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CN1317098A - Radially nonuniform and azimuthally asymmetric optical fiber - Google Patents

Radially nonuniform and azimuthally asymmetric optical fiber Download PDF

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Publication number
CN1317098A
CN1317098A CN99810742A CN99810742A CN1317098A CN 1317098 A CN1317098 A CN 1317098A CN 99810742 A CN99810742 A CN 99810742A CN 99810742 A CN99810742 A CN 99810742A CN 1317098 A CN1317098 A CN 1317098A
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core
refractive index
sector
waveguide
radius
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V·A·巴加万吐拉
R·M·霍克
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Corning Inc
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Corning Inc
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B37/00Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
    • C03B37/01Manufacture of glass fibres or filaments
    • C03B37/012Manufacture of preforms for drawing fibres or filaments
    • C03B37/01205Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
    • C03B37/01211Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments by inserting one or more rods or tubes into a tube
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B37/00Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
    • C03B37/01Manufacture of glass fibres or filaments
    • C03B37/012Manufacture of preforms for drawing fibres or filaments
    • C03B37/01205Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
    • C03B37/01211Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments by inserting one or more rods or tubes into a tube
    • C03B37/01222Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments by inserting one or more rods or tubes into a tube for making preforms of multiple core optical fibres
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B37/00Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
    • C03B37/01Manufacture of glass fibres or filaments
    • C03B37/012Manufacture of preforms for drawing fibres or filaments
    • C03B37/01205Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
    • C03B37/01225Means for changing or stabilising the shape, e.g. diameter, of tubes or rods in general, e.g. collapsing
    • C03B37/01228Removal of preform material
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B37/00Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
    • C03B37/01Manufacture of glass fibres or filaments
    • C03B37/012Manufacture of preforms for drawing fibres or filaments
    • C03B37/01205Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
    • C03B37/01225Means for changing or stabilising the shape, e.g. diameter, of tubes or rods in general, e.g. collapsing
    • C03B37/01228Removal of preform material
    • C03B37/01231Removal of preform material to form a longitudinal hole, e.g. by drilling
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • G02B6/02295Microstructured optical fibre
    • G02B6/02314Plurality of longitudinal structures extending along optical fibre axis, e.g. holes
    • G02B6/02319Plurality of longitudinal structures extending along optical fibre axis, e.g. holes characterised by core or core-cladding interface features
    • G02B6/02338Structured core, e.g. core contains more than one material, non-constant refractive index distribution in core, asymmetric or non-circular elements in core unit, multiple cores, insertions between core and clad
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B2203/00Fibre product details, e.g. structure, shape
    • C03B2203/10Internal structure or shape details
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B2203/00Fibre product details, e.g. structure, shape
    • C03B2203/10Internal structure or shape details
    • C03B2203/12Non-circular or non-elliptical cross-section, e.g. planar core
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B2203/00Fibre product details, e.g. structure, shape
    • C03B2203/10Internal structure or shape details
    • C03B2203/22Radial profile of refractive index, composition or softening point
    • C03B2203/29Segmented core fibres
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B2203/00Fibre product details, e.g. structure, shape
    • C03B2203/32Eccentric core or cladding
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B2203/00Fibre product details, e.g. structure, shape
    • C03B2203/34Plural core other than bundles, e.g. double core
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • G02B6/036Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
    • G02B6/03616Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
    • G02B6/03638Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 3 layers only
    • G02B6/03644Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 3 layers only arranged - + -

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
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  • Manufacturing & Machinery (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Organic Chemistry (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Integrated Circuits (AREA)
  • Manufacture, Treatment Of Glass Fibers (AREA)
  • Knitting Of Fabric (AREA)

Abstract

揭示了一种单模波导纤维,和一种制造单模或多模波导纤维的方法,其中所述波导纤维具有方位角和径向不对称的纤芯。此不对称性为形成具有特定性能的波导提供了附加的自由度。

A single-mode waveguide fiber and a method for manufacturing single-mode or multimode waveguide fibers are disclosed, wherein the waveguide fiber has a core with azimuth and radial asymmetry. This asymmetry provides additional degrees of freedom for forming waveguides with specific properties.

Description

The asymmetric optical fiber of radially nonuniform and azimuthally
Background of invention
The present invention is based on the U.S. Provisional Application of submitting on September 9th, 1,998 60/099,535.We require the priority date of this application.
The present invention relates to a kind of optical fiber and a kind of methods for optical fiber manufacture, the refractive index distribution curve of described optical fiber radially with the position angle two changes of direction.The additional adaptability of giving along azimuthal variation provides such refractive index distribution curve design, promptly with refractive index only radially coordinate direction situation about changing compare, these designs can be satisfied more waveguide fiber performance requirement.
The waveguide fiber that the index distribution of recent development radially changes footpath demonstrates, and can optimize guide properties by regulating this distribution curve.For example with the simple step mode of a kind of ratio more generally mode change refractive index distribution curve, this change allows to select the value of one or more guide properties under the situation of not sacrificing one group of basic characteristic (decay, intensity or bending resistance).
In addition, the asymmetric fiber core refractive index distribution in some position angle (having the distribution of ellipse, triangle or square fibre core geometric configuration such as those) demonstrates, and they can provide the waveguide performance of usefulness, such as keeping or mixed polarized pattern.
Therefore, expectation along the position angle and radially the fiber core refractive index distribution curve of two changes of direction can offer an opportunity make be suitable in telecommunications, signal Processing or sensing system, using, have new or through the waveguide of improvement performance.
In the United States Patent (USP) 3,909,110 of authorizing Marcuse (being called for short ' 110 patents), a kind of multimode waveguide has been described, its fibre core relative bearing is asymmetric.Calculating in ' 110 patents shows, refractive index radially produces Mode Coupling with the cyclical variation meeting of position angle both direction, thereby increases the loss because of being coupled and producing with radial mode of bandwidth, restriction simultaneously.This notion does not extend to single mode waveguide.The scope of patent is also only limited to sinusoidal azimuthal variation in addition, ' 110.
