Patent Grant
8953917
The present invention relates to optical fibers having low bend losses.
There is a need for low bend loss optical fibers, particularly for optical fibers utilized in so-called “access” and fiber to the premises (FTTx) optical networks. Optical fiber can be deployed in such networks in a manner which induces bend losses in optical signals transmitted through the optical fiber. Some fiber applications that can impose physical demands such as tight bend radii, or compression of optical fiber, etc., that induce fiber bend losses. The requirements that impose these demands include, for example, the deployment of optical fiber in optical drop cable assemblies, distribution cables with Factory Installed Termination Systems (FITS) and slack loops, small bend radius multiports located in cabinets that connect feeder and distribution cables, and jumpers in Network Access Points between distribution and drop cables. It has been difficult in some single mode optical fiber designs to achieve both low bend loss at both large and small bends at the same time.
For example, single mode optical fibers with a low index trench in the cladding are being used for making fibers with low bend loss performance. These fibers have a trench where the depth of the trench is relatively constant across the width of the trench. In these designs, while the performance of the fiber at smaller diameters (˜10 mm mandrel diameter) is excellent (<0.25 dB/turn), the performance at large diameters (˜30 mm mandrel diameter) is not as good as in other bend optimized fibers that have been optimized for larger bend diameters. To improve the bend performance at both small and larger bend radii, fiber designs that include multiple trenches have been proposed. However, such an approach results in additional steps during processing and makes making of the fiber more costly.
According to some embodiments a single mode optical fiber includes:
a central core region having outer radius r1 and a relative refractive index delta Δ1max;
a cladding region comprising (i) a first inner cladding region having an outer radius r2>6 microns and a relative refractive index delta Δ2 and 0.3≦r1/r2≦0.85; (ii) and a second inner cladding region having an outer radius r3>9 microns and comprising a minimum relative refractive index delta Δ3min, wherein said second cladding region has at least one region with a relative refractive index delta that becomes more negative with increasing radius; and (iii) an outer cladding region surrounding the inner cladding region and comprising relative refractive index delta Δ4, wherein Δ1max>Δ2>Δ3min, Δ3min<Δ4;
According to some embodiments, disclosed herein are optical fibers comprising a central core region having outer radius r1 and a maximum relative refractive index delta Δ1max, a cladding comprising a first inner cladding region having an outer radius r2>8 microns and a relative refractive index delta Δ2, a second inner cladding region having a relative refractive index delta Δ3 and a minimum relative refractive index delta Δ3min, wherein Δ1>Δ2>Δ3min, such that the difference between Δ2 and Δ3min is greater than 0.15%, and an outer cladding region surrounding the two inner cladding regions. The fibers embodiments disclosed herein preferably exhibit a 22 m cable cutoff less than or equal to 1260 nm, a mode field diameter (MFD) at 1310 nm between 8.2 and 9.6 microns and a zero wavelength dispersion between 1300 and 1324 nm. In at least some fibers embodiments r1/r2 is greater than or equal to 0.25, more preferably greater than 0.3. Preferably |Δ4−Δ2|≧0.01.
According to some other embodiments a single mode optical fiber includes:
a germania doped central core region having outer radius r1, peak (maximum) relative refractive index delta in the central core region of Δ1,max; and the core region having a refractive index alpha profile, αcore, with αcore between 1 and 100 (and for example, 1.8≦αcore≦100; 1.8≦αcore≦2.2; 2≦αcore≦100; 5≦αcore≦100; 2≦αcore≦20, or 5≦αcore≦20);
a cladding region comprising (i) a first inner cladding region having an outer radius r2>6 microns and relative refractive index Δ2 and 0.3≦r1/r2≦0.85; (ii) and a second inner cladding region having an outer radius r3>9 microns and comprising a minimum relative refractive index delta Δ3min, wherein said second cladding region has at least one region with a relative refractive index delta that becomes more negative with increasing radius; and (iii) an outer cladding region surrounding the inner cladding region and comprising relative refractive index Δ4, wherein Δ1>Δ2>Δ3, Δ3<Δ4.
