high intensity beams impinge on connectors or lenses. Thus any reduction in the maximum intensity of a beam can be useful at connection points, particularly where the initial intensity of the beam can be regained after transmission through the connection. By exploiting a reduction in maximum intensity obtained as a result of using, as the connection interface, a point in a multimode fibre at which higher order re-images are obtained, the risk of such damage can be reduced. For example, R. M. Jenkins, R. W. J. Devereux, and J. M. Heaton, in their paper “Waveguide beam splitters and recombiners based on multimode propagation phenomena”, published at page 991 of Optics Letters, Volume 14 (1992), propose a rectangular waveguide splitter in which an input beam is split into two. Modeling presented in that paper demonstrates a reduction in the intensity of the split beams in comparison to the input beam. By providing photonic crystal fibres terminated with lengths of such waveguide selected such that such a second order re-image is obtained at the output, the maximum intensity at any point on the connecting interface is reduced in comparison to the maximum intensity of the input beam. For high power beams (of the order of 100 W or greater), which photonic crystal fibres are often used to transmit, the reduction of maximum intensity obtained in such a way reduces the risk of damage occurring at the connection interface. The splicing of rectangular waveguide, of dimensions selected such that a second order re-image of the input is obtained at the output end, onto photonic crystal fibre, can therefore be used where high power beams are to be transmitted along the photonic crystal fibre.
Similarly, the third order re-image could be exploited. The third order re-image, for the above geometry, is expected to have a lower maximum intensity. However, the length of multimode waveguide required to obtain a third order re-image is one third that required to obtain a one-to-one re-image of the input beam. Thus, two photonic crystal fibres to be connected together are terminated by complimentary lengths of multimode waveguide: one photonic crystal fibre is terminated by a length of multimode fibre one-third that required to form a one-to-one re-image, and a photonic crystal fibre to which it is to be connected can be terminated by a length of multimode waveguide that is two-thirds that required to form a one-to-one re-image. To ensure the correct terminations are combined, it is desirable to form the terminated ends in male and female connectors. Higher order re-images could also be used. As those skilled in the art will appreciate, such applications are not restricted to connecting photonic crystal fibres, but will be of use wherever high power laser beams are transmitted along waveguides.
Having described the invention with reference to various specific embodiments, it is noted that these embodiments are purely exemplary, and that variations and modifications to these embodiments are possible without departing from the spirit and scope of the invention, which is defined in the appended claims. For example, whilst it has been described above to use photonic crystal fibres and multimode fibres fabricated from silica for use at wavelengths of or around 532 nm, it will be immediately obvious to those skilled in the art that the invention extends to other wavelength ranges, in which it may be necessary to use fibres fabricated from materials other than silica. In particular, for operation at longer wavelengths, such as between 2 μm and 4 μm, photonic crystal fibres and multimode fibres fabricated from telluride, fluoride or chalcogenide glasses can be used.
Moreover, those skilled in the art will immediately realise that, whilst the use of solid-core photonic crystal fibres has been described above, it will also be possible to apply the inventive concepts described to hollow-core photonic crystal fibres. In such embodiments, hollow-core waveguides are used to form the re-imaging multimode transmission region. Those skilled in the art will appreciate that it will be necessary to incorporate a window into the waveguide at some point in order to seal the holes of the photonic crystal fibre—for example, at the outer end of the multimode hollow-core waveguide. Those skilled in the art will also realise that, whilst in the above it has been described to use multimode fibre to provide the re-imaging device, any multimode transmission device capable of supporting multimode interference and re-imaging can be used in conjunction with the present invention, such as multimode waveguides of other geometries. Such multimode transmission devices could include square or rectangular waveguides. Moreover, any re-imaging device operable to reproduce its optical input at its output could be used to terminate photonic crystal fibres in accordance with the invention.
It is also to be clearly understood that any feature described above in relation to any one embodiment may be used alone, or in combination with other features described, and may also be used in combination with one or more features of any other of the embodiments, or any combination of any other of the embodiments.
| Number | Date | Country | Kind |
|---|---|---|---|
| 07270041.2 | Aug 2007 | EP | regional |
| 0715505.4 | Aug 2007 | GB | national |
| 0810375.6 | Jun 2008 | GB | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/GB2008/050668 | 8/6/2008 | WO | 00 | 12/12/2008 |
