US20020181911A1

US20020181911A1 - Optical material and a method for its production

Info

Publication number: US20020181911A1
Application number: US09/845,528
Authority: US
Inventors: William Wadsworth; Brian Mangan; Timothy Birks; Jonathan Knight; Philip Russell
Original assignee: Individual
Current assignee: Individual
Priority date: 2001-04-30
Filing date: 2001-04-30
Publication date: 2002-12-05
Also published as: US7116875B2; DE60222111T2; ATE371878T1; DK1388018T3; WO2002088802A1; EP1388018B1; US20040151450A1; EP1388018A1; DE60222111D1

Abstract

A composite material for supporting propagation of light of a wavelength λ, comprising a plurality of cylinders each having a longitudinal axis, the cylinders being separated from each other by regions of a matrix material and the cylinders having their longitudinal axes substantially parallel to each other, and each cylinder having a diameter, in the plane perpendicular to the longitudinal axis, that is small enough for the composite material to be substantially optically homogeneous in respect of light of wavelength λ.

Description

This invention relates to the field of optical materials.

U.S. Pat. No. 5,155,792 teaches an optical fibre having a low index of refraction. In one embodiment described in the Patent, the cladding of the fibre comprises a uniform array of tube structures each being of a diameter less than the shortest wavelength of light guided by the fibre. The core may be formed from a rod or from several rods of uniform refractive index. In another embodiment, the core of the fibre also comprises a uniform array of tube structures each being of a diameter less than the shortest wavelength of light guided by the fibre, the core having a higher refractive index than the cladding but nevertheless a uniform and low refractive index.

However, that U.S. Patent does not contemplate the possibility of engineering the optical properties of a material other than by providing a uniform and low refractive index.

An object of the invention is to provide an optical material having optical properties that can readily be engineered. An object of the invention is to provide a method of engineering such properties.

According to the invention there is provided a composite material for supporting propagation of light of a wavelength λ, comprising a plurality of cylinders each having a longitudinal axis, the cylinders being separated from each other by regions of a matrix material and the cylinders having their longitudinal axes substantially parallel to each other, and each cylinder having a diameter, in the plane perpendicular to the longitudinal axis, that is small enough for the composite material to be substantially optically homogeneous in respect of light of wavelength λ.

Such an arrangement of cylinders is referred to below as “nanostructure”, although the cylinders may, in some circumstances, be of dimensions and/or separations of a larger scale than nanometers.

Substantially optically homogeneous material causes no significant perturbation of the transverse optical field profile of light propagating in the composite material. Of course, whether or not the cylinders cause significant perturbation of the transverse optical field profile of propagating light is a question that may be determined experimentally. However, one way to quantify the effect of the cylinders is to calculate a modified version of the well-known V-parameter (also known as the V-value or normalised frequency). In a simple case of cylinders of cross-sectional area A and of a material of refractive index n _cylinderembedded in a matrix material of refractive index n_matrix, the modified V-value V is given by

\begin{matrix} V^{2} = \frac{4 π A}{λ^{2}} \langle n_{cylinder}^{2} - n_{matrix}^{2} \rangle & (1) \end{matrix}

The modified V-value gives a measure of how confined to the cylinders is the transverse optical field. If the V-value is small (less than 1, for example) then the optical field is not well confined and the cylinders will not cause a significant perturbation. Ever smaller values of V are in general preferable, for example V<0.6 or even V<0.4.

In more complicated embodiments of the invention, such as, for example, when each cylinder comprises an inner region of refractive index n ₁and area A₁, surrounded by an annular outer region of refractive index n₂and area A₂, one may calculate a “collective V-value” V_c. For p regions embedded, directly or indirectly, in a matrix material, each region being of refractive index n_pand area A_p, we define

\begin{matrix} V_{c} = \sqrt{\sum_{p} V_{p}^{2}}, where V_{p}^{2} = \frac{4 π A_{p}}{λ^{2}} \langle n_{p}^{2} - n_{matrix}^{2} \rangle & (2) \end{matrix}

Again, if the v-value is small, then the optical field is not well confined and the embedded regions will not cause a significant perturbation of the transverse profile of an optical field of wavelength λ.

In some circumstances, such as when a waveguide is defined in the material, another indication of the effect the cylinders would have on an optical field can be obtained by evaluating a transverse component k sin θ of the wavevector k for light propagating at an angle θ to the longitudinal axis of the cylinders. That component gives an effective transverse wavelength

\begin{matrix} λ_{eff} = \frac{2 π}{k \sin θ} & (3) \end{matrix}

which will in general be greater than λ. The material will be substantially optically homogeneous if the diameter of the cylinders is small compared with λ _eff.