Disclosed herein are optical fiber embodiments comprising a central core region having outer radius r1 and a maximum relative refractive index delta Δ1, a cladding region comprising a first inner cladding region having an outer radius r2>8 microns and a relative refractive index delta Δ2, and a second inner cladding region surrounding the first inner cladding region and having relative refractive index Δ3, wherein Δ1 max>Δ2>Δ3min, and Δ2−Δ3min is ≧0.15. The fibers disclosed herein preferably exhibit a 22 m cable cutoff less than or equal to 1260 nm, a mode field diameter (MFD) at 1310 nm between 8.2 and 9.6 microns and a zero wavelength dispersion between 1300 and 1324 nm. In these fibers some embodiments r1/r2 is greater than or equal to 0.25, more preferably greater than 0.3. Preferably, |Δ4−Δ2|≧0.01.
Applicants discovered having a fiber with a trench that has a non-constant relative refractive index delta helps in achieving good macrobending performance at both small (<10 mm) and large (>20 mm) diameters. The following single mode fiber embodiments have an offset trench with a non-constant relative refractive index delta that decreases with an increasing radius in at least a region thereof, resulting in low macrobend loss and opticals (optical performance parameters) that are ITU-G.652 standards compliant. In at least some embodiments the index in the second inner cladding region decreases with increasing radial position.
In at least some embodiments the shape of the trench is defined by the parameter
is the average index slope in the second inner cladding region that is determined by averaging the index slope at different radial locations between R2 and R3. In some embodiments, the parameter β is greater than 0.25, more preferably greater than 0.5 and even more preferably greater than 0.75. Preferably β<1.5. For fiber embodiments with a triangular trench the value of parameter β is 1.
In at least some embodiments αt≦50, where is a trench alpha parameter. For some embodiments 0.5≦αt≦5.
The moat volume ratio, V3a3ratio, is defined as follows:
V3a3ratio=V3a3/[Δ3min(r32−r22)]
Preferably the optical fibers herein have a moat volume ratio of 0.3≦V3a3ratio≦0.8.
Reference will now be made in detail to the present preferred embodiments, examples of which are illustrated in the accompanying drawings.
Additional features and advantages will be set forth in the detailed description which follows and will be apparent to those skilled in the art from the description or recognized by practicing as described in the following description together with the claims and appended drawings.
The “refractive index profile” is the relationship between refractive index or relative refractive index and optical fiber radius. The radius for each segment of the relative refractive index profile is given by the abbreviations r1, r2, r3, r4, etc. and lower an upper case are used interchangeability herein (e.g., r1 is equivalent to R1).
The “relative refractive index percent” is defined as Δ %=100×(ni2−nc2)/2ni2, and as used herein nc is the average refractive index of the outer cladding region and unless otherwise specified is the refractive index of pure silica. As used herein, the relative refractive index is represented by Δ and its values are given in units of “%”, unless otherwise specified. The terms: relative refractive index delta, delta, Δ, Δ %, % Δ, delta %, % delta and percent delta may be used interchangeability herein. In cases where the refractive index of a region is less than the average refractive index of the outer cladding, the relative index percent is negative and is referred to as having a depressed region or depressed index. In cases where the refractive index of a region is greater than the average refractive index of the outer cladding region, the relative index percent is positive. An “updopant” is herein considered to be a dopant which has a propensity to raise the refractive index relative to pure undoped SiO2. A “downdopant” is herein considered to be a dopant which has a propensity to lower the refractive index relative to pure undoped SiO2. Examples of updopants include GeO2 (germania), Al2O3, P2O5, TiO2, Cl, Br. Examples of down dopants include fluorine and boron. For a person skilled in the art, it will be obvious that the relative index profiles disclosed herein can be modified such that entire index profile is shifted linearly up or down relative to the index of pure silica and result in similar optical properties of the resulting optical fibers.