Describe present position angle and radially during asymmetric fibre core, introducing the notion of fibre core sector.A fibre core sector is the part of fibre core, and it is limited by the track that forms first and second radius point of annulus in the waveguide.Two radiuses differ from one another, and are less than or equal to fiber core radius.The residue border of sector is at angle two planes each other, and each plane all comprises the center line of waveguide fiber.Refractive index is meant to have the refractive index difference of two points on this straight line at least along the variation of a straight line in the sector.
Definition
Below definition meets the conventional usage of this area.
-segmented core is a kind of fibre core that has specific refractive index in the layering of preliminary election radius.A particular hierarchical has the first refractive index point and last refractive index point.Radius from the waveguide core line to the first refractive index point position is the inside radius of core region or fibre core layering.Equally, from the waveguide core line to the end the radius of refractive index point position be the external radius of fibre core layering.
-relative index of refraction Δ, it is defined by following formula: Δ=(n 1 2-n 2 2)/2n 1 2, wherein, n 1Be the largest refractive index of refractive index layering 1, and n 2Be with reference to refractive index, in this application, it is the minimum refractive index of covering.Term " Δ % " is used in this area, and it is 100 * Δ.
-term " refractive index distribution curve " is meant, in the relation between Δ % or refractive index and the radius on the fibre core one selected part.Term " α distribution curve " is meant, satisfies the refractive index distribution curve of following equation:
n(r)=n 0(1-Δ[r/a] α),
Wherein r is a fiber core radius, the definition of Δ as above, a is the last point of distribution curve, r locates to be chosen as zero first of distribution curve, and α is the index that limits profile shape.Other refractive index distribution curve comprises the step change type refractive index of step change type refractive index, trapezoidal refractive index and band fillet, wherein generally causes owing to alloy spreads in the fast-changing zone of refractive index with fillet.
Summary of the invention
In a first aspect of the present invention, the fibre core of single mode waveguide has a sector at least.In the sector outside more at least refractive index and the sector more at least refractive index different.When the sector just in time is half fibre core, can selects to constitute in the sector part of any arbitrarily, and not lose the accuracy of distribution curve definition.The fiber core refractive index distribution curve changes along at least a portion of a radius, produces radially asymmetric.On the radius of a preliminary election, the fiber core refractive index in the sector is different with the fiber core refractive index outside the sector, thereby provides the position angle asymmetric.
In one embodiment, whole fibre core is a cylinder symmetric, and therefore radius r, position angle φ and the center line height z of being convenient to cylindrical coordinates describes.The preliminary election radius part Δ r that refractive index changes is at 0<Δ r≤r 0Scope in, r wherein 0It is fiber core radius.At least be that different preliminary election radius is in this same scope for two different orientations refractive indexes.
In another embodiment, the preliminary election radius partly is layering Δ r=r2-r1, wherein 0≤r 1<r 2, and r 2<r 0
In another embodiment, refractive index is along any or all change in radius in the sector, and the included angle of described sector is greater than zero degree, but is less than or equal to 180 °.
In another embodiment, the radius part is at 0<Δ r≤r 0Scope in, and position angle φ and the height z have any value, as long as coordinate points (r, φ is z) in core region.
In other embodiment of the present invention, stipulated the number of sector and the Angular Dimension and the radius size of sector, and stipulated the funtcional relationship between radius r and the relative index of refraction Δ %.The example of funtcional relationship is the step change type refractive index distribution curve of α distribution curve, step change type and band fillet, and the trapezoidal profile curve.
In other embodiment of the present invention, waveguide has a segmented core and stated number destination sector, has embedded the vitreum with specific size and shape in some zones of sector.Below described and had three and four sectors and embodiment that have particular fiber cored structure and embedded part.In certain embodiments, embedded part itself has the refractive index structures of layering.
In general, the embodiment of first aspect present invention can be single mode or multimode waveguide fiber.
A second aspect of the present invention is a kind of position angle and method of asymmetric waveguide fiber radially made.This method can be used for making single mode or multimode waveguide fiber.
One embodiment of the present of invention may further comprise the steps: change the shape of wire drawing prefabricated rods, then prefabricated stick drawn wire is become a waveguide fiber with round section.Like this, the shape of prefabricated rods just has been transferred to the cylinder symmetric feature that is comprised in the prefabricated rods, specifically has been transferred to the cylinder symmetric feature of fibre core.The shape of wire drawing prefabricated rods can be used such as any method in the methods such as etching, saw, boring or mill and change.
In an embodiment of this method, change prefabricated rods by formation hole or surface gap in prefabricated rods.Prefabricated rods after the change becomes the waveguide fiber with round section through follow-up wire drawing, make the fibre core of circular symmetry become radially or the position angle asymmetric.
Summary of drawings
Figure 1A is a sectional view, shows the present invention and has the waveguide of central core design or an embodiment of prefabricated rods.
Figure 1B is the refractive index distribution curve of obtaining by the 1B cross section of Figure 1A.
Fig. 1 C is the refractive index distribution curve of obtaining by the 1C cross section of Figure 1A.
Fig. 1 D is a sectional view, shows the present invention and has the waveguide of central core design or an embodiment of prefabricated rods.
Fig. 1 E is the refractive index distribution curve of obtaining by the 1E cross section of Fig. 1 D.
Fig. 1 F is the refractive index distribution curve of obtaining by the 1F cross section of Fig. 1 D.
Fig. 1 G is a sectional view, shows the present invention and has the waveguide of embedding core design or an embodiment of prefabricated rods.
Fig. 2 A is a sectional view, shows to have the waveguide that embeds core design or an embodiment of prefabricated rods.
Fig. 2 B is the refractive index distribution curve of obtaining by the 2B cross section of Fig. 2 A.
Fig. 2 C is a sectional view, shows to have the waveguide that embeds core design or an embodiment of prefabricated rods.
Fig. 2 D is the refractive index distribution curve of obtaining by the 2D cross section of Fig. 2 C.
Fig. 2 E is a sectional view, shows to have the waveguide that embeds core design or an embodiment of prefabricated rods.
Fig. 2 F is a sectional view, shows to have the waveguide that embeds core design or an embodiment of prefabricated rods.
Fig. 3 is a sectional view, shows the novel waveguide or the prefabricated rods that contain the hole.
Fig. 4 A and 4B and 4C and 4D are sectional views, show wire drawing after the prefabricated rods profile pass to fibre core.