As light propagating in the material will in general see only an average of the optical properties of the cylinders and the matrix regions, the optical properties of the material may be engineered by appropriate choice of cylinder and matrix properties and by the arrangement of the cylinders in the matrix. A wide range of properties may be introduced, for example by using cylinders comprising different materials in different parts of the material or by doping the cylinders.

Preferably, the composite material is arranged to support propagation of light in a direction substantially parallel to the longitudinal axes. Preferably, the cylinders are solid. The cylinders may comprise a dielectric material. The cylinders may comprise a metal. At least some of the cylinders may be holes defined by the matrix regions. The holes may be filled with a fluid; such an arrangement of holes filled with a gas, in particular a gas other than air, or a liquid may be used to provide a nonlinear material. Preferably, the material is arranged to guide light propagating in a direction not in the plane perpendicular to the longitudinal axis.

It will be understood that the word “cylinder” refers to any three-dimensional figure of uniform cross-section, which cross-section is not necessarily circular. Preferably, the cylinders are of circular cross section.

Preferably, the diameter of the cylinders is less than 1 micron.

The refractive index of the cylinders may be less than that of the regions of a matrix material. The refractive index of the cylinders may be greater than that of the regions of a matrix material. Alterations to the refractive indices may be achieved in different ways, some of which are discussed below.

Preferably, the cylinders comprise an inner region having a first refractive index n _innerand an outer region having a second refractive index n_outerand surrounding the inner region so that the refractive index of the cylinder is an effective refractive index that is between the first and the second refractive indices. If the diameter of the cylinders is small compared with the wavelength of propagating light, and if the absolute variation of refractive index is small, the effective refractive index n_eff ^cylwill be given approximately by

\begin{matrix} n_{eff}^{cyl} = \frac{n_{inner} A_{inner} + n_{outer} A_{outer}}{A_{inner} + A_{outer}} & (4) \end{matrix}

where A _innerand A_outerare the cross-sectional areas respectively of the inner and outer regions of each cylinder. Equation (4) is an approximation given for the purpose of aiding understanding of the invention; in general, expressions for the effective refractive index are not so simple but may readily be calculated by a person skilled in the art.

The effective refractive index may be equal to the refractive index of the matrix regions. It is thus possible to use different materials in the inner region, the outer region and the matrix region, each of which materials may have different, desirable properties, but still present a uniform effective refractive index to propagating light.

Some parts of the material may have different properties from other parts of the material. The cylinders may be distributed in the matrix material at different densities in different parts of the material. It may be that the regions of a matrix material are not all of the same material and/or that the cylinders are not all identical to each other; for example, it may be that the cylinders are not all of the same refractive index, shape, size and/or material.

Preferably, at least some of the cylinders have been doped with a dopant. At least some of the regions of a matrix material may have been doped with a dopant. Doping is a convenient way to change the optical properties of a material; stresses in the material may be much less than if two different materials are used and fused together.

Preferably, the doping results in a change in refractive index. Doping can then be used to provide a selected effective refractive index of the material and, for example, to introduce refractive-index structures into the material.

Preferably, at least some of the cylinders are doped with an optically active dopant.

Preferably, the optically active dopant renders the material photosensitive; examples of suitable dopants would be germanium, boron, or tin. It may be that not all of the cylinders are doped in the same manner, so that not all regions of the material are equally photosensitive. Such a material could be incorporated into, for example, multicore fibre.

The optically active dopant may provide optical gain; for example, the optically active dopant may comprise ytterbium or erbium. It may be that not all of the cylinders are doped with the same optically active dopant, so that gain is provided at two or more different wavelengths; thus “dual wavelength” operation may be provided.

Preferably, the composite material has a selected effective-refractive-index profile in the plane perpendicular to the longitudinal axes. Such a selected effective-refractive-index profile may be provided, for example, by altering the refractive index of a bulk material by any of the means described above.

Preferably, the selected effective-refractive-index profile is a gradual decrease in refractive index radially from the centre of the material. Such a graded-index structure may be a useful waveguiding structure.

Nanostructuring according to the invention is a convenient means of introducing other effective-refractive-index profiles into the material. For example, the selected effective-refractive-index profile may define a regular polygon. Alternatively, the selected effective-refractive-index profile may define a non-regular figure.