“Chromatic dispersion”, herein referred to as “dispersion” unless otherwise noted, of an optical fiber is the sum of the material dispersion, the waveguide dispersion, and the inter-modal dispersion. In the case of single mode optical fibers the inter-modal dispersion is zero. Zero dispersion wavelength is a wavelength at which the dispersion has a value of zero. Dispersion slope is the rate of change of dispersion with respect to wavelength.
“Effective area” is defined as:
Aeff=2π(∫f2rdr)2/(∫f4rdr),
where the integration limits are 0 to ∞, and f is the transverse component of the electric field associated with light propagated in the optical fiber. As used herein, “effective area” or “Aeff” refers to optical effective area at a wavelength of 1550 nm unless otherwise noted.
The term “α-profile” refers to a relative refractive index profile of the region (e.g., core region), expressed in terms of Δ(r) which is in units of “%”, where r is radius. The α-profile of the core (which is defined by the core alpha, or alphacore herein) follows the equation,
Δ(r)=Δ(ro)(1−[|r−ro|/(r1−ro)]α),
where ro is the point at which Δ(r) is maximum, the radius r is moving radially outward from the centerline, r1 is the radial location at which Δ(r) % first reaches the value 0.03%, and r is in the range ri≦r≦rf, where Δ is defined above, ri is the initial point of the α-profile, rf is the final point of the α-profile, and α is an exponent which is a real number.
The mode field diameter (MFD) is measured using the Peterman II method wherein, 2w=MFD, and w2=(2∫f2r dr/∫[df/dr]2r dr), the integral limits being 0 to ∞.
The bend resistance of an optical fiber can be gauged by induced attenuation under prescribed test conditions, for example by deploying or wrapping the fiber around a mandrel of a prescribed diameter, e.g., by wrapping 1 turn around a either a 6 mm, 10 mm, 20 mm, 30 mm or similar diameter mandrel (e.g. “1×10 mm diameter macrobend loss” or the “1×30 mm diameter macrobend loss”) and measuring the increase in attenuation per turn.
One type of bend test is the lateral load microbend test. In this so-called “lateral load” test (LLWM), a prescribed length of optical fiber is placed between two flat plates. A #70 wire mesh is attached to one of the plates. A known length of optical fiber is sandwiched between the plates and a reference attenuation is measured while the plates are pressed together with a force of 30 Newtons. A 70 Newton force is then applied to the plates and the increase in attenuation in dB/m is measured. The increase in attenuation is the lateral load attenuation of the optical fiber in dB/m at a specified wavelength (typically within the range of 1200-1700 nm, e.g., 1310 nm or 1550 nm or 1625 nm).
Another type of bend test is the wire mesh covered drum microbend test (WMCD). In this test, a 400 mm diameter aluminum drum is wrapped with wire mesh. The mesh is wrapped tightly without stretching, and should have no holes, dips, or damage. Wire mesh material specification: McMaster-Carr Supply Company (Cleveland, Ohio), part number 85385T106, corrosion-resistant type 304 stainless steel woven wire cloth, mesh per linear inch: 165×165, wire diameter: 0.0019″, width opening: 0.0041″, open area (%): 44%. A prescribed length (750 meters) of optical fiber is wound at 1 m/s on the wire mesh drum at 0.050 centimeter take-up pitch while applying 80 (+/−1) grams tension. The ends of the prescribed length of fiber are taped to maintain tension and there are no fiber crossovers. The attenuation of the optical fiber is measured at a specified wavelength (typically within the range of 1200-1700 nm, e.g., 1310 nm or 1550 nm or 1625 nm); a reference attenuation is measured on the optical fiber wound on a smooth drum. The increase in attenuation is the wire mesh covered drum attenuation of the optical fiber in dB/km at a specified wavelength (typically within the range of 1200-1700 nm, e.g., 1310 nm or 1550 nm or 1625 nm).
