Large effective area waveguide fiber

Abstract: A single mode optical waveguide fiber having a segmented core designed to provide a large effective area for light transmission. The large effective area reduces waveguide fiber non-linearities. The inventive waveguide is thus suited for transmission of high power signals over long distances. Embodiments of the inventive single mode waveguide including five core segments are given triple clad with central index dip, quadruple clad with central index dip, alpha profile with pedestal, alpha profile with additional high index ring, and quadruple clad with depressed cladding. The large effective area is achieved with essentially no degradation in optical or mechanical performance of the waveguide.

Description: Background The invention relates to a single mode optical waveguide fiber having a large effective area, A eff , for light transmission. The large effective area reduces non-linear optical effects, including self phase modulation, four wave mixing, cross phase modulation, and non-linear scattering processes, which can cause degradation of signals in high power systems. In general, a mathematical description of these non-linear effects includes the ratio, P/A eff , where P is optical power. For example, a non-linear optical effect usually follows an equation containing a term, exp [PxL eff /A eff ], where L eff is effective length. Thus, an increase in A eff produces a decrease in the non-linear contribution to the degradation of a light signal. The requirement in the telecommunication industry for greater information capacity over long distances, without regenerators, has led to a reevaluation of single mode fiber index profile design. The focus of this reevaluation has been to provide optical waveguides which: reduce non-linear effects such as those noted above; are optimized for the lower attenuation operating wavelength range around 1550 nm; are compatible with optical amplifiers; and, retain the desirable properties of optical waveguides such as high strength, fatigue resistance, and bend resistance. A waveguide fiber, having at least two distinct refractive index segments was found to have sufficient flexibility to meet and exceed the criteria for a high performance waveguide fiber system. The genera of segmented core designs are disclosed in detail in U. S. patent 4,715,679, Bhagavatula. Species of the profiles disclosed in the '679 patent, having properties especially suited for particular high performance telecommunications systems, are disclosed in applications S.N. 08/323,795 and S.N. 08/287,262. The present invention is yet another core index profile species which reduces non-linear effects and which is particularly suited to transmission of high power signals over long distances without regeneration. The definition of high power and long distance is meaningful only in the context of a particular telecommunication system wherein a bit rate, a bit error rate, a multiplexing scheme, and perhaps optical amplifiers are specified. There are additional factors, known to those skilled in the art, which have impact upon the meaning of high power and long distance. However, for most purposes, high power is an optical power greater than about 10 mw. For example, a long distance is one in which the distance between electronic regenerators can be in excess of 100km. Considering the Kerr non-linearities, i.e., self phase modulation, cross phase modulation and four wave mixing, the benefit of large A eff can be shown from the equation for refractive index. The refractive index of silica based optical waveguide fiber is known to be non-linear with respect to the light electric field. The refractive index may be written as, n = n o + n 2 P/A eff ,where n o is the linear refractive index, n 2 is the non-linear index coefficient, P is light power transmitted along the waveguide and A eff is the effective area of the waveguide fiber. Because n 2 is a constant of the material, increase in A eff is essentially the only means for reducing the non-linear contribution to the refractive index, thereby reducing the impact of Kerr type non-linearities. Thus there is a need for an optical waveguide fiber designed to have a large effective area. The window of operation of greatest interest at this time is that near 1550 nm. Definitions - The effective area is A eff = 2π (∫E 2 r dr) 2 /(∫E 4 r dr), where the integration limits are 0 to ∞, and E is the electric field associated with the propagated light. An effective diameter, D eff , may be defined as, A eff = Π (D eff /2) 2 An alpha profile is n = n o (1 -Δ(r/a) α ), where n o is the refractive index at the first point of the alpha index profile, Δ is defined below, r is radius, and a is the radius measured from the first to the last point of the alpha index profile, and r is chosen to be zero at the first point of the alpha index profile. The width of an index profile segment is the distance between two vertical lines drawn from the respective beginning and ending points of the index profile to the horizontal axis of the chart of refractive index vs. radius. The % index delta is % Δ = [(n 1 2 - n c 2 )/2n 1 2 ] x 100, where n 1 is a core index and n c is the clad index. Unless otherwise stated, n 1 is the maximum refractive index in the core region characterized by a % Δ. A tapered step index profile, is a step index profile which has been modified by dopant diffusion during the waveguide fiber manufacturing process. The dopant diffusion causes the substantially right angles at the top and bottom of the step to become rounded and the sides of the step to be tapered. The amount of diffusion depends upon several variables including the details of the process steps and upon the initial height and width of the step index profile. The exact amount of taper is not a critical determinant of the waveguide fiber properties herein discussed. However, a general description of degree of taper may be given. A Sharply tapered step is one in which the width at half the % Δ is in the range of about 30 to 50% of the base width and the width at 0.9 of the % Δ is in the range of about 15 to 25% of the base width. A moderately tapered step is one in which the width at half the % Δ is in the range of about 60 to 80 % of the base width and the width at 0.9 of the % Δ is in the range of about 35 to 50% of the base width. The index profiles discussed herein, in general, are in the ranges of sharply or moderately tapered profiles. However, the invention is not limited to profile segments having a particular degree of taper. A number of known optical fibres make use of segmented core designs to achieve certain desired waveguide fibre properties. Examples of these are disclosed in the articles entitled "Attenuation-Optimised Dispersion-Flattened Quadruple-Clad fibres with moderate F-doping in the first inner cladding " by Yangsheng Gao et al published in IEE Photonics Technology Letters (1992) June, no. 6, New York, "Low-Loss Dispersion-Shifted Single-Mode fibre manufactured by the OVD process" by T. D. Croft et al published in the Journal of Lightwave Technology, volume 3 LT-3, no. 5 October 1985 and, "Dispersion-Shifted Segmented-Core Single-Mode fibres" by Bhagavatula et al published in Optics Letters, volume 9, no. 5 May 1984. Each of these references shows that segmented refractive index profiles offer waveguide fibres that can exhibit a desired set of waveguide fibre properties. Summary of the Invention This invention meets the need for a waveguide fibre having an index profile tailored for high performance operation in the 1550 nm window while maintaining a relatively large effective transmission area. It is noteworthy that a large effective area is achieved while maintaining good bend resistance. The invention relates to a single mode waveguide fiber having an operating range from about 1500 nm to 1600 nm. A waveguide designed for operation in this wavelength range may be called a dispersion shifted waveguide. That is, the zero of total dispersion lies in range of about 1500 nm to 1600 nm. The waveguide has a core glass region comprising segments surrounded by a clad glass layer of refractive index n c . The index profiles of the segments comprising the core region are tailored to provide an effective area of at least 70 microns 2 . (For simplicity the S.I. unit "micrometre" is denoted herein by its commonly used abbreviation "micron".) The fiber has a centerline which is the axis of symmetry along the length of the fiber, and is characterized in that said core region comprises a central segment of minimum refractive index n 0 , a first annular segment, adjacent said central segment, said first segment having a tapered step index profile of maximum refractive index n 1 , a second annular segment, adjacent said first annular segment, having a lower substantially constant refractive index n 2 , and a third annular segment, adjacent said second annular segment having a tapered step index profile of maximum index n 3 , wherein n 1 >n 3 >n 0 >n 2 , said refractive index