Preferably, the selected effective-refractive-index profile defines a waveguide including a core having an effective refractive index that is larger than the effective refractive index of material surrounding the core. Preferably, the core is larger than 10 microns in its smallest transverse dimension and the difference between the effective refractive index of the core and the effective refractive index of the material surrounding the core is sufficiently small for the waveguide to support single-mode propagation of light (for example, a 25 micron diameter core with a refractive index of 1.5 would support propagation of light of wavelength 1.5 microns in a single mode if the refractive index difference is less than 0.0007). Ever larger cores may be preferable in many applications; preferably, the core is larger than 15 microns, more preferably larger than 20 microns and still more preferably larger than 25 microns in its smallest transverse dimension.

The refractive-index profile may result in additional changes in the optical properties of the material; for example, it may define an optically dispersive material.

The composite material may exhibit birefringence due to mechanical stresses between the cylinders and the regions of a matrix material. Birefringence will generally result if the material has no rotational symmetry higher than two-fold rotational symmetry, about any longitudinal axis Thus, the material may have two-fold rotational symmetry or no rotational symmetry about such an axis. The rotational symmetry of the material may result at least partly from the shape of the cylinders. The rotational symmetry of the material may result at least partly from the distribution of the cylinders.

Also according to the invention there is provided an optical amplifier comprising a composite material as described above as being according to the invention. Preferably, the optical amplifier is a large-mode-area amplifier. Also according to the invention there is provided a laser including such an optical amplifier.

Also according to the invention there is provided a method of providing a selected optical property in a composite material for supporting propagation of light of a wavelength λ comprising: (i) providing a plurality of rods each having a longitudinal axis, a inner region of a first solid material and an outer region of a second solid material and surrounding the inner region; (ii) forming a bundle of the rods, in which the rods have their longitudinal axes substantially parallel to each other, and (iii) drawing an elongate, fused rod from the bundle; cutting the fused rod into a plurality of lengths; and (iv) repeating steps (ii) and (iii) at least once by forming the bundle from the lengths of fused rod and drawing a further, elongate fused rod from the bundle; wherein, the inner regions of the rods used in step (i) form, in the further, elongate fused rod produced at the end of step (iv), a plurality of solid cylinders each having a longitudinal axis, the cylinders being separated from each other by regions of a matrix material and the cylinders having their longitudinal axes substantially parallel to each other, and each cylinder having a diameter, in the plane perpendicular to the longitudinal axis, that is small enough for the composite material to be substantially optically homogeneous in respect of light of wavelength λ.

Thus, the optical properties of the composite material are fixed by arranging macroscopic objects and then drawing reduces the dimensions of the structure until the material becomes substantially optically homogeneous.

Preferably, the bundle of rods is enclosed in a jacket in step (ii). An advantage of using a jacket is that the spaces between the canes may be evacuated to eliminate unwanted air holes that would otherwise be formed in the drawing process.

Also according to the invention there is provided a method of manufacturing an optical fibre, including the step of drawing an optical fibre from a preform comprising at least one rod manufactured by such a method. Preferably, the method includes the step of enclosing the preform in a jacket prior to drawing the fibre.

Preferably, in at least some of the rods the inner region has a first refractive index and the outer region has a second, different refractive index.

Also according to the invention there is provided an optical fibre comprising a composite material as described above as being according to the invention. Preferably, the fibre is a photonic crystal fibre. Photonic crystal fibres are also known as microstructured fibres. Such fibres typically have a cladding comprising an array of elongate holes. If the effective refractive index of the cladding is lower than that of the core then a photonic-crystal fibre generally guides light by total internal reflection. Otherwise, a photonic-crystal fibre has its elongate holes arranged in a periodic lattice that excludes light at certain frequencies, forming a photonic band-gap. The core in such a fibre acts as a defect that breaks the periodicity of the lattice and allows propagation of light at frequencies in the photonic band-gap; the light is thereby confined to the core.

Also according to the invention, there is provided a fibre amplifier comprising such a fibre. Also according to the invention, there is provided a fibre laser comprising such an amplifier.

Also according to the invention, there is provided a method of transmitting light in a composite material described above as being according to the invention.