Fig. 5 A and 5B are sectional views, show the influence of the hole of prefabricated rods to core shape.
Fig. 6 A and 6B and 7A and 7B show the sectional view of preform core and pipe assembly, and the waveguide to obtaining after the assembly wire drawing.
Fig. 8 A and 8B are sectional views, show the segmented core prefabricated rods of fluting, and the waveguide that obtains after the wire drawing.
Detailed description of the present invention
Breach 4 makes that the fibre core 2 of Figure 1A is that the position angle is asymmetric.In this illustrated novel prefabricated rods or waveguide fiber, the material of breach is identical with the material of covering 6.Figure 1B and Fig. 1 C show the vertical cross-section by fibre core respectively, and have provided the azimuthal variation of step change type refractive index distribution curve width.This specific distribution curve is a radial symmetry.
The prefabricated rods of Fig. 1 D or waveguide cores radially with all be asymmetric on the position angle.In this illustrated novel waveguide or prefabricated rods, fibre core is divided into four sectors.Shown in the sector 1F and 1E that obtain by fibre core, sector, two diagonal angles 8 and 10 is the other side's catoptron picture mutually.In Fig. 1 E, label 16 expression 1E sectors are to dependence radially, and it is band fillet step change type distribution curve or α distribution curve.In Fig. 1 F, the distribution curve 18 of 1F sector is the step change type refractive index distribution curve.Clad section 12 and 14 can comprise any material of refractive index less than adjacent core region.That is to say that the situation that the composition of covering generally only is subjected to fibre core cladding structure guided wave situation rather than radiant light to enter waveguide limits.
Fig. 1 G is according to the complicated structure of an example of novel prefabricated rods and waveguide.In this illustrated waveguide, fibre core or fibre core prefabricated rods 20 comprise a segmented core, and this fibre core has center 22 and adjacent annulus 28,24 and 26.Each district all uses corresponding relative index of refraction Δ %, refractive index distribution curve and is characterized by radius 32,34,36,38 and 40 determined zones.For example, center 22 and annulus 24 comprise separately mixes germanite English glass accordingly, and annulus 28 and 26 comprises quartz, and the relative size in each district is referring to accompanying drawing.The vitreum 30 that embeds is with asymmetric introducing fibre core prefabricated rods, and the refractive index of vitreum 30 is general different with its annular layering that is contacted 24 or 26.
Vitreum 30 can form in the following manner, and for example saw or grinding earlier used such as modes such as depositions to be filled in the container with glass then.The luminous energy that each layering 22,28,24,26 and 30 relative index of refraction and size thereof will determine 20 of fibre cores to deliver distributes.Luminous energy distributes on fibre core prefabricated rods or fibre core 20 and has determined the functional characteristic of waveguide.
In another embodiment of novel prefabricated rods or waveguide, shown in Fig. 2 A, fibre core is made of host glass 50, and host glass 50 has the vitreum 42,44 and 48 of embedding.Vitreum extends in prefabricated rods or the waveguide that obtained by prefabricated stick drawn wire from the beginning to the end.Glass-clad 52 is wrapped in fibre core 50.The refractive index of glass of fiber core 50 is greater than the refractive index of covering 52.Fig. 2 B shows the cross section 2B by an embedded body, and it has the step change type refractive index distribution curve.The size that embeds the sectional area of vitreum 42,44 and 48 can be identical or different, and glass-clad can have many relative orientations relatively.
The structure of Fig. 2 A is made by following method, promptly to prefabricated rods boring, makes the wall in gained hole smooth, and glass dust or rod are inserted in the hole.Another kind method is, with many bar construction fibre cores, then rod inserted in the holding tube, can use or not use insulating glass rod or glass particle.If these rods are combined, so just do not need holding tube with suitable glass isolated material.Surrounding layer can be deposited on the coupling unit, perhaps be made into a pipe, before the wire drawing or during pipe is collapsed on assembly.
Fig. 2 C shows another embodiment, and it comprises host glass and a plurality of embedding vitreum.Here, the general structure of waveguide 54 is similar to the structure of Fig. 2 A, except each embeds the refractive index distribution curve that vitreum 56,58 and 60 all has a segmented core.Fig. 2 D illustration a segmented core distribution curve, it is the cross section by an embedded body, wherein the center has higher relatively Δ %, coated outside two annuluses 62 and 64.In the figure, the Δ % of first ring 62 is less than second ring 64.Be appreciated that each layering all has a radially dependence of selecting from multiple possibility, such as the step change type distribution curve of α distribution curve or band fillet, and can regulate the relative Δ % of each layering, so that different waveguide functional characteristics to be provided.
The manufacture method of prefabricated rods or waveguide shown in Fig. 2 C manufacture method with prefabricated rods shown in Fig. 2 A or waveguide in fact is identical.
Fig. 2 E and Fig. 2 F show two other embodiment of this prefabricated rods or waveguide type.Embedding vitreum 66,68 and 70 among Fig. 2 E has the cross section of rectangle, and is arranged in the drift angle of equilateral triangle substantially.Also attempted embedding Vitrea other and arranged, such as diameter arrangement along core region.Core region 72 can comprise many kinds of shapes and form very much.In the simple case shown in Fig. 2 E, glass of fiber core 72 is step change type refractive index distribution curves, and presses the leaded light needs, and its refractive index is at least greater than the part of covering 74.
In Fig. 2 F, show a kind of five Vitrea structures of embedding that comprise.Here, four vitreums 76,78,80 and 82 with diamond-shaped cross-section are made the symmetry layout about circular central core region 84.Clearly, this design can have many kinds to change.For example, embedded body 76,78,80,82 and 84 refractive index can have the relative index of refraction different with fibre core 86.
As shown in Figure 3, the embedded body 88 in prefabricated rods or the waveguide can be the hole.The waveguide that has elongated hole along major axis can be made by forming elongated hole, for example forms by boring or etching in fibre core or the wire drawing prefabricated rods.The refractive index of glass of fiber core 90 must be different from the refractive index in hole, and asymmetric core region is provided thus.In wire drawing prefabricated rods shown in Figure 3, can be collapsed in the hole, to produce asymmetric fibre core.The shape of core region is decided by the relative viscosity of core material 90 and clad material 92 after collapsing in the hole.By control prefabricated rods in just by the thermograde of the part of wire drawing, can keep to the glass relative viscosity control.Relative viscosity also depends on the composition of fibre core and cladding glass.