profile being configured to provide a total dispersion zero outside the limits from 1540 nm to 1557 nm and an effective area greater than 70 micrometers 2 at near 1550 nm. In a first embodiment, the core region comprise three annular segments. The first annular segment is a tapered step index profile having a maximum % Δ and a width, measured at the base of the step. The exact amount of taper and the shape of the top of the index profile, whether triangular or uneven, is in general not of critical importance. Unless expressly stated otherwise, all widths are measured at the base of a particular core segment. The first annular segment surrounds an index depression, forming a central segment, on the waveguide centerline, i.e., the line of symmetry along the long waveguide fiber axis. This depression approximates the shape of an inverted cone. The central depression is due to the well known dopant loss by diffusion. It is also well known that process differences can increase or decrease the size of this central depression. However, with proper process the central depression can be held relatively constant from waveguide to waveguide. In general, this central depression is not cylindrically symmetric. A second annular segment, adjacent the first annular segment, has a substantially constant % Δ and a width. A third annular segment, adjacent the second annular segment, has a tapered step index profile and a width. The geometry and % Δ range, of each core segment, which together provide an A eff greater than about 70 microns 2 , are given in example 1. A second embodiment of the invention comprises a core region having four segments. The central segment has a substantially constant refractive index n o and a radius. A first annular segment, adjacent the central segment, has a tapered step index profile of maximum refractive index n 1 and a width. A second annular segment, adjacent the first annular segment, has a substantially constant refractive index n 2 and a width. A third annular region, adjacent the second annular region, has a tapered step index profile of maximum index n 3 and a width. The relationship among the indexes is n 1 > n 3 > n o > n 2 . The detailed description of this embodiment is given in example 2. A third embodiment of the invention comprises a core region having five segments. The central core segment is cylindrically symmetrical and has a substantially constant refractive index n o and a radius. A first annular segment, adjacent the central core segment, has a tapered step index profile of maximum refractive index n 1 and a width. A second annular segment, adjacent the first annulus, has a substantially constant refractive index n 2 and a width. A third annular segment, adjacent the second annulus, has a tapered step index profile of maximum index n 3 and a width. A fourth annular segment, adjacent the third annulus, has a substantially constant refractive index n 4 and a width. The relations among the indexes are, n 1 > n 3 >n o ≥ n c , and both n 2 and n 4 < n c . The appropriate ranges of refractive indexes and profile geometries which yield an A eff greater than 70 microns 2 and given in example 4. The refractive index profile is chosen to provide an A eff greater than about 70 microns 2 , and preferably a zero total dispersion greater than 1560 nm and a dispersion slope less than about 0.09 ps/nm 2 -km. This remarkable combination of properties may be achieved using a refractive index profile such as those found in several of the examples below. Brief Description of the Drawings FIG. 1 is a modelled index profile showing a segment core region having a central index depression. FIG. 2 is a modelled index profile showing a four segment core region. FIG. 3 is a modelled index profile showing a five segment core region wherein two of the segments have a refractive index lower than the clad refractive index. FIG. 4 is a chart comparing the calculated effective diameter of the index profile of FIG. 3 compared to the mode field diameter calculated for the profile of FIG. 3. Detailed Description of the Invention The segmented core design has been shown to be sufficiently flexible to meet a wide range of waveguide fiber specifications as is shown in the patent and patent applications referenced above. Changing the shape and location of the refractive index profiles of the segments of a core region, changes the mode power distribution of the propagating light and the waveguide dispersion. Combining a pre-selected waveguide dispersion with a material