Various embodiments of the invention will now be described, by way of example only, with reference to the accompanying drawings, of which: [0042]
FIG. 1 is an optical micrograph of a preform produced as a step in a method according to the invention; [0043]
FIGS. 2 and 3 are optical micrographs of the cleaved ends of photonic-crystal fibres according to the invention drawn from the preform of FIG. 1; [0044]
FIGS. 4 and 5 are schematic cross-sections through optical fibres incorporating in their cores an optical material according to the invention, the optical material having a graded refractive-index structure; [0045]
FIG. 6 is a schematic cross-section through a single-mode waveguide laser or amplifier, which has a very large core incorporating an optical material according to the invention; [0046]
FIG. 7 is a schematic cross-section through a single-mode optical fibre having unusual dispersion properties resulting from use of a core incorporating an optical material according to the invention; [0047]
FIG. 8 is a schematic cross-section through a photonic-crystal fibre, which exhibits photosensitivity resulting from incorporation in its core of an optical material according to the invention; [0048]
FIG. 9 is a schematic cross-section through a photonic-crystal fibre laser or amplifier, which exhibits dual-wavelength gain resulting from incorporation in its core of an optical material according to the invention; [0049]
FIGS. 10 and 11 are schematic cross-sections through optical fibres, which exhibit birefringence resulting from incorporation in their core of an optical material according to the invention; [0050]
FIG. 12 is a schematic cross-section through a further photonic-crystal fibre incorporating an optical material according to the invention.[0051]
The schematic figures are, of course, not drawn to scale. [0052]
In an embodiment of the invention, a bundle is formed from rods each having a core region of doped silica and a second, outer region, of undoped silica, which surrounds the core region. A jacket, in the form of a tube of undoped silica is placed around the bundle. An elongate, fused rod is drawn from the jacketed bundle by heating it and stretching it in a manner well known in the prior art. The fused rod is cut into segments of equal length and a further bundle is formed from those lengths of fused rod. That further bundle is placed inside a jacket of undoped silica and further fused rod is similarly drawn from that further bundle. The rod resulting from three bundling steps is shown in FIG. 1. [0053] Doped regions 10 and undoped matrix regions 20 result from the doped cores and the undoped outer regions (respectively) of the rods provided initially. The jackets placed around those rods form matrix regions 30 and the jacket placed around the further rods forms region 40. The jacketed bundle has been drawn into a further rod, which has been bundled together with rods in the form of capillaries. That bundle is also jacketed and drawn. Elongate holes 50 result from the hollow cores of the capillaries and regions 60 result from the material of the capillary walls. Interstitial holes 70 result from the imperfect tiling of the capillary cross-sections.
The rod of FIG. 1 is a preform for production of optical fibre. The rod is drawn, in the usual way, to produce photonic-crystal fibre of [0054] diameter 120 μm and core diameter 15 μm between the innermost air-holes. FIG. 2 shows such a fibre that has a ratio of hole diameter d to hole pitch λ of d/λ=0.3. FIG. 3 shows a fibre drawn from the same preform but drawn to have larger holes, with d/λ=0.55. Different hole sizes are achieved by changing the drawing tension by controlling the temperature of the drawing furnace.
In the drawn fibres of FIG. 2 and FIG. 3, [0055] core region 80 is optically homogeneous even though it is formed from cylindrical doped regions separated by silica matrix regions (the regions in which the cylinders are embedded, invisible in FIGS. 2 and 3 but corresponding to doped regions 10 and matrix regions 20 and 30 in FIG. 1; in this embodiment, the regions of a matrix material are continuous with each other and with the silica of the photonic crystal cladding 82 and the fibre jacket 87). The effective refractive index step is approximately 0.001. Optical homogeneity result because each of the cylindrical doped regions has a diameter of less than 250 nm, which is small compared with the effective transverse wavelength of the guided mode of light that the fibre is to guide (in this case 1040 nm). The area filling fraction of the doped glass is a few percent so the resulting effective-refractive-index step is insufficient for guidance of light within the cylinders themselves to occur.
FIGS. [0056] 4 to 12 show other ways in which material structured at a scale small enough for the material to appear homogeneous to light can be used to provide fibres and other devices having interesting properties.
The single-mode optical fibre (the example illustrated is not a photonic crystal fibre) of FIG. 4 has a graded-index structure. The graded-index structure is achieved by provision of doped [0057] cylinders 110, 120 in a fibre comprising principally of bulk, undoped silica 130. Cylinders 110 are arranged to form hexagonal region 140 at the centre of the fibre cross-section. Region 140 is enclosed by six hexagonal regions 150, formed by cylinders 120. Hexagonal regions 140, 150 result from the bundling and drawing process. Cylinders 110 (and, similarly, cylinders 120) are separated by matrix material 160, which results from the undoped silica outer regions of the rods from which the material is drawn. Regions 140, 150 are separated by matrix material 170, which results from jacketing the bundles in the bundling and drawing process and, in this embodiment, is also formed of undoped silica. Regions 140, 150 are themselves surrounded by a thick cladding region 180, which is formed by repeated jacketing of a bundle comprising the preforms for regions 140, 150.