The “pin array” bend test is used to compare relative resistance of optical fiber to bending. To perform this test, attenuation loss is measured for a optical fiber with essentially no induced bending loss. The optical fiber is then woven about the pin array and attenuation again measured. The loss induced by bending is the difference between the two measured attenuations. The pin array is a set of ten cylindrical pins arranged in a single row and held in a fixed vertical position on a flat surface. The pin spacing is 5 mm, center to center. The pin diameter is 0.67 mm During testing, sufficient tension is applied to make the optical fiber conform to a portion of the pin surface. The increase in attenuation is the pin array attenuation in dB of the optical fiber at a specified wavelength (typically within the range of 1200-1700 nm, e.g., 1310 nm or 1550 nm or 1625 nm).
The theoretical fiber cutoff wavelength, or “theoretical fiber cutoff”, or “theoretical cutoff”, for a given mode, is the wavelength above which guided light cannot propagate in that mode. A mathematical definition can be found in Single Mode Fiber Optics, Jeunhomme, pp. 39-44, Marcel Dekker, New York, 1990 wherein the theoretical fiber cutoff is described as the wavelength at which the mode propagation constant becomes equal to the plane wave propagation constant in the outer cladding. This theoretical wavelength is appropriate for an infinitely long, perfectly straight fiber that has no diameter variations.
Fiber cutoff is measured by the standard 2 m fiber cutoff test, FOTP-80 (EIA-TIA-455-80), to yield the “fiber cutoff wavelength”, also known as the “2 m fiber cutoff” or “measured cutoff”. The FOTP-80 standard test is performed to either strip out the higher order modes using a controlled amount of bending, or to normalize the spectral response of the fiber to that of a multimode fiber.
By cabled cutoff wavelength, or “cabled cutoff” as used herein, we mean the 22 m cabled cutoff test described in the EIA-445 Fiber Optic Test Procedures, which are part of the EIA-TIA Fiber Optics Standards, that is, the Electronics Industry Alliance—Telecommunications Industry Association Fiber Optics Standards.
Unless otherwise noted herein, optical properties (such as dispersion, dispersion slope, etc.) are reported for the LP01 mode.
Applicants discovered that putting an off-set trench with a non-constant depth in the profile of a single mode fiber can simultaneously improve bend performance at both small (≦5 mm) and large (≧10 mm) bend radii. The following fiber embodiments result in low bend performance at small and large bend diameters and have other opticals that are G.652 standards compliant (MFD between 8.2 and 9.6 microns at 1310 nm, a zero dispersion wavelength between 1300 and 1324 nm, cable cutoff wavelength less than or equal to 1260 nm). Optical fibers disclosed herein are capable of exhibiting an effective area at 1310 nm which is between 52 and 72 microns2. Optical fibers disclosed herein are capable of exhibiting an effective area at 1550 nm which is between 75 and 90 microns2.
Preferably MFD (at a wavelength of 1310 nm) of the optical fiber 10 is between 8.2 μm and 9.6 μm. For example, 8.2 microns≦MFD≦ and 9.6 microns, or 8.5 μm≦MFD≦ and 9.4 microns (e.g., 8.6, 8.8, 9, 9.2, 9.4, 9.6 microns, or therebetween).
Several relative refractive index profiles of an exemplary fiber 10 are shown in
In at least some embodiments ατ≦50, where ατ, is a trench alpha parameter. For some embodiments, 0.5≦ατ≦5.
In the exemplary embodiments, Δ1max>Δ2>Δ3min and Δ3min<Δ4. Preferably Δ2−Δ3min≧0.1%; more preferably Δ2−Δ3min≧0.15%, even more preferably Δ2−Δ3≧0.2%. In the embodiments illustrated in
The index of refraction (and thus the relative refractive index delta) of the second inner cladding region 3 (the trench) preferably decreases with increasing radial position. The shape of the second inner cladding region 3 is defined by the parameter
is the average index slope in the second inner cladding region that is determined by averaging the index slope at different radial locations between R2 and R3. For a triangular trench the value of parameter β is 1. For a rectangular trench, the value of parameter β is 0. In other embodiments of optical fiber 10, the parameter β is greater than 0.25, more preferably greater than 0.5 and even more preferably greater than 0.75. Preferably, β is less than 1.5, and more preferably less than 1.1.