dispersion allows one to obtain a wide range of shapes and magnitudes for the total or chromatic dispersion of the waveguide. Thus, one can change the location of the total dispersion zero or alter the magnitude or slope of the total dispersion over a pre-selected wavelength range. In addition, changing the mode power distribution produces changes in mode field diameter, bend resistance and effective area for light transmission. In general, the mode power distribution and the shape of the waveguide dispersion, cannot be changed completely independently. The variables which define the segmented core structure must be adjusted to obtain the best trade off of properties for a given telecommunication system application. Of the essentially infinite number of possible segmented core designs, a design is sought which provides the desired values for: zero dispersion wavelength; cut off wavelength; magnitude and sign of total dispersion for a pre-selected wavelength range; slope of total dispersion over a pre-selected wavelength range; effective area; and, bend resistance. It is assumed that other essential properties such as maximum attenuation over a pre-selected wavelength range, fatigue resistance and strength are not affected by the core region segmented profile. The feature of particular importance in the inventive segmented core waveguide is the effective area of the waveguide. As noted above, increasing effective area for transmission of light, decreases the deleterious non-linear effects. A series of segmented core designs have been found, which increase effective area by about 40 % relative to waveguides designed for use in the dispersion shifted window, 1500 nm to 1600 nm, and having analogous index profile shapes. In general, the increase in A eff is greater than 40%. A typically effective area for a dispersion shifted waveguide is about 50 microns 2 . The inventive segmented profiles provide an effective area of at least 70 microns 2 . As will be seen in the following embodiments, the effective area can be made much larger than 70 microns 2 while maintaining acceptable bend resistance. The compromise which is made in the index profile design involves the size and position of the profile segments. A segment having a relatively high maximum refractive index and positioned away from the waveguide centerline will tend to broaden the light power distribution, thereby increasing the effective transmission area. However, as the light power distribution is broadened, the resistance of the waveguide fiber to bend loss decreases. The inventive waveguide fiber provides good bend resistance and larger A eff . Example 1 - Four Segment Core The index profile illustrated in FIG. 1 shows a first annular index profile 2 , which is essentially a tapered step index profile, surrounded by a substantially flat profile region 4 . The index depression on the waveguide centerline, 6 , is due to diffusion during preform processing and can be considered as a central index profile segment. The maximum % Δ 10 may have a value in the range of about 0.8 to 0.95 % and may be located in a radius range of about 1.5 to 2.5 microns. The minimum % Δ of the centerline depression 6 is typically in the range of about 0 to 0.4 %. Region 6 is roughly the shape of an inverted cone having a base radius, drawn from the index peak 10 to the centerline, of about 1 to 1.75 microns. The annulus 4 has a % Δ of essentially zero and a width in the range of about 3.5 to 4 microns. The annulus 12 has a maximum % Δ, 8 , in the range of about 0.40 to 0.55 % and is located in the radius range of about 6.5 to 7.5 microns. The width of annulus 12 is in the range of about 1 to 1.7 microns. The properties of this design are: A eff about 75 microns 2 ; Dispersion zero about 1562; and LP 11 cut off about 1590 nm. The properties of this design can be modified by shifting the location of the center of segment 2 outward by about 0.15 microns. The properties of the design then are: A eff , about 86 microns 2 ; Dispersion zero about 1531 nm; and, LP 11 cut off about 1598 nm. Note that the cut off wavelength is measured on the waveguide fiber before cabling. In general, the cabling process decreases the cut off wavelength by an amount greater than about 200 nm. Example 2 - Four Segment Core The core shown in FIG. 2 has segments 14, 16, 18, and 20. Segment 14 is a cylindrically symmetric step index profile of refractive index n 0 . Annular segment 16, adjacent segment 14, has a tapered step index profile of maximum refractive index