[0058] Cylinders 110 are formed of silica doped with germanium ions Such doped silica has a refractive index that is higher than that of bulk silica. The separation of the cylinders 110 is small compared with the wavelength of light that the fibre is to be used to guide and so the effective refractive index seen by the light is an average of the refractive index n_cylinderof the doped silica and the refractive index n_motrixof the undoped matrix regions between cylinders 110. The diameter of the cylinders is small compared with the wavelength of propagating light, and the absolute variation of refractive index is small, so the effective refractive index n_errof region 130 is given approximately by: $\begin{matrix} n_{eff} = \frac{n_{cylinder} A_{cylinder} + n_{matrix} A_{matrix}}{A_{cylinder} + A_{matrix}} & (5) \end{matrix}$
where A[0059] _cylinderand A_matrixare the areas taken up by cylinders and matrix regions in region 140.
[0060] Cylinders 120 are formed of silica that is less heavily doped. Each of those cylinders 120 thus has a refractive index that is higher than that of bulk silica but lower than that of the doped silica in cylinders lo. The effective refractive index of region 150 is thus higher than that of cladding 180 but lower than that of region 140.
The refractive index seen by light propagating in the fibre thus decreases from the centre of the fibre radially outwards. Light is guided by total internal reflection but the interface between the [0061] core region 110 and the cladding 180 of the fibre is distributed over a portion of the fibre diameter rather than being a single, abrupt step. Thus the fibre acts as a graded-index fibre. The profile of the refractive-index variation may readily be adjusted in different fibres by adjusting the dopant concentrations at different sites.
The fibre of FIG. 5 embodies another approach to providing a graded-index fibre by providing nanostrucure. [0062] Central region 240 corresponds to region 140 in FIG. 4. However, regions 250 are formed from bundles in which rods doped to the same concentration as the rods forming region 240 are interspersed with undoped rods. That arrangement of rods results in regions 250 having a lower effective refractive index than region 240 and, furthermore, cylinders 220, which result from the doped rods, are themselves arranged in region 250 to be concentrated more to the centre of the fibre so that the effective refractive index of regions 250 themselves decreases radially outward.
The single-mode waveguide laser of FIG. 6 has a very [0063] large core 300 formed by use of nanostructured material to create a very small but uniform refractive-index contrast. Core 300 comprises an approximately rectangular arrangement of hexagonal regions 330, which each contain cylinders, which are made of doped silica, separated by undoped silica matrix regions.
[0064] Core 300 is embedded in an inner cladding 340 (which is made of bulk, undoped silica) to facilitate cladding pumping. Inner cladding 340 is supported in a glass tube 360 so that an outer cladding region of air 370 results that surrounds inner cladding 340 within tube 360.
The [0065] cylinders forming regions 330 are of two types. Those of the first type, of refractive index n_cylinder ^Er, are doped with Erbium ions to provide a gain medium (they are also co-doped with aluminium to improve erbium ion solubility). Those of the second type, of refractive index n_cylinder ^Ge, are doped with germanium to control the effective refractive index of core 300. The diameter of the cylinders is small compared with the wavelength of propagating light, and the absolute variation of refractive index is small, so the effective refractive index of the core 300 is given approximately by: $\begin{matrix} n_{eff} = \frac{n_{matrix} A_{matrix} + n_{cylinder}^{Ge} A_{cylinder}^{Ge} + n_{cylinder}^{Er} A_{cylinder}^{Er}}{A_{matrix} + A_{cylinder}^{Ge} + A_{Cylinder}^{Er}} & (6) \end{matrix}$
where A[0066] _matrix, A_cylinder ^Geand A_cylinder ^Erare the areas taken up by the matrix regions, germanium-doped cylinders and Erbium-doped cylinders in the cross-section of core 300.
The cylinders of several different materials are repeatedly mixed during bundling and drawing to increase the uniformity. [0067]
The effective refractive index of the [0068] core 300 is controlled so that the difference in refractive index between the core 300 and the inner cladding 340 is sufficiently small for the waveguide to guide light propagating in a large single mode. The condition for single-mode operation is well-known: the normalised frequency V must be less than 2.405, where in this case $\begin{matrix} V^{2} = \frac{4 π A}{λ^{2}} (n_{eff}^{2} - n_{cladding}^{2}) & (7) \end{matrix}$
where A is the area of the core and n[0069] _claddingis the refractive index of the cladding.
It is interesting to note that, if the same amount of doped glass were to be contained within a single doped region, then the guided mode of the fibre would be very strongly peaked in the doped region. In order to obtain a large mode area, a single doped region would have to be much smaller and hence would contain fewer dopant ions, reducing the absorption and gain. [0070]
The single-mode optical fibre of FIG. 7 has an unusual dispersion characteristic, which is similar to that of known W-index fibres. The fibre consists of a core [0071] 400 surrounded by a cladding 470. The core 400 contains hexagonal regions 430, 440, 450, each containing cylinders 410 of silica doped with germanium, separated by matrix regions of undoped silica. Region 430 is drawn from bundled doped rods. Region 450 is also drawn from bundled doped rods but the concentration of dopant in the doped cores is lower than for region 430. Region 440 is drawn from a bundle containing rods such as those from which region 450 is drawn but, in region 440, the doped rods are interspersed with undoped silica rods. The effective refractive index of the core thus decreases radially outwards from a maximum in region 430, through a local minimum in region 440, increases to a higher figure in region 450 (but not as high as in region 430) and then decreases again to the index of the bulk silica that forms the cladding 470.