Fig. 4 A and Fig. 4 B show the shape 98 that makes prefabricated rods among Fig. 4 A and pass to the core segment 102 of the waveguide 100 that obtains through prefabricated rods 98 wire drawings Fig. 4 B from the clad section 94 of prefabricated rods.When the symmetry of the initial symmetry of preform core and waveguide covering 104 was identical, the transmission shown in Fig. 4 A and Fig. 4 B took place.Shown cylinder symmetric among the figure, because this is and the present prefabricated rods manufacturing symmetry the most compatible with drawing process.Other symmetry also is fine, and for example the shape with prefabricated rods partly passes to the waveguide cores shape, i.e. the net shape stray circle cylindrical symmetry of waveguide.
Fig. 4 C shows the cross section of square segmented core prefabricated rods.After becoming cylindrical waveguide to the prefabricated rods heating and with its wire drawing, the segmented core 106 among Fig. 4 D is got square, because core material generation drag flow, to adapt to the cylindrical surface of covering.
Use similar mode, when the prefabricated stick drawn wire that has fibre core 110, covering 112 and elongated hole 108 in Fig. 5 A becomes cylindrical waveguide, it will produce asymmetric fibre core.But in this case, prefabricated rods is columniform, and core material fills up the hole during can Yin Lasi and is moved.As long as keep the shape of prefabricated rods when prefabricated stick drawn wire is become waveguide, fibre core will inevitably be out of shape, and promptly becomes asymmetric, to fill up the hole.
For example
With the prefabricated rods type shown in the outside vapor deposition process shop drawings 5A.Core region 110 is to mix germanite English, and covering 112 is quartzy.By boring, make hole wall smooth with etching solution then, in prefabricated rods, form hole 108.Prefabricated stick drawn wire is become a waveguide fiber, and its zero-dispersion wavelength is in the operation window of 1500nm, even waveguide generation dispersion shift.Compare with having the dispersion shift waveguide in 7 μ m to 8 mu m ranges of azimuthal symmetry fibre core and mode field diameter, this waveguide has very large mode field diameter 10.4 μ m.
Fig. 6 A and Fig. 6 B show the manufacture method of asymmetric fibre core.Make segmented core prefabricated rods 114,116 and 118 with any method in several known methods, described known method comprises OVD, axial vapor deposition method, plasma deposition processes or modified chemical vapor deposition method.The fibre core prefabricated rods is inserted in the pipe 122, in pipe 122, prefabricated rods is kept in position with spacer rod 120.Spacer rod can be made by quartz, doping quartz etc.If desired, covering 124 can be deposited on the pipe.Now, the wire drawing of prefabricated rods assembly can be become a waveguide fiber, shown in Fig. 6 B, its fibre core 130,132 and 134 is embedded in the glass of fiber core 128, and is wrapped in by glass-clad 126.Can directly carry out wire drawing to the assembly shown in Fig. 6 A.Another kind method is, before wire drawing, with the covering consolidation of deposition.In addition, before the deposition covering, can fully heat, make its surface softening, cause to each other to stick together, thereby form more stable structure, so that in surrounding layer or drawing process, use to pipe, fibre core prefabricated rods and spacer rod assembly.
Method shown in the manufacture method of the asymmetric fibre core shown in Fig. 7 A and Fig. 7 B and Fig. 6 A and Fig. 6 B is closely related.In Fig. 7 A, fibre core is encircled 136 and is being retrained, and ring 136 can make light propagate in step change type refractive index fibre core prefabricated rods 138,140 and 142 better.As mentioned above, can stablize the relative position of fibre core prefabricated rods in ring with spacer rod or glass dust.Can be directly to the assembly wire drawing of fibre core prefabricated rods, selectable isolated material, ring and outsourcing layer, perhaps elder generation is with assembly consolidation, wire drawing then.Fig. 7 B shows resulting waveguide fiber.
Fig. 8 A and 8B show the manufacture method of last routine asymmetric fibre core.In Fig. 8 A, the segmented core of prefabricated rods has center 144, first annulus 146 and second annulus 148.Prefabricated rods is passed through technologies such as grinding and cut, forms groove 152.These grooves can be empty, perhaps fill up material 150, and material 150 is different from the composition of covering 154.To the wire drawing of prefabricated rods assembly, form a waveguide, it has the asymmetric fibre core shown in Fig. 8 B.Here, can perhaps before wire drawing, deposit directly with the assembly wire drawing equally, consolidation or positioning step, so that each parts in the prefabricated rods keep suitable relative positioning.
Although in this announcement with describe specific embodiment of the present invention, the present invention is only limited by the accompanying Claim book.