Another parameter that can be used to define the trench shape in the second inner cladding region 3 is the parameter, αt, which refers to a relative refractive index profile in the second inner cladding region 3, expressed in terms of Δ(r) which is in units of “%”, where r is radius, which follows the equation,
Δ(r)=Δ3,min(1−[|r3−r|/(r3−r2)]αt),
where αt is the trench alpha parameter. For a rectangular trench, the value of parameter αt is greater than 100, while for a triangular trench the value of parameter αt is 1. Preferably αt≦50. In some embodiments of optical fiber 10, the parameter αt is 0.5≦αt≦5, in some embodiments 0.5≦αt≦3, and in some embodiments 0.75≦αt≦2.
Preferably, according to the exemplary embodiments disclosed herein the optical fibers have the moat volume ratio of 0.3≦V3a3ratio≦0.8, where V3a3ratio, is:
V3a3ratio=V3a3/[Δ3min(r32−r22)]
Central core region 1 comprises an outer radius r1, r1 is the point when the radius r moving radially outward from the centerline corresponds to at the value at which Δ(r) % first reaches 0.03%. Core region 1 (also referred to as a core herein) preferably exhibits a maximum relative refractive index delta percent, Δ1 max, between about 0.3 to 0.5, more preferably between about 0.31 to 0.48, for example between about 0.31 to 0.45. In some embodiments, Δ1max is between 0.31 and 0.43. In some embodiments Δ1max is less than 0.42. Core radius r1 is preferably between 3 and 10 microns, more preferably between about 3.5 to 8.0 microns, for example 3.5≦r1≦7.0 microns, or 3.5≦r1≦5.0 microns. Central core region 1 may comprise a single segment, step index profile. In some embodiments, central core region 1 exhibits an alpha profile with an alpha (αcore) value greater than 0.5 and less than 10, and in some embodiments less than 7.5, less than 5, or less than 3 (for example, between 1.8 and 2.2, such as 1.85, 1.95, 1.98, 2, 2.05, 2.1 or therebetween). However, in other embodiments, central core region 1 may comprise an alpha, αcore between about 2 and about 100; or between 10 and 40, such as 15, 20, 30, or therebetween), and in some cases 5≦alphacore≦20.
In some preferred embodiments, central core region 1 exhibits an 5≦alphacore≦20, and a core region 1 having a relative refractive index delta percent, Δ1 between 0.30 to 0.48 (e.g., 0.32≦Δ1≦0.4). In some preferred embodiments, central core region 1 exhibits an alpha 5≦alphacore≦20, and a core region 1 having a refractive index delta percent, Δ1max between 0.3 to 0.48 (e.g., 0.32≦Δ1≦0.4), and a core radius between about 3.5 to 7 microns. In some preferred embodiments, central core region 1 exhibits an alpha greater than 0.5 and less than 10, and in some embodiments less than 7.5, less than 5, or less than 3, and a core region 1 has a relative refractive index delta percent, Δ1 between 0.30 to 0.48 (e.g., 0.32≦Δ1≦0.4). In some embodiments, central core region 1 exhibits an alpha greater than 0.5 and less than 10, and in some embodiments less than 7.5, less than 5, or less than 3, and a core region 1 having a refractive index delta percent, Δ1max between 0.3 to 0.48 (e.g., 0.32≦Δ1≦0.4), and a core radius between about 3.5 to 7 microns.