The fibre of FIG. 8 is a photonic crystal fibre into which a photosensitive material has been incorporated by means of a [0072] nanostructured core 500. The core is surrounded by a photonic-crystal cladding region 530 surrounded by a jacket region 570. Cladding region 530 includes a periodic array of cylindrical holes, arranged on a triangular lattice, running through bulk silica. The jacket is bulk silica Core 500 acts as a defect in the photonic crystal and light at certain wavelengths, which are excluded from propagation in the photonic crystal, can propagate in the defect. Core 500 comprises hexagonal regions 520, which in turn are made from cylinders 510 separated by undoped silica matrix regions. Cylinders 510 are made from silica doped with Germanium ions. Germanium-doped silica glass is photosensitive, so that the refractive index of Germanium-doped silica changes on exposure to light. Such a fibre can be used to make fibre Bragg gratings by exposure to light, for example in order to form an optical cavity within the fibre or to form a wavelength-selective filter.
The fibre of FIG. 9 exhibits gain over two wavelength bands centred on two independent transitions and thus has an extended gain spectrum. Such dual-wavelength operation is possible because the fibre has a [0073] nanostructured core 600 that is doped with both Ytterbium ions and Erbium ions. Ytterbium exhibits gain at a centre wavelength of around 1040 nm and Erbium exhibits gain at a centre wavelength of around 1550 nm. Core 600 is surrounded by bulk silica cladding 670 and comprises hexagonal regions 640. Each hexagonal region 640 is drawn from a bundle of rods, half of which have been doped with Ytterbium ions and half of which have been doped with Erbium ions. The dopant ions thus provide uniform grain at both lasing wavelengths across core 600. However, because cylinders 610, drawn from the doped rods, are spatially separated on a nanometer scale by bulk silica matrix material (originating in the outer, undoped part of each doped rod), energy-transfer effects between the dopant ions are reduced.
The fibres of FIGS. 10 and 11 are birefringent because of the symmetries of the nanostructuring of their cores. The fibre of FIG. 10 has a substantially [0074] circular core 700, made of many cylinders 710 of substantially elliptical cross-section, the ellipses being significantly eccentric. The core 700 is here drawn from a bundle of rods that have been flattened in one direction perpendicular to their longitudinal axis so that they have an elliptical cross-section. The two-fold rotational symmetry of each of the cylinders results in birefringence, because light polarised in a direction parallel to the major axis of each ellipse sees a different refractive index from light polarised in a direction perpendicular to that direction. However, because the cylinders have diameters smaller than the wavelength of the light that the fibre is to support, the birefringence produced may be regarded as an inherent optical property of the nanostructured material, rather than as a structure affecting the light at the scale of the fibre cross-section. The core 700 is surrounded by a cladding 770.
The fibre of FIG. 11 achieves the same result—creation of a birefringent nanostructured material—by drawing a [0075] rectangular core 800 from a bundle of rods arranged in diagonal rows. Across the cross-section of the fibre, the rows are alternately bulk silica rods and rods Made from germanium-doped silica. In the fibre, the doped cores form cylinders 810, which are similarly arranged in rows, and the undoped silica forms matrix regions 820. Light polarised in a direction parallel to the rows therefore sees a different refractive index from light polarised in a direction perpendicular to that direction and so the fibre exhibits birefringence, again at the scale of the material rather than the fibre core. Cladding 870 surrounds the core 800.
The photonic-crystal fibre of FIG. 12 comprises a core [0076] 900 surrounded by a cladding region comprising a periodic array of elongate holes 950 (not all shown), which is in turn surrounded by a jacket 970. Core 900 is formed of hexagonal regions 930, which each comprise an array of cylinders 910, which has been drawn from a bundle of rods. As is shown in the magnified portion of FIG. 12, each cylinder comprises an inner region 912 and an outer region 917 and the cylinders are, as in the other illustrated embodiments, separated by an undoped silica matrix 920. The inner regions 912 are doped with germanium so that they have a refractive index n_inner ^Gethat is higher than the refractive index of silicon n_matrix. The outer regions 917 have been doped with fluorine so that they have a refractive index n_outer ^Fthat is less than that of silicon. The cylinders are drawn from rods made by enclosing a germanium-doped rod in a fluorine-doped jacket. The doping levels are chosen so that, because the raised-index and depressed-index regions occur on a scale that is small compared with the wavelength of propagating light, and the absolute variation of refractive index is small, the effective refractive index of the material is approximately equal to the refractive index n^Siof bulk silica: $\begin{matrix} n_{eff} = \frac{n_{matrix} A_{matrix} + n_{inner}^{Ge} A_{inner}^{Ge} + n_{outer}^{F} A_{outer}^{F}}{A_{matrix} + A_{inner}^{Ge} + A_{outer}^{F}} = n^{Si} & (4) \end{matrix}$
where A[0077] _matrix, A_inner ^Geand A_outer ^Fare the areas occupied by the matrix regions, the germanium-doped regions and the fluorine-doped regions, respectively. Thus, by nanostructuring, dopants may be incorporated into a material without changing the bulk refractive index of that material.