Claims (29)

1.一种单模光纤,它具有径向和方位角不对称的纤芯,其特征在于,包括:1. A single-mode optical fiber having a radially and azimuthally asymmetric core, characterized in that it comprises: 纤芯区,它与周围的包层接触,纤芯区中至少一部分的折射率大于包层中至少一部分的折射率;a core region in contact with the surrounding cladding, at least a portion of the core region having a higher refractive index than at least a portion of the cladding; 波导的中心线平行于波导的长度方向,并且波导至少有一个由第一和第二平面限定的纤芯扇区,并且第一和第二平面在外围与纤芯区的一个分层相交,其中第一和第二平面都包含中心线并且在中心线处形成一夹角φ≤180°,The centerline of the waveguide is parallel to the length direction of the waveguide, and the waveguide has at least one core sector defined by first and second planes, and the first and second planes intersect a layer of the core area at the periphery, wherein Both the first and second planes contain the centerline and form an included angle φ≤180° at the centerline, 纤芯折射率沿一预选半径的至少一部分Δr变化,所述预选半径部分垂直于中心线向外延伸;并且the core refractive index varies along at least a portion Δr of a preselected radius extending outward perpendicular to the centerline; and 在所述至少一个纤芯扇区内的一预先半径上至少有一点的纤芯折射率不同于所述至少一个纤芯扇区外的该预选半径上至少一点的纤芯折射率值。The core refractive index at least one point on a predetermined radius within the at least one core sector is different from the core refractive index value at least one point on the preselected radius outside the at least one core sector. 2.如权利要求1所述的单模波导,其特征在于,纤芯区是圆柱形,并且纤芯区中的点具有柱面坐标,即半径r、方位角φ和中心线高度z,并且纤芯区的半径为r=r0,并且预选半径部分在0<Δr≤r0的范围内。2. A single-mode waveguide as claimed in claim 1, wherein the core region is cylindrical, and points in the core region have cylindrical coordinates, i.e. radius r, azimuth φ and center line height z, and the core The radius of the zone is r=r 0 , and the preselected radius portion is in the range of 0<Δr≤r 0 . 3.如权利要求2所述的单模波导,其特征在于,预选半径部分是分层Δr=r2-r1,其中0≤r1<r2,而r2<r03. 2. The single mode waveguide of claim 2, wherein the preselected radius portion is a layer Δr=r 2 -r 1 , where 0 ≤ r 1 <r 2 and r 2 <r 0 . 4.如权利要求2或3所述的单模波导,其特征在于,预选半径部分沿着至少一个扇区中的任何一个半径,所述至少一个扇区的夹角为0<φ≤180°。4. The single-mode waveguide according to claim 2 or 3, wherein the preselected radius portion is along any radius in at least one sector, and the included angle of said at least one sector is 0<φ≤180°. 5.如权利要求2所述的单模波导,其特征在于,预选半径部分Δr在0<Δr≤r0的范围内,该半径的方位角在0<φ≤360°的范围内,并且该半径从中心线上的任何一点z画出。5. The single-mode waveguide according to claim 2, characterized in that, the preselected radius part Δr is in the range of 0< Δr≤r0 , the azimuth angle of the radius is in the range of 0<φ≤360°, and the radius is from Any point z on the centerline is drawn. 6.如权利要求2所述的单模波导,其特征在于,预选半径部分是分层Δr=r2-r1,其中0≤r1<r2,而r2≤r0,包含该分层的半径方位角在0<φ≤360°的范围内,并且包含该分层半径从中心线上的任何一点z画出。6. A single-mode waveguide as claimed in claim 2, characterized in that the preselected radius portion is a layer Δr=r 2 -r 1 , where 0≤r 1 <r 2 , and r 2 ≤r 0 , including the The radius azimuth angle is in the range of 0<φ≤360°, and the layered radius is drawn from any point z on the center line. 7.如权利要求2所述的单模波导,其特征在于,纤芯具有四个等体积的扇区,它们按逆时针方位角方向依次编号为1-4,每个扇区的边界面都呈90°的夹角,并且扇区1和扇区3具有函数f(r)限定的折射率径向变化,而扇区2和扇区4具有函数g(r)限定的折射率径向变化。7. The single-mode waveguide according to claim 2, wherein the fiber core has four sectors of equal volume, which are numbered 1-4 in the counterclockwise azimuth direction, and the boundary surface of each sector is 90° °, and Sector 1 and Sector 3 have a radial change in refractive index defined by the function f(r), while Sector 2 and Sector 4 have a radial change in refractive index defined by the function g(r). 8.如权利要求7所述的单模波导,其特征在于,g(r)是阶跃型折射率,而f(r)是α分布曲线。8. 7. The single mode waveguide of claim 7 wherein g(r) is the step index and f(r) is the alpha profile. 9.如权利要求2所述的单模波导,其特征在于,纤芯具有4个等体积的扇区,每个扇区的边界面都呈90°的夹角,并且每个扇区的折射率分布曲线都具有一中心部分,其半径为rc,相对折射率为Δc,并且在限定该扇区的平面之间延伸,9. The single-mode waveguide according to claim 2, wherein the fiber core has 4 sectors of equal volume, the boundary surfaces of each sector are at an angle of 90°, and the refractive index distribution of each sector is The curves each have a central portion with radius rc and relative index of refraction Δc and extend between the planes defining the sector, 第一环形区,它与中心部分接触,它具有外半径r1、相对折射率Δ1,并且在限定扇区的平面之间延伸,a first annular region, which is in contact with the central portion, has an outer radius r 1 , a relative refractive index Δ 1 , and extends between planes defining the sector, 第二环形区,它与第一环形区接触,它具有外半径r2、相对折射率Δ2,并且在限定扇区的平面之间延伸,a second annular region in contact with the first annular region, having an outer radius r 2 , a relative refractive index Δ 2 , and extending between planes defining the sector, 第三环形区,它与第二环形区接触,它具有外半径r3、相对折射率Δ3,并且在限定扇区的平面之间延伸,a third annular region in contact with the second annular region, having an outer radius r 3 , a relative refractive index Δ 3 , and extending between planes defining the sector, 第一体积,它具有恒定的折射率,镶嵌在第一扇区的纤芯中,并且限定该扇区的第一平面的一部分限定了其表面的第一部分,而第一、第二和第三环形区的一部分限定了其表面的第二部分,The first volume, which has a constant refractive index, is embedded in the core of the first sector, and part of the first plane defining the sector defines a first part of its surface, while the first, second and third a portion of the annular region defines a second portion of its surface, 第二体积,它具有恒定的折射率,镶嵌在第一扇区的纤芯中,并且限定该扇区的第二平面的一部分限定了其表面的第一部分,而第一、第二和第三环形区的一部分限定了其表面的第二部分,其中The second volume, which has a constant refractive index, is embedded in the core of the first sector, and part of the second plane defining the sector defines the first part of its surface, while the first, second and third A portion of the annular region defines a second portion of its surface, wherein 剩余的三个扇区都包含嵌入体,这些嵌入体表面的限定方式对应于第一扇区内嵌入的体积,其中各相对折射率和半径满足以下不等式:The remaining three sectors all contain embeddings whose surfaces are defined in a manner corresponding to the volume embedded within the first sector, where the respective relative indices of refraction and radii satisfy the following inequalities: 0≤rc<r1<r2<r3≤r0,并且Δc≥Δ2>Δ1≥Δ3 。