In the embodiment illustrated in
Inner cladding region 2 comprises refractive index delta percent Δ2 which is calculated using:
In some embodiments, the first inner cladding region 2 comprises silica which is substantially undoped with either fluorine or germania, i.e., such that the region is essentially free of fluorine and germania. Inner cladding region 3 preferably includes a down-dopant, for example fluorine to provide a minimum relative refractive index delta that is lower than that of region 2. In the embodiments illustrated in
The volume V3 of the second inner cladding region 3 (the trench), is defined as shown in Eq. 2, and given in units of percent delta micron square (% Δmicrons2)
In the embodiments of
Outer cladding region 4 surrounds the depressed annular region 3 and comprises relative refractive index delta percent Δ4 which is higher than the index Δ3 min of inner cladding region 3. In some embodiments outer cladding region 4 has relative refractive index greater than that of first inner cladding region 2, thereby forming a region which is an “updoped” outer cladding region 4 with respect to first inner cladding region 2, e.g. by adding an amount of dopant (such as germania or chlorine) sufficient to increase the relative refractive index of the outer cladding region 4. Note, however, that it is not critical that region 4 be updoped in the sense that an index increasing dopant must be included in region 4. Indeed, the same sort of raised index effect in outer cladding region 4 may be achieved by downdoping first inner cladding region 2 with respect to outer cladding region 4. Outer cladding region 4 comprises a higher relative refractive index than first inner cladding region 2, and may comprises relative refractive index delta percent Δ4 which is greater than 0.01%, and in some embodiments be greater than 0.02% or 0.03%, relative to relative refractive index in the first inner cladding region 2. Preferably, the higher index portion (compared to first inner cladding region 2) of outer cladding region 4 extends at least to the point where the optical power which would be transmitted through the optical fiber is greater than or equal to 90% of the optical power transmitted, more preferably to the point where the optical power which would be transmitted through the optical fiber is greater than or equal to 95% of the optical power transmitted, and most preferably to the point where the optical power which would be transmitted through the optical fiber is greater than or equal to 98% of the optical power transmitted. In many embodiments, this is achieved by having the “updoped” third annular region extend at least to a radial point of about 30 microns. Consequently, the volume V4 of the third annular region 4, is defined herein being calculated between radius r3 and r30 (the radius at 30 microns) and thus is defined as
The volume V4 of the outer cladding region 4 (inside 30 microns) compared to that of the first inner cladding region 2, is preferably greater than 5 Δ % microns2, more preferably greater than 7 Δ % microns2, and may be greater than 10% Δ microns2. This volume V4 of the outer cladding region (inside 30 microns) is in some embodiments less than 50% Δ microns2.
In some embodiments, the relative refractive index Δ4 of the outer cladding region 4 is greater than first inner cladding index Δ2 by 0.01%, more preferably greater than 0.02%. In some embodiments, the outer cladding region 4 comprises chlorine (Cl). In some embodiments the outer cladding region includes germania (GeO2).
The core region 1 preferably has a positive relative refractive index throughout. The core 1 comprises a maximum relative refractive index Δ1MAX occurring between r=0 and r=3 μm. Δ1MAX is preferably between 0.30% and 0.48%, and even more preferably 0.3% to 0.45%.
The first inner cladding region 2 preferably has a substantially constant relative refractive index profile, i.e. the difference between the relative refractive index at any two radii within the intermediate region is less than 0.02%, and in some preferred embodiments less than 0.01%. Thus, the relative refractive index profile of the first inner cladding region 2 preferably has a substantially flat shape. In some embodiments the outer cladding region 4 is updoped relative to pure silica and in some embodiments the first inner cladding region 2 is downdoped relative to pure silica.
The core region 1 may be a step index core, and may comprise an alpha (α) shape. In preferred embodiments, r1 is less than 8.0 microns, and more preferably is between 3.5 microns and 7.0 microns. The fibers are capable of exhibiting mode field diameter at 1310 nm between 8.2 and 9.6 microns, zero dispersion wavelength between 1300 and 1324 nm, cable cutoff less than or equal to 1260 nm and a bend loss of less than 2, and preferably less than 1 dB/turn when wound upon on a 10 mm radius mandrel.
The fibers disclosed herein may be drawn from optical fiber preforms made using conventional manufacturing techniques and using known fiber draw methods and apparatus, for example as is disclosed in U.S. Pat. No. 7,565,820, the specification of which is hereby incorporated by reference.
Various exemplary embodiments will be further clarified by the following examples. It will be apparent to those skilled in the art that various modifications and variations can be made without departing from the spirit or scope of the claims.