Claims

1. A composite material for supporting propagation of light of a wavelength λ, comprising a plurality of cylinders each having a longitudinal axis, the cylinders being separated from each other by regions of a matrix material and the cylinders having their longitudinal axes substantially parallel to each other, and each cylinder having a diameter, in the plane perpendicular to the longitudinal axis, that is small enough for the composite material to be substantially optically homogeneous in respect of light of wavelength λ.

2. A composite material as claimed in claim 1, in which the cylinders are solid.

3. A composite material as claimed in claim 1, in which the cylinders comprise a dielectric material.

4. A composite material as claimed in claim 1, in which the cylinders comprise a metal.

5. A composite material as claimed in claim 1, in which at least some of the cylinders are holes defined by the matrix regions.

6. A composite material as claimed in claim 5, in which at least some of the holes are filled with a fluid.

7. A composite material as claimed in any preceding claim, in which the diameter of the cylinders is less than 1 micron.

8. A composite material as claimed in any preceding claim, in which the refractive index of the cylinders is less than that of the regions of a matrix material.

9. A composite material as claimed in any of claims 1 to 7, in which the refractive index of the cylinders is greater than that of the regions of a matrix material.

10. A composite material as claimed in any preceding claim, in which the cylinders comprise an inner region having a first refractive index and an outer region having a second refractive index and surrounding the inner region so that the refractive index of the cylinder is an effective refractive index that is between the first and the second refractive indices.

11. A composite material as claimed in claim 10, in which the effective refractive index is equal to the refractive index of the matrix regions.

12. A composite material as claimed in any preceding claim, in which the cylinders are distributed in the matrix material at different densities in different parts of the material.

13. A composite material as claimed in any preceding claim, in which the regions of a matrix material are not all of the same material.

14. A composite material as claimed in any preceding claim, in which the cylinders are not all identical to each other.

15. A composite material as claimed in claim 14, in which the cylinders are not all of the same refractive index.

16. A composite material as claimed in claim 14 or claim 15, in which the cylinders are not all of the same shape.

17. A composite material as claimed in any of claims 14 to 16, in which the cylinders are not all of the same size.

18. A composite material as claimed in any of claims 14 to 17, in which the cylinders are not all of the same material.

19. A composite material as claimed in any preceding claim, in which at least some of the cylinders have been doped with a dopant.

20. A composite material as claimed in any preceding claim, in which at least some of the regions of a matrix material have been doped with a dopant.

21. A composite material as claimed in claim 19 or claim 20, in which the doping results in a change in refractive index.

22. A composite material as claimed in any of claims 19 to 21, in which at least some of the cylinders are doped with an optically active dopant.

23. A composite material as claimed in claim 22, in which the optically active dopant renders the material photosensitive.

24. A composite material as claimed in claim 23, in which the optically active dopant is germanium, boron, or tin.

25. A composite material as claimed in claim 23 or claim 24, in which not all of the cylinders are doped in the same manner, so that not all regions of the material are equally photosensitive.