n 1 . Annular segment 18, adjacent annular segment 16, has a substantially constant refractive index n 2 . Annular segment 20, adjacent annular segment 16 has a tapered step index profile of maximum index n 3 . The relationship of these indexes are n 1 > n 3 > n 0 > n 2 , as can be seen from the figure. Segment 14 has a radius no greater than about 1 micron and a % index Δ no greater than about 0.4 %. Annular segment 16 , has a width no greater than about 2.5 microns and a maximum % index Δ in the range of about 0.8 to 1 %. This maximum occurs at a radius in the range of about 1.5 to 2 microns. Annular segment 18 has a width in the range of about 2.5 to 4 microns and n 2 is about equal to n c . Annular segment 20 has a width in the range of about 1.5 to 2.5 microns and a maximum % Δ in the range of about 0.45 to 0.75. This maximum occurs at a radius in the range of about 6.5 to 7.5 microns. The effective area of the core is about 78 microns 2 as compared to an effective area of about 52 microns 2 for standard dispersion shifted waveguide fiber, having this segmented core configuration. The power distribution is shown by line 22 . The additional effective area of the core index profile shown in FIG. 2, relative to standard dispersion shifted fiber, is a result of the higher % Δ of annulus 20 , which shifts power away from the waveguide center. Referring now to FIG. 4 note that the effective diameter, line 50 , is larger than the mode field diameter, line 52 , over the wavelength range of at least 1200 nm to 1700 nm. This may indicate that D eff is more descriptive of the mode power distribution than is the mode field diameter for refractive index profiles of this type. Example 3-Five Segment Depressed Index The refractive index profile of FIG 3 shows a cylindrically symmetric central segment, 32 , having a substantially constant index n 0 . The first annular segment 34 , adjacent segment 32, has a tapered step index profile of maximum refractive index n 1 . The second annular segment 36 , adjacent annular segment 34 , has a substantially constant index n 2 . The third annular segment 38 , adjacent annular segment 36 , has a tapered step index profile of maximum refractive index n 3 . The fourth annular segment 40 , adjacent annular segment 38 , has a substantially constant index n 4 . The relationship among the indexes, as can be seen in FIG. 3 is n 1 > n 3 > n 0 ≥ n c and both n 2 and n 4 < n c . Central segment 32 has a % Δ in the range of about 0.1 to 0.15 % and a radius in the range of about 0.5 to 1 micron. Annular segment 34 has a maximum % Δ in the range of about 0.7 to 0.85 %, located in the radius range from about 1.5 to 2.5 microns, and a width in the range of 1 to 2.5 microns, Annular segment 36 has a substantially constant % Δ in the range of about -0.1 to -0.2 % and a width in the range of about 3.5 to 4.5 microns. Annular segment 38 has a maximum % Δ in the range of about 0.55 to 0.7 % located in the radius range of about 7 to 9 microns and a width in the range of about 1.75 to 2.5 microns. Annular segment 40 has a substantially constant % Δ in the range of about -0.1 to -0.2 % and a width in the range of about 5 to 7 microns. This index profile is calculated to have an effective area of about 72.4 microns 2 as well as a dispersion zero of about 1564 nm and a dispersion slope of about 0.08 ps/nm 2 -km. The LP 11 cut off is about 1564 and the predicted bend resistance is good. This design clearly provides a superior waveguide fiber for use in a high performance telecommunication system using high intensity producing optical amplifiers and wavelength division multiplexing. Flexibility of this design can be seen from the following comparative calculations. Segment 34 , is made about 0.2 microns wider at the base. Segment 36 is made about 0.3 microns wider. Segment 38 is made about 0.15 microns wider. The resulting index profile provides an effective area of about 79.5 microns 2 , a dispersion zero of about 1563 nm and a dispersion slope of about 0.08 ps/nm 2 -km. The LP 11 cut off is 1628 nm as measured on the uncabled waveguide fiber. As is noted above, the cut off wavelength decreases by at least 200 nm in most cable designs. In a second comparative calculation, segment 32 is decreased by about 0.2 microns, segment 36 decreased by about 0.15 microns and segment 38 increased in base width by about 1 micron. The resulting waveguide fiber has an effective area of about 120 microns 2 , a dispersion zero of 1540 nm and a dispersion slope of 0.11 ps/nm 2 -km.