Tables 1A, 1B, 2A, 2B, 3-5 below list characteristics of modeled illustrative examples 1-6 and 8-27, manufactured fiber example 7, and those of the two comparative example fibers. In particular, set forth below for each example of Table 1A and 1B is the relative refractive index delta Δ1, alpha, and outer radius r1 of the central core region 1, relative refractive index delta Δ2 and outer radius r2 first inner cladding region 2, relative refractive index delta Δ3 and volume V3 of the second inner cladding region 3, relative refractive index delta Δ4 and volume V4 of the outer cladding region 4, which is calculated between inner radius r3 of outer cladding region 3 and a radial distance of 30 microns, and a moat volume ratio.
Also set forth (Tables 2A, 2B) are modeled data including: theoretical cutoff wavelength in nm, chromatic dispersion and dispersion slope at 1310 nm, chromatic dispersion and dispersion slope at 1550 nm, mode field diameter at 1310 nm and 1550 nm, effective area Aeff at 1550 nm, lateral load wire mesh microbend at 1550 nm, pin array macrobend at 1550 nm, zero dispersion wavelength, 22 m cable cutoff, 1×10 and 1×30 mm diameter induced bend losses in dB per turn at 1550 nm, and kappa value (dispersion D divided by the dispersion slope).
More specifically, the exemplary fiber embodiments Tables 1A, 1B, 2A and 2B have core alpha values between 2 and 20, core radii between about 4 and about 5.5 microns, and 0.3%<Δ1MAX<0.4%. Most of these fiber embodiments have a bend loss of less than 0.5 dB/turn (at 1550 nm) when bent around 10 mm diameter mandrel, and less than 0.01 dB/turn when bent around 30 mm mandrel.
Also set forth (Tables 4, 5 and 6) are modeled data including: theoretical cutoff (LP11) wavelength in nm, chromatic dispersion and dispersion slope at 1310 nm, chromatic dispersion and dispersion slope at 1550 nm, mode field diameter at 1310 nm and 1550 nm, effective area Aeff at 1550 nm, lateral load wire mesh microbend at 1550 nm, pin array macrobend at 1550 nm, zero dispersion wavelength, 22 m cable cutoff, MACCab, and 1×10, 1×20 and 1×30 mm diameter induced bend losses in dB per turn at 1550 nm. The optical fiber embodiments of Tables 4, 5 and 6 (fiber examples 8-27) have core alpha values between 5 and 15, core radii between about 4 and about 5 microns, and 0.3%<Δ1MAX<0.4%. Most of these fiber embodiments have a bend loss of less than 2 dB/turn (at 1550 nm) when bent around the 10 mm diameter mandrel, less than 0.5 dB/turn (at 1550 nm) when bent around the 20 mm mandrel, and less than 0.01 dB/turn when bent around 30 mm mandrel. The optical fiber embodiments corresponding to Tables 4, 5 and 6 have mode field diameters (MFD) between about 8.5 microns and about 9.1 microns at 1310 nm, and between about 9.6 microns and about 10.3 microns at 1310 nm; Cable Cutoff between 1190 nm and 1250 nm, and MACCab values between 7.1 and 7.6 (MACCab=MFD in microns at 1310 nm/Cable Cutoff in microns).