0≤r c <r 1 <r 2 <r 3 ≤r 0 , and Δ c ≥Δ 21 ≥Δ 3 . 10.如权利要求2所述的单模波导,其特征在于,纤芯具有三个扇区,每个扇区都包括具有恒定折射率的第一玻璃体,第一玻璃体镶嵌在具有恒定折射率的第二玻璃体中,其中第一玻璃的折射率大于第二玻璃的折射率。10. The single-mode waveguide of claim 2, wherein the core has three sectors, each sector comprises a first glass body with a constant refractive index, the first glass body is embedded in a second glass body with a constant refractive index. A glass body in which the refractive index of a first glass is greater than that of a second glass. 11.如权利要求10所述的单模波导,其特征在于,每个第一玻璃体都是一细长体,其长轴平行于中心线,其中细长体的垂直截面选自以下形状组成的组:圆、椭圆和平行四边形。11. The single-mode waveguide of claim 10, wherein each first glass body is an elongated body with a long axis parallel to the centerline, wherein the vertical cross-section of the elongated body is selected from the group consisting of: Circles, ellipses and parallelograms. 12.如权利要求2所述的单模波导,其特征在于,纤芯具有三个扇区,每个扇区都包括一细长的玻璃体,该玻璃体具有中心部分、第一环形部分和至少一个附加环形部分,其中第一环形部分包裹并接触中心部分,而至少一个附加环形部分接触并包裹环形部分,每个细长结构的长轴都平行于中心线。12. The single mode waveguide of claim 2, wherein the core has three sectors, each sector comprising an elongated glass body having a central portion, a first annular portion and at least one additional annular portion A portion wherein a first annular portion wraps around and contacts the central portion and at least one additional annular portion touches and wraps around the annular portion, each elongated structure having a major axis parallel to the centerline. 13.如权利要求12所述的单模波导,其特征在于,中心部分是一圆柱体,其半径为rc,折射率为Δc,环形部分是管子,其外半径分别为ri,折射率为Δi,其中i=1…n,n是环形部分的数目,并且i为偶数时的Δi大于i为奇数时的Δi13. A single-mode waveguide as claimed in claim 12, wherein the central part is a cylinder with radius r c and refractive index Δ c , and the annular part is a tube with outer radii r i and refractive index Δ i , where i=1...n, n is the number of annular parts, and Δ i when i is even is larger than Δ i when i is odd. 14.如权利要求2所述的单模波导,其特征在于,纤芯具有四个扇区,每个扇区都包括第一玻璃体,第一玻璃体的相对折射率为Δ1,并且嵌入每个扇区第一玻璃体中的是一个细长的、相对折射率为Δ2的第二玻璃体,其中各细长体相对中心线对称布置。14. The single-mode waveguide of claim 2, wherein the core has four sectors, each sector comprising a first glass body having a relative refractive index Δ1 embedded in each sector Within the first glass body is an elongated second glass body with a relative refractive index Δ2 , wherein each elongated body is arranged symmetrically with respect to the center line. 15.一种用于制造径向和方位角不对称的单模或多模光纤的方法,其特征在于,包括以下步骤:15. A method for manufacturing radially and azimuthally asymmetric single-mode or multimode optical fibers, comprising the steps of: a)制造单模或多模光纤预制棒,所述预制棒具有长轴、纤芯和包层,其中预制棒垂直于长轴的任何截面都是圆形的;a) making a single-mode or multimode optical fiber preform, said preform having a major axis, a core and a cladding, wherein any section of the preform perpendicular to the major axis is circular; b)研磨、锯掉或者去除预制棒的周边部分,改变预制棒的表面,致使预制棒垂直于长轴的任何截面的形状实质上与预制棒垂直于长轴的任何其它截面的形状相同;b) grinding, sawing or removing peripheral portions of the preform, altering the surface of the preform so that any section of the preform perpendicular to the major axis has substantially the same shape as any other section of the preform perpendicular to the major axis; c)对预制棒加热,并沿其长轴将其拉丝成一波导纤维,该波导纤维具有纤芯、长轴,并且在长轴的任何一点上都具有垂直于长轴的圆形截面,从而提供了具有改变后预制棒之形状的波导纤芯。c) heating the preform and drawing it along its major axis into a waveguide fiber having a core, a major axis, and at any point on the major axis a circular cross-section perpendicular to the major axis, thereby providing A waveguide core with a modified preform shape is obtained. 16.如权利要求15所述的方法,其特征在于,步骤b)包括下述步骤,即在预制棒表面形成一个或多个缺口。16. The method of claim 15, wherein step b) includes the step of forming one or more indentations in the surface of the preform. 17.如权利要求16所述的方法,其特征在于,制造步骤a)包括下述步骤,即制造一分层纤芯预制棒,该预制棒具有中心纤芯区和至少一个包裹并接触中心纤芯区的环形部分,其中中心区的相对折射率不同于环形部分的相对折射率,并且至少有一个或多个缺口渗透到环形部分中。17. The method of claim 16, wherein manufacturing step a) includes the step of manufacturing a layered core preform having a central core region and at least one wrapping and contacting the central core region wherein the relative refractive index of the central region is different from that of the annular portion, and at least one or more notches penetrate into the annular portion. 18.一种用于制造径向和方位角不对称的单模或多模波导的方法,其特征在于,包括以下步骤:18. A method for manufacturing a radially and azimuthally asymmetric single-mode or multimode waveguide, characterized in that it comprises the steps of: a)制造一光纤预制棒,所述预制棒具有长轴、纤芯和包层,其中预制棒垂直于长轴的任何截面都是圆形的;a) manufacturing an optical fiber preform, said preform having a major axis, a core and a cladding, wherein any section of the preform perpendicular to the major axis is circular; b)在波导预制棒中钻出、磨出或者制作出一个或多个延长轴延伸的孔;b) drilling, milling or fabricating one or more elongated axis-extending holes in the waveguide preform; c)对预制棒加热,并沿其长轴将其拉丝成一波导纤维,该波导纤维具有纤芯、长轴,并且在长轴的任何一点上都具有垂直于长轴的圆形截面,从而提供了径向和方位角不对称的波导纤芯。