Claims: A single mode optical waveguide fiber which reduces non-linear effects and is dispersion shifted for use over a wavelength range of 1500 nm to 1600 nm comprising: a core region comprising segments, each said segment having a refractive index profile; and, a clad layer, having refractive index n c , surrounding said core region: said single mode wavelength fiber having a centerline which is the axis of symmetry along the length of said waveguide fiber, characterized in that said core region comprises a central segment of minimum refractive index n 0 , a first annular segment, adjacent said central segment, said first segment having a tapered step index profile of maximum refractive index n 1 , a second annular segment, adjacent said first annular segment, having a lower substantially constant refractive index n 2 , and a third annular segment, adjacent said second annular segment having a tapered step index profile of maximum index n 3 , wherein n 1 >n 3 >n 0 >n 2 , said refractive index profile being configured to provide a total dispersion zero outside the limits from 1540 nm to 1557 nm and an effective area greater than 70 micrometers 2 at near 1550 nm. The single mode waveguide fiber of claim 1, wherein said core region includes: a first annular tapered step index segment having a maximum % Δ in the range of 0.8 % to 0.95 %, said step index segment having a centerline index depression of minimum % Δ index in the range of 0 to 0.4 % as a central segment, a second annular segment, adjacent said first annular segment, having a substantially constant % Δ of about 0, and, a third annular segment, adjacent said second annular segment, having a tapered step index shape and a maximum % Δ in the range of 0.40 % to 0.55 %. The single mode waveguide fiber of claim 2, wherein the maximum % Δ of said first annular segment is located within the radius range of 1.5 to 2.5 µm and the maximum % Δ of said third annular segment is located within the radius range of 6.5 to 7.5 µm, wherein the radius to the outer edge of said first annular segment is in the range of 1.75 to 2.5 µm and the widths of said second annular segment, and of said third annular segment are in the range of about 3.5 to 4 µm, and 1 to 1.7 µm respectively, and, wherein said centerline index depression is essentially an inverted cone having a base radius in the range of 1 to 1.75 µm. The single mode waveguide fiber of claim 1, wherein said central segment has a radius no greater than 1 µm and a % index Δ no greater than 0.4%, said first annular segment has a width no greater than about 2.5 µm and a % index Δ in the range of 0.8 to 1%, said second annular segment has a width in the range of 2.5 to 4 µm and n 2 is about equal to n c , and, said third annular segment has a width in the range of 1.5 to 2.5 µm and a % Δ in the range of 0.45 to 0.75. The single mode waveguide fiber of any one of claims 1 to 4, wherein the zero dispersion wavelength of the fiber lies in the range 1500 nm to 1600 nm. The single mode waveguide fiber of claim 1, wherein the second annular segment has a maximum index n 2 , and the fiber further comprises a fourth cladding segment surrounding the third annular segment having a maximum index n 4 , wherein n 1 > n 3 > n 2 and wherein n 2 is substantially equal to n 4 . The single mode waveguide fiber of any one of claims 1 to 6, exhibiting a fiber cutoff wavelength between 1564 nm and 1628nm. The single mode waveguide fiber of claim 1, wherein said central segment is cylindrically symmetric having substantially constant refractive index n 0 , further comprising a fourth annular segment, adjacent said third annular segment, having a substantially constant refractive index n 4 , wherein, n 1 > n 3 > n 0 ≥ n c and both n 2 and n 4 < n c . The single mode fiber of claim 8, wherein said central segment has a % Δ in the range of 0.1 to 0.15% and a radius in the range of 0.5 to 1 µm, said first annular segment has a maximum % Δ in the range of 0.7 to 0.85%, located in the radius range from 1.5 to 2.5 µm, and a width in the range of 1 to 2.5 µm, said second annular segment has a substantially constant % Δ in the range of -0.1 to -0.2% and a width in the range of 3.5 to 4.5 µm, said third annular segment has a maximum % Δ in the range of 0.55 to 0.7% located in the radius range of 7 to 9 µm and a width in the range of 1.75 to 2.5 µm, and, said fourth annular segment has a substantially constant % Δ in the range of -0.1 to -0.2% and a width in the range of 5 to 7 µm.

Inventors: LIU YANMING, NEWHOUSE MARK A, LIU, YANMING, NEWHOUSE, MARK A., Liu, Yanming, c/o Corning Incorporated, Newhouse, Mark A., c/o Corning Incorporated
Applicants: CORNING INC, CORNING INCORPORATED
Application year: 1996
Main classification: G02B6
IPC codes: G02B6