The relative refractive index profiles of a comparative example fiber (rectangular trench) and exemplary fiber embodiments (exemplary fiber embodiments 1, 2 and 3) of Table 1A are illustrated in
The relative refractive index profiles of another comparative example fiber 2 (rectangular trench) and three fiber embodiments (Fiber Examples 4, 5 and 6) of Table 1 are illustrated in
The relative refractive index profiles for another modeled fiber corresponding to this profile are illustrated in
Preferably, exemplary optical fiber embodiments 10 exhibit a bend loss at 1550 nm, when wound upon on a 20 mm diameter mandrel, of less than 0.5 dB/turn, and in some cases less than 0.25 dB/turn. These fibers also exhibit a bend loss at 1550 nm, when wound upon on a 10 mm diameter mandrel, of less than 2 dB/turn, more preferably less than 1 dB/turn, more preferably less than 0.5 dB/turn, and some fibers most preferably less than 0.2 dB/turn. These fibers also exhibit a bend loss at 1550 nm, when wound upon on a 30 mm diameter mandrel, of less than 0.01 dB/turn, and some fibers more preferably less than 0.003 dB/turn. Some of these examples employ chlorine in the outer cladding region in an amount greater than 2000 ppm, and in some cases greater than 3 000 or even greater than 4000 ppm by weight. In some embodiments the outer cladding region comprises chlorine in an amount greater than 2000 and less than 12000 ppm by weight.
Some exemplary optical fiber embodiments 10 exhibit a bend loss at 1550 nm, when wound upon on a 15 mm diameter mandrel, of less than 0.5 dB/turn, and in some cases less than 0.25 dB/turn. At least some of these e fibers also exhibit a bend loss at 1550 nm, when wound upon on a 10 mm diameter mandrel, of less than 1 dB/turn, more preferably less than 0.5 dB/turn, and some fibers most preferably less than 0.2 dB/turn. The fibers exhibit a bend loss at 1550 nm, when wound upon on a 15 mm diameter mandrel, of less than 0.25 dB/turn, and some fibers more preferably less than 0.15 dB/turn. The fibers exhibit a bend loss at 1550 nm, when wound upon on a 20 mm diameter mandrel, of less than 0.1 dB/turn, and some fibers more preferably less than 0.03 dB/turn.
Attenuation (spectral) at 1550 nm is preferably less than 0.21 dB/km, more preferably less than 0.20 dB/km, even more preferably less than 0.197 dB/km. In some preferred embodiments the attenuation (spectral) at 1550 nm is less than or equal to 0.191 dB/km, even more preferably less than or equal to 0.189 dB/km, even more preferably less than or equal to 0.182 dB/km.
Thus, the embodiments of the optical fibers 10 described herein provide outstanding bending performance, and additionally provide cutoff wavelengths suitable for single mode operation at wavelengths greater than about 1260 nm.
In some embodiments, the core may comprise a relative refractive index profile having a so-called centerline dip which may occur as a result of one or more optical fiber manufacturing techniques. However, the centerline dip in any of the relative refractive index profiles disclosed herein is optional.
The optical fiber disclosed herein comprises a core and a cladding layer (or cladding or outermost annular cladding region) surrounding and directly adjacent the core. Preferably, the core is comprised of silica doped with germanium, i.e. germania doped silica. Dopants other than germanium, singly or in combination, may be employed within the core, and particularly at or near the centerline, of the optical fiber disclosed herein to obtain the desired refractive index and density. In preferred embodiments, the core of the optical fiber disclosed herein has a non-negative relative refractive index profile, more preferably a positive relative refractive index profile, wherein the core is surrounded by and directly adjacent to a cladding layer.
Preferably, the optical fiber disclosed herein has a silica-based core and cladding. In preferred embodiments, the cladding has an outer diameter, 2 times r4, of about 125 micron.
The fibers disclosed herein exhibit low PMD values particularly when fabricated with OVD processes. Spinning of the optical fiber may also lower PMD values for the fiber disclosed herein.
It is to be understood that the foregoing description is exemplary only and is intended to provide an overview for the understanding of the nature and character of the fibers which are defined by the claims. The accompanying drawings are included to provide a further understanding of the preferred embodiments and are incorporated and constitute part of this specification. The drawings illustrate various features and embodiments which, together with their description, serve to explain the principals and operation. It will become apparent to those skilled in the art that various modifications to the preferred embodiments as described herein can be made without departing from the spirit or scope of the appended claims.
This application claims the benefit of priority under 35 U.S.C. §119 of U.S. Provisional Application Ser. No. 61/564,902 filed on Nov. 30, 2011 the content of which is relied upon and incorporated herein by reference in its entirety.
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