c) heating the preform and drawing it along its major axis into a waveguide fiber having a core, a major axis, and at any point on the major axis a circular cross-section perpendicular to the major axis, thereby providing A waveguide core with radial and azimuthal asymmetry. 19.一种用于制造径向和方位角不对称的单模或多模光纤的方法,其特征在于,包括以下步骤:19. A method for manufacturing radially and azimuthally asymmetric single-mode or multimode optical fibers, comprising the steps of: a)制造至少两根光纤预制棒,每根预制棒都具有一长轴;a) making at least two optical fiber preforms, each preform having a major axis; b)将至少两根纤芯预制棒插入由包层玻璃制成的管子中,形成一个具有长轴的纤芯预制棒-管子组件,其中在至少两个纤芯预制棒的边界之间和管子的内部形成填隙孔;b) inserting at least two core preforms into a tube made of cladding glass to form a core preform-tube assembly having a major axis, wherein between the boundaries of the at least two core preforms and the tube Filling holes are formed inside; c)对组件加热,并沿其长轴将其拉丝成一波导纤维,该波导纤维具有纤芯、长轴,并且在长轴的任何一点上都具有垂直于长轴的圆形截面,从而提供了具有径向和方位角不对称纤芯的波导纤维。c) heating the assembly and drawing it along its major axis into a waveguide fiber having a core, a major axis, and at any point on the major axis a circular cross-section perpendicular to the major axis, thereby providing Waveguide fibers with radially and azimuthally asymmetric cores. 20.如权利要求19所述的方法,其特征在于,在步骤c)之前还包括下述步骤,即将包层玻璃插入在至少两个纤芯预制棒和管子之间形成的填隙孔内,其中所述包层玻璃的形状选自由以下物质形成的组:粒子、棒和微球体。20. The method of claim 19, further comprising the step of inserting cladding glass into interstitial holes formed between at least two core preforms and the tube before step c), wherein the The shape of the cladding glass is selected from the group formed by particles, rods and microspheres. 21.如权利要求19所述的方法,其特征在于,制造步骤a)包括下述步骤,即制造一分层纤芯预制棒,该预制棒包括中心纤芯区和至少一个包裹并接触中心纤芯区的环形部分,其中中心区的相对折射率不同于环形部分的相对折射率。twenty one. The method of claim 19, wherein step a) of making comprises the step of making a layered core preform comprising a central core region and at least one wrapping and contacting the central core region The annular portion, wherein the relative refractive index of the central region is different from the relative refractive index of the annular portion. 22.一种多模光纤,它具有径向和方位角不对称的纤芯,其特征在于,包括:twenty two. A multimode optical fiber having a radially and azimuthally asymmetric core, characterized in that it comprises: 纤芯区,它与周围的包层接触,纤芯区中至少一部分的折射率大于包层中至少一部分的折射率;a core region in contact with the surrounding cladding, at least a portion of the core region having a higher refractive index than at least a portion of the cladding; 波导的中心线平行于波导的长度方向,并且波导有四个纤芯扇区,每个扇区都由第一和第二平面限定,并且第一和第二平面在外围与纤芯区的一个分层相交,其中第一和第二平面都包含中心线并且在中心线处形成一夹角φ≤180°,The center line of the waveguide is parallel to the length direction of the waveguide, and the waveguide has four core sectors, each sector is defined by the first and second planes, and the first and second planes are in the periphery with one of the core areas intersecting in layers, where the first and second planes both contain the centerline and form an angle φ≤180° at the centerline, 纤芯区为圆柱形,并且纤芯区上的一点具有柱面坐标,即半径r,方位角φ以及中心线高度z,并且纤芯区的半径为r=r0,并且折射率沿半径部分Δr变化,而Δr在0<Δr≤r0的范围内,其中The core area is cylindrical, and a point on the core area has cylindrical coordinates, that is, radius r, azimuth φ, and centerline height z, and the radius of the core area is r=r 0 , and the refractive index is along the radius part Δr changes, and Δr is in the range of 0<Δr≤r 0 , where 四个纤芯扇区体积相等,按逆时针方位角方向依次编号为1-4,并且每个扇区的边界面都呈90°的夹角,并且扇区1和扇区3具有函数f(r)限定的折射率径向变化,而扇区2和扇区4具有函数g(r)限定的折射率径向变化。The volumes of the four core sectors are equal, and they are numbered 1-4 in the counterclockwise azimuth direction, and the boundary surfaces of each sector form an angle of 90°, and sector 1 and sector 3 have a function f( r) defines a radial variation of the refractive index, while sectors 2 and 4 have a radial variation of the refractive index defined by the function g(r). 23.如权利要求22所述的波导,其特征在于,g(r)是阶跃型折射率,而f(r)是α分布曲线。twenty three. 22. The waveguide of claim 22 wherein g(r) is the step index and f(r) is the alpha profile. 24.如权利要求22所述的波导,其特征在于,四个纤芯扇区具有相等的体积,每个扇区的边界面都呈90°的夹角,每个扇区的折射率分布曲线都具有一中心部分,其半径为rc,相对折射率为Δc,并且在限定该扇区的平面之间延伸,twenty four. The waveguide according to claim 22, wherein the four core sectors have equal volumes, the boundary surfaces of each sector form an included angle of 90°, and the refractive index profile of each sector has a central portion having radius r c and relative index of refraction Δ c extending between the planes delimiting the sector, 第一环形区,它与中心部分接触,它具有外半径r1、相对折射率Δ1,并且在限定扇区的平面之间延伸,a first annular region, which is in contact with the central portion, has an outer radius r 1 , a relative refractive index Δ 1 , and extends between planes defining the sector, 第二环形区,它与第一环形区接触,它具有外半径r2、相对折射率Δ2,并且在限定扇区的平面之间延伸,a second annular region in contact with the first annular region, having an outer radius r 2 , a relative refractive index Δ 2 , and extending between planes defining the sector, 第三环形区,它与第二环形区接触,它具有外半径r3、相对折射率Δ3,并且在限定扇区的平面之间延伸,a third annular region in contact with the second annular region, having an outer radius r 3 , a relative refractive index Δ 3 , and extending between planes defining the sector, 第一体积,它具有恒定的折射率,镶嵌在第一扇区的纤芯中,并且限定该扇区的第一平面的一部分限定了其表面的第一部分,而第一、第二和第三环形区的一部分限定了其表面的第二部分,The first volume, which has a constant refractive index, is embedded in the core of the first sector, and part of the first plane defining the sector defines a first part of its surface, while the first, second and third a portion of the annular region defines a second portion of its surface, 第二体积,它具有恒定的折射率,镶嵌在第一扇区的纤芯中,并且限定该扇区的第二平面的一部分限定了其表面的第一部分,而第一、第二和第三环形区的一部分限定了其表面的第二部分,其中The second volume, which has a constant refractive index, is embedded in the core of the first sector, and part of the second plane defining the sector defines the first part of its surface, while the first, second and third A portion of the annular region defines a second portion of its surface, wherein 剩余的三个扇区都包含嵌入体,这些嵌入体表面的限定方式对应于第一扇区内嵌入的体积,其中各相对折射率和半径满足以下不等式:The remaining three sectors all contain embeddings whose surfaces are defined in a manner corresponding to the volume embedded within the first sector, where the respective relative indices of refraction and radii satisfy the following inequalities: 0≤rc<r1<r2<r3≤r0,并且Δc≥Δ2>Δ1≥Δ30≤r c <r 1 <r 2 <r 3 ≤r 0 , and Δ c ≥Δ 21 ≥Δ 3 . 25.如权利要求22所述的波导,其特征在于,四个纤芯扇区都包括第一玻璃体,第一玻璃体的相对折射率为Δ1,并且嵌入每个扇区第一玻璃体中的是一个细长的、相对折射率为Δ2的第二玻璃体,其中各细长体相对中心线对称布置。25. The waveguide of claim 22, wherein each of the four core sectors includes a first glass body having a relative refractive index Δ 1 , and embedded in the first glass body of each sector is a thin An elongated second glass body with a relative refractive index Δ2 , wherein each elongated body is arranged symmetrically with respect to the center line. 26.一种多模光纤,它具有径向和方位角不对称的纤芯,其特征在于,包括:26. A multimode optical fiber having a radially and azimuthally asymmetric core, characterized in that it comprises: 纤芯区,它与周围的包层接触,纤芯区中至少一部分的折射率大于包层中至少一部分的折射率;a core region in contact with the surrounding cladding, at least a portion of the core region having a higher refractive index than at least a portion of the cladding; 波导的中心线平行于波导的长度方向,并且波导有四个纤芯扇区,每个扇区都由第一和第二平面限定,并且第一和第二平面在外围与纤芯区的一个分层相交,其中第一和第二平面都包含中心线并且在中心线处形成一夹角φ≤180°,其中The center line of the waveguide is parallel to the length direction of the waveguide, and the waveguide has four core sectors, each sector is defined by the first and second planes, and the first and second planes are in the periphery with one of the core areas layered intersection, wherein both the first and second planes contain the centerline and form an angle φ≤180° at the centerline, where 纤芯区为圆柱形,并且纤芯区上的一点具有柱面坐标,即半径r,方位角φ以及中心线高度z,并且纤芯区的半径为r=r0,并且折射率沿半径部分Δr变化,而Δr在0<Δr≤r0的范围内,其中The core area is cylindrical, and a point on the core area has cylindrical coordinates, that is, radius r, azimuth φ, and centerline height z, and the radius of the core area is r=r 0 , and the refractive index is along the radius part Δr changes, and Δr is in the range of 0<Δr≤r 0 , where 纤芯具有三个扇区,每个扇区都包括具有恒定折射率的第一玻璃体,第一玻璃体镶嵌在具有恒定折射率的第二玻璃体中,其中第一玻璃的折射率大于第二玻璃的折射率。The core has three sectors, each sector includes a first glass body with a constant refractive index, the first glass body is embedded in a second glass body with a constant refractive index, where the first glass has a higher refractive index than the second glass refractive index. 27.如权利要求26所述的波导,其特征在于,每个第一玻璃体都是一细长体,其长轴平行于中心线,其中细长体的垂直截面选自以下形状组成的组:圆、椭圆和平行四边形。27. The waveguide of claim 26, wherein each first glass body is an elongated body with a long axis parallel to the centerline, wherein the vertical cross-section of the elongated body is selected from the group consisting of: circular, Ellipse and parallelogram. 28.如权利要求26所述的波导,其特征在于,三个纤芯扇区都包括一细长的玻璃体,该玻璃体具有中心部分、第一环形部分和至少一个附加环形部分,其中第一环形部分包裹并接触中心部分,而至少一个附加环形部分接触并包裹环形部分,每个细长结构的长轴都平行于中心线。28. The waveguide of claim 26, wherein each of the three core sectors comprises an elongated glass body having a central portion, a first annular portion and at least one additional annular portion, wherein the first annular portion wraps and contacting the central portion, and at least one additional annular portion contacting and surrounding the annular portion, each elongated structure having a major axis parallel to the centerline. 29.如权利要求28所述的波导,其特征在于,中心部分是一圆柱体,其半径为rc,折射率为Δc,环形部分是管子,其外半径分别为ri,折射率为Δi,其中i=1…n,n是环形部分的数目,并且i为偶数时的Δi大于i为奇数时的Δi29. The waveguide of claim 28, wherein the central portion is a cylinder having a radius r c and a refractive index Δ c , and the annular portion is a tube having outer radii r i and a refractive index Δ i , where i=1...n, n is the number of annular parts, and Δ i when i is even is greater than Δ i when i is odd.
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CN107017548A (en) * 2015-12-04 2017-08-04 恩耐公司 Using the optical mode filter of radially asymmetric optical fiber
CN110114320A (en) * 2016-12-28 2019-08-09 住友电气工业株式会社 Method for manufacturing fibre-optical preform

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CN107017548B (en) * 2015-12-04 2020-07-17 恩耐公司 Optical Mode Filters Using Radially Asymmetric Fibers
CN105500719A (en) * 2016-01-28 2016-04-20 北京交通大学 Method for manufacturing terahertz waveguide preform by means of 3D printing technology
CN110114320A (en) * 2016-12-28 2019-08-09 住友电气工业株式会社 Method for manufacturing fibre-optical preform
CN110114320B (en) * 2016-12-28 2021-11-30 住友电气工业株式会社 Method for manufacturing optical fiber preform

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