26. A composite material as claimed in claim 22, in which the optically active dopant provides optical gain.

27. A composite material as claimed in claim 26, in which not all of the cylinders are doped with the same optically active dopant, so that gain is provided at two or more different wavelengths.

28. A composite material as claimed in claim 26 or claim 27 in which the optically active dopant comprises ytterbium or erbium.

29. A composite material as claimed in any preceding claim, having a selected effective-refractive-index profile in the plane perpendicular to the longitudinal axes.

30. A composite material as claimed in claim 29, in which the selected effective-refractive-index profile is a gradual decrease in refractive index radially from the centre of the material.

31. A composite material as clamed in claim 29, in which the selected effective-refractive-index profile defines a regular polygon.

32. A composite material as claimed in claim 29, in which the selected effective-refractive-index profile defines a non-regular figure.

33. A composite material as claimed in any of claims 29 to 32, in which the selected effective-refractive-index profile defines an optically dispersive material.

34. A composite material as claimed in any of claims 29 to 32, in which the selected effective-refractive-index profile defines a waveguide including a core having an effective refractive index that is larger than the effective refractive index of material surrounding the core.

35. A composite material as claimed in claim 34, in which the core is larger than 10 microns in its smallest transverse dimension and the difference between the effective refractive index of the core and the effective refractive index of the material surrounding the core is sufficiently small for the waveguide to support single-mode propagation of light.

36. A composite material as claimed in any preceding claim, which exhibits birefringence due to mechanical stresses between the cylinders and regions of a matrix material.

37. A composite material as claimed in any preceding claim, in which the material has no rotational symmetry higher than two-fold rotational symmetry about any longitudinal axis, so the composite material is birefringent.

38. A composite material as claimed in claim 37, in which the material has no rotational symmetry about any longitudinal axis.

39. A composite material as claimed in claim 37, in which the material has two-fold rotational symmetry about a longitudinal axis.

40. A composite material as claimed in any of claims 37 to 39, in which the rotational symmetry of the material results at least partly from the distribution of the cylinders.

41. A composite material as claimed in any of claims 37 to 40, in which the rotational symmetry of the material results at least partly from the shape of the cylinders.

42. A composite material as claimed in any of claims 1 to 40, in which the cylinders are of circular cross-section.

43. An optical amplifier comprising a composite material as claimed in any preceding claim.

44. An optical amplifier as claimed in claim 43, which is a large-mode-area amplifier.

45. A laser including an optical amplifier as claimed in claim 43 or claim 44.

46. A method of providing a selected optical property in a composite material for supporting propagation of light of a wavelength λ comprising:

providing a plurality of rods each having a longitudinal axis, a inner region of a first solid material and an outer region of a second solid material and surrounding the inner region;

forming a bundle of the rods, in which the rods have their longitudinal axes substantially parallel to each other, and drawing an elongate, fused rod from the bundle;

cutting the fused rod into a plurality of lengths; and

repeating steps (ii) and (iii) at least once by forming the bundle from the lengths of fused rod and drawing a further, elongate fused rod from the bundle;

wherein, the inner regions of the rods used in step (i) form, in the further, elongate fused rod produced at the end of step (iv), a plurality of solid cylinders each having a longitudinal axis, the cylinders being separated from each other by regions of a matrix material and the cylinders having their longitudinal axes substantially parallel to each other, and each cylinder having a diameter, in the plane perpendicular to the longitudinal axis, that is small enough for the composite material to be substantially optically homogeneous in respect of light of wavelength λ.

47. A method as claimed in claim 46, in which the bundle of rods is enclosed in a jacket in step (ii).

48. A method of manufacturing an optical fibre, including the step of drawing an optical fibre from a preform comprising at least one rod manufactured by the method according to claim 46 or claim 47.

49. A method as claimed in claim 48, including the step of enclosing the preform in a jacket prior to drawing the fibre.

50. A method as claimed in any of claims 46 to 49, in which in at least some of the rods the inner region has a first refractive index and the outer region has a second, different refractive index.

51. An optical fibre comprising a composite material according to any of claims 1 to 42.

52. An optical fibre as claimed in claim 51 and being a photonic crystal fibre.

53. A fibre amplifier comprising a fibre according to claim 51 or claim 52.

54. A fibre laser comprising an amplifier according to claim 53.

55. A method of transmitting light in a composite material according to any of claims 1 to 42.

56. A method of manufacturing an optical material substantially as herein described with reference to the accompanying drawings.

57. An optical material substantially as herein described with reference to the